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cf30947ffa667cdecbbacea74a60e4b101897d88 | 449d555969bfd7befe906877abab098c6e63a0e8 | /3472/CH30/EX30.11/Example30_11.sce | bb7909999bcedcfe61edff52deb3581269797d48 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 1,934 | sce | Example30_11.sce | // A Texbook on POWER SYSTEM ENGINEERING
// A.Chakrabarti, M.L.Soni, P.V.Gupta, U.S.Bhatnagar
// DHANPAT RAI & Co.
// SECOND EDITION
// PART III : SWITCHGEAR AND PROTECTION
// CHAPTER 4: UNSYMMETRICAL FAULTS IN POWER SYSTEMS
// EXAMPLE : 4.11 :
// Page number 520-521
clear ; clc ; close ; // Clear the work space and console
// Given data
n = 6.0 // Number of alternator
kV_A = 6.6 // Alternator rating(kV)
X_1 = 0.9 // Positive sequence reactance(ohm)
X_2 = 0.72 // Negative sequence reactance(ohm)
X_0 = 0.3 // Zero sequence reactance(ohm)
Z_n = 0.2 // Resistance of grounding resistor(ohm)
// Calculations
E_a = kV_A*1000/3**0.5 // Phase voltage(V)
// Case(a)
Z_1_a = %i*X_1/n // Positive sequence impedance when alternators are in parallel(ohm)
Z_2_a = %i*X_2/n // Negative sequence impedance when alternators are in parallel(ohm)
Z_0_a = %i*X_0/n // Zero sequence impedance when alternators are in parallel(ohm)
I_a_a = 3*E_a/(Z_1_a+Z_2_a+Z_0_a) // Fault current assuming 'a' phase to be fault(A)
// Case(b)
Z_0_b = 3*Z_n+%i*X_0 // Zero sequence impedance(ohm)
I_a_b = 3*E_a/(Z_1_a+Z_2_a+Z_0_b) // Fault current(A)
// Case(c)
Z_0_c = %i*X_0 // Zero sequence impedance(ohm)
I_a_c = 3*E_a/(Z_1_a+Z_2_a+Z_0_c) // Fault current(A)
// Results
disp("PART III - EXAMPLE : 4.11 : SOLUTION :-")
printf("\nCase(a): Fault current if all alternator neutrals are solidly grounded, I_a = %.f A", imag(I_a_a))
printf("\nCase(b): Fault current if one alternator neutral is grounded & others isolated, I_a = %.1f∠%.1f° A", abs(I_a_b),phasemag(I_a_b))
printf("\nCase(c): Fault current if one alternator neutral is solidly grounded & others isolated, I_a = %.2fj A\n", imag(I_a_c))
printf("\nNOTE: ERROR: Calculation mistakes in the textbook solution")
|
dd79dfb7a4bcf58a9ad118ed13fdd70d015772aa | 449d555969bfd7befe906877abab098c6e63a0e8 | /476/CH4/EX4.17/Example_4_17.sce | ac5ea04137b1c1f26454cc115e45a62b78db6ea5 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 568 | sce | Example_4_17.sce | //A Textbook of Chemical Engineering Thermodynamics
//Chapter 4
//Second Law of Thermodynamics
//Example 17
clear;
clc;
//Given:
To = 275; //temperature of quenching oil (K)
//To calculate loss in capacity of doing work
//Referrring example 4.9 (Page no. 95)
S_steel = -26.25; //change in entropy os casting (kJ/K)
S_oil = 43.90; //change in entropy of oil (kJ/K)
S_tot = S_steel+S_oil; //total entropy change
//Let W be loss in capacity for doing work
W = To*S_tot; //(kJ)
mprintf('The loss in capacity for doing work is %f kJ',W);
//end |
c0a15fe90367f8940a5f78a4d266e7574f26740c | 449d555969bfd7befe906877abab098c6e63a0e8 | /249/CH18/EX18.1/18_01.sce | 6e102ae11eb6ecf40c622b3b7bae2983e2d0f295 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 1,580 | sce | 18_01.sce | clear
clc
dp=2.4*(10^-3);L=dp/6;
//Effective mass conductivity(m3/hr.mcat)
De=5*10^-5;
//Effective thermal conductivity(KJ/hr.mcat.K)
Keff=1.6;
//For the gas film surrounding the pellet
h=160;//heat transfer coefficient(KJ/hr.m2cat.K)
kg=300;//mass transfer coefficient(m3/hr.m2cat)
//For the reaction
Hr=-160;//KJ/molA
CAg=20;//mol/m3
rA_obs=10^5;//mol/hr.m3cat
kobs=rA_obs/CAg;
Vp=3.14*(dp^3)/6;
S=3.14*(dp^2);
//Observed rate/rate if film resistance controls
ratio=kobs*Vp/(kg*S);
printf("\n Part a")
if ratio<0.01
printf("\n Resistance to mass transport to film should not influence rate of reaction")
else
printf("\n Resistance to mass transport to film should influence rate of reaction")
end
printf("\n Part b")
Mw=rA_obs*(L^2)/(De*CAg);
printf("\n Mw= %f",Mw)
if Mw>4
printf("\n Pore diffusion is influencing and hence strong pore diffusion")
else
printf("\n Pore diffusion is not influencing and hence weak pore diffuusion")
end
//Temp variation within pellet
dt_max_pellet=De*(CAg-0)*(-Hr)/Keff;
//Temp variation Across the gas film
dt_max_film=L*rA_obs*(-Hr)/h;
printf("\n Part c")
printf("\n dTmax,pellet is %f",dt_max_pellet)
printf(" degree C \n dTmax,film is %f",dt_max_film)
printf(" degree C")
if dt_max_pellet<1
printf("\n Pellet is close to uniform in temperature")
else
printf("\n There is a variation in temp within pellet")
end
if dt_max_film<1
printf("\n Film is close to uniform in temperature")
else
printf("\n There is a variation in temp within Film")
end |
30128524a7a68c52eb9957d4bf88767644fbe9cd | 449d555969bfd7befe906877abab098c6e63a0e8 | /3116/CH10/EX10.2/Ex10_2.sce | 6a6032e323edd7a792f7438ca5b66c77898ce135 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 375 | sce | Ex10_2.sce |
clc
// Given that
d1 = 15.2 // Initial diameter in mm
d2 = 12.2 // Final diameter in mm
printf("Example 10.2\n")
per_CW = (d1^2 - d2^2)*100/d1^2
printf("\n The tensile strength is read directly from the curve for copper(figure 10.9b) \n as 340 MPa From figure 10.19c, the Ductility at %0.1f CW is about 7%% EL.",per_CW)
// Some values are deduced from figures
|
8daa3369c880cd73178e5f83bd767d0371340b48 | 449d555969bfd7befe906877abab098c6e63a0e8 | /1322/CH13/EX13.6/93ex1.sce | 4c488c8a4d45699f214eca108dd1bad00f9e5163 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 116 | sce | 93ex1.sce |
clear;
clc;
close;
x=poly(0,'x');
p1=(x+2);
p2=(x^2-x+1);
p3=p1*p2;//on collecting like terms
disp(p3,"product=")
|
b5c9f7e8e824241bba9374486eb5e218db74ad09 | 717ddeb7e700373742c617a95e25a2376565112c | /1442/CH14/EX14.2/14_2.sce | 7f468369b1c642e2a27c8731439cb8f960dad181 | [] | no_license | appucrossroads/Scilab-TBC-Uploads | b7ce9a8665d6253926fa8cc0989cda3c0db8e63d | 1d1c6f68fe7afb15ea12fd38492ec171491f8ce7 | refs/heads/master | 2021-01-22T04:15:15.512674 | 2017-09-19T11:51:56 | 2017-09-19T11:51:56 | 92,444,732 | 0 | 0 | null | 2017-05-25T21:09:20 | 2017-05-25T21:09:19 | null | UTF-8 | Scilab | false | false | 252 | sce | 14_2.sce | clc
//initialisation of variables
a=552.6 //kPa m^6/kmol^2
b= 0.03402 //m^3/kmol
p= 100 //kPa
R= 8.314 //J/mol K
//CALCULATIONS
x= poly('0',x)
vector= roots('p*x^3-a*x+2*a*b')
T= 2*a*(x-b)^2/(R*x^3)
//RESULTS
printf (' isotherm= %.1f K',T)
|
74a5aa0e9c41fae2dc42f0ce9637c8c643d72c27 | a5f0fbcba032f945a9ee629716f6487647cafd5f | /Development/Preprocessing/PCA/PCA.sci | 15e269f21f029eaa289d70b0fb5e37310bd1b343 | [] | no_license | SoumitraAgarwal/Scilab-gsoc | 692c00e3fb7a5faf65082e6c23765620f4ecdf35 | 678e8f80c8a03ef0b9f4c1173bdda7f3e16d716f | refs/heads/master | 2021-04-15T17:55:48.334164 | 2018-08-07T13:43:26 | 2018-08-07T13:43:26 | 126,500,126 | 1 | 1 | null | null | null | null | UTF-8 | Scilab | false | false | 456 | sci | PCA.sci | // Macro for PCA of dataset -- Scilab
function pcaDataset = PCA(x)
width = length(x(1, :));
n = length(x(:, 1));
means = [];
for i = 1:width
means = [means, mean(x(:, i))];
end
for i = 1:n
x(i, :) = x(i, :) - means;
end
covarianceMat = cov(x);
[eigenVector, eigenVals] = spec(covarianceMat);
eigenVector = flipdim(eigenVector, 2);
eigenVals = diag(eigenVals)
pcaDataset = eigenVector'*x';
pcaDataset = pcaDataset';
endfunction |
2bf8e44738a262ee84448313d8bd9e99ab4388aa | 1489f5f3f467ff75c3223c5c1defb60ccb55df3d | /tests/test_cache_3_d.tst | 9f99e41d0698ac600a994466a100d9a07be26c40 | [
"MIT"
] | permissive | ciyam/ciyam | 8e078673340b43f04e7b0d6ac81740b6cf3d78d0 | 935df95387fb140487d2e0053fabf612b0d3f9e2 | refs/heads/master | 2023-08-31T11:03:25.835641 | 2023-08-31T04:31:22 | 2023-08-31T04:31:22 | 3,124,021 | 18 | 16 | null | 2017-01-28T16:22:57 | 2012-01-07T10:55:14 | C++ | UTF-8 | Scilab | false | false | 535 | tst | test_cache_3_d.tst | total_physical_store_count = 0
total_physical_fetch_count = 65536
<cache info>
items cached: 1000/1000
regions in use: 1/1
items per region: 65536
counter: 32768
temp_read_num: 65535
temp_write_num: -1
item_req_count = 65536
item_hit_count = 0
item hit ratio = 0%
<cache region: 0-65535>
item_cost: 1000
flush_cost: 0
counter_total: 32518000
most_recently_used: 65535
least_recently_used: 64536
most_recently_changed: -1
least_recently_changed: -1
most_recently_unchanged: 65535
least_recently_unchanged: 64536
|
5bcd6bcd1b66a0ae81b23d694887e927a54efe74 | 449d555969bfd7befe906877abab098c6e63a0e8 | /767/CH6/EX6.10.2/Ch06Exa6_10_2.sci | 005e8f393a1b3743f71c4632051691cdde4a0af9 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 735 | sci | Ch06Exa6_10_2.sci | // Scilab code Exa6.10.2 : To calculate the radius of proton orbit in synchrotron of given energy Page 275(2011)
c= 3e+08; // Speed of light in vacuum, m/s
q = 1.602e-019; // Charge on proton, coulomb
amu = 931; // Energy equivalent of 1 amu, MeV
m = 938; // Rest mass of a proton, MeV
KE = 12e+03; // Kinetic energy of proton, MeV
B = 1.9; // Magnetic field, T
E = m + KE; // Total energy of proton, MeV
// As E = m*amu, solving for m, the mass of proton
m = E/amu*1.672e-027; // Proton mass in motion, kg
v = 0.9973*c; // Velocity of the proton, m/s
r = m*v/(B*q); // Radius of the proton, m
printf("\nRadius of the proton orbit : %4.2f m", r)
// Result
// Radius of the proton orbit: 22.84 m |
8dc1aa04d0cafafd12b8d520d2ba9b430d917120 | 676ffceabdfe022b6381807def2ea401302430ac | /utilities/FieldConvert/Tests/Tet_channel_npart_wss.tst | d79e1b19074c570252c576c475c61f0399d69cc3 | [
"MIT"
] | permissive | mathLab/ITHACA-SEM | 3adf7a49567040398d758f4ee258276fee80065e | 065a269e3f18f2fc9d9f4abd9d47abba14d0933b | refs/heads/master | 2022-07-06T23:42:51.869689 | 2022-06-21T13:27:18 | 2022-06-21T13:27:18 | 136,485,665 | 10 | 5 | MIT | 2019-05-15T08:31:40 | 2018-06-07T14:01:54 | Makefile | UTF-8 | Scilab | false | false | 770 | tst | Tet_channel_npart_wss.tst | <?xml version="1.0" encoding="utf-8"?>
<test>
<description> Process npart to tecplot file </description>
<executable>FieldConvert</executable>
<parameters> -f -e --nparts 2 -m wss:bnd=2 Tet_channel_m3_xml:xml Tet_channel_m3.fld wss.fld </parameters>
<files>
<file description="Session File Directory">Tet_channel_m3_xml</file>
<file description="Field File">Tet_channel_m3.fld</file>
</files>
<metrics>
<metric type="L2" id="1">
<value variable="x" tolerance="1e-6">0.5</value>
<value variable="y" tolerance="1e-6">0</value>
<value variable="z" tolerance="1e-6">0.288675</value>
<value variable="Shear_x" tolerance="1e-6">2.06477e-16</value>
</metric>
</metrics>
</test>
|
edb0d10b28503233f8ad872c46fedc85e74f016c | 449d555969bfd7befe906877abab098c6e63a0e8 | /1913/CH1/EX1.4/ex4.sce | 3e65e4a1f057bb439cfdd1324c8a94209e0092d8 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 369 | sce | ex4.sce | clc
clear
//Input data
v1=0.056;//Initial volume of gas in m^3
v2=0.007;//Final volume of gas in m^3
p1=100;//Initial perssure compressed Isothermally in kN/m^2
//Calculations
p2=(p1*v1)/v2;//Final pressure in kN/m^2
W=p1*v1*(log(v2/v1));//Work done in kJ
//Output
printf('(a)Final pressure p2= %3.2f kN/m^2 \n (b)The work done on gas W= %3.2f kJ',p2,W)
|
d356463d7e936b5ae9c4cbdd8bb5b83b72cd4897 | 449d555969bfd7befe906877abab098c6e63a0e8 | /2240/CH1/EX0.4/EXI_4.sce | 6a5d380960b91074a5b1cbe3779b542a6e02c8f1 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 598 | sce | EXI_4.sce | // Grob's Basic Electronics 11e
// Chapter No. I
// Example No. I_4
clc; clear;
// Express the following numbers in engineering notation: (a) 27,000 (b) 0.00047.
disp ('To express the number 27,000 in engineering notation, it must be written as a number between 1 and 1000 times a power of 10 which is a multiple of 3.')
disp ('Therefore 27000 = 27*10^3 in engineering')
disp ('To express the number 0.00047 in engineering notation, it must be written as a number between 1 and 1000 times a power of 10 which is a multiple of 3.')
disp ('Therefore 0.00047 = 470*10^-6 in engineering')
|
270eb4311c3c6f07323b11538d75972c69808b2f | 449d555969bfd7befe906877abab098c6e63a0e8 | /3769/CH11/EX11.6/Ex11_6.sce | e1437959fcb7e7fb34ad38f637af50a2c2356d39 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 187 | sce | Ex11_6.sce | clear
//Given
M=8.0*10**22 //Am**2
R=64*10**5 //m
//Calculation
//
I=(3*M)/(4.0*%pi*R**3)
//Result
printf("\n earths magnetisation is %0.1f A/m",I)
|
d30b56a7cc21439e8afd581e072aad4be1d7601f | 449d555969bfd7befe906877abab098c6e63a0e8 | /615/CH7/EX7.8/7_8.sce | b351af809e361ce7bdaba781ca16fed384f2c6bb | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 386 | sce | 7_8.sce | //water chemistry//
//example 7.8//
N=150;//amount of NaCl in solution in g/l//
V=8;//volume of NaCl solution//
M=N*V;
printf("The amount of NaCl in 8 lit of solution is %fgms",M);
V=10000;//volume of hard water//
W=58.5;//molecular weight of NaCl//
K=(M*100/(W*2))/V;
printf("\nfor 1 litre hardness is %fg/l",K);
J=K*1000;
printf("\nHardness of water is %fmg/l or ppm",J);
|
26e2d0b6640bf0d6779b69dca4ee0676c879e226 | 68ca3dfa429602a00a0e728649484916bdff7d81 | /scilab/insert_waveform_in_scene.sci | 75ef021ea1ce112b93cb728e201fbc619f4fed29 | [] | no_license | bambang/toodles | f6e4c01a3326cd4dfb9674f11b727d8695daf369 | 2a65c5dec5d23b799d8246650716d4f683d4ae18 | refs/heads/master | 2020-12-28T20:30:53.721415 | 2012-03-12T16:00:12 | 2012-03-12T16:00:12 | null | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 288 | sci | insert_waveform_in_scene.sci | function inserted = insert_waveform_in_scene(waveform, scene)
[nrows, ncols] = size(scene);
wavesize = size(waveform, '*');
inserted = zeros(nrows, ncols);
for i = [1:wavesize]
inserted(nrows/2-wavesize/2+i, ncols/2) = waveform(1, i);
end
endfunction |
c50eea6d50886e71f68a8fcb8f90ddc21ab18299 | 449d555969bfd7befe906877abab098c6e63a0e8 | /1580/CH4/EX4.7/Ch04Ex7.sce | fd456b1eb9e9716bdaa1348e0b734e1b255b26b3 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 359 | sce | Ch04Ex7.sce | // Scilab Code Ex4.7 Page-4.16 (2004)
clc;clear;
a = 0.38; // Lattice constant of copper, nm
h =1, k = 1, l = 0; // Miller Indices (hkl)= (110)
d = a/sqrt(h^2 + k^2 + l^2); // Interplanar spacing for (110) plane, unit
printf("\nInterplanar spacing for (110) plane = %4.2f nm", d);
// Result
// Interplanar spacing for (110) plane = 0.27 nm
|
283d234637049a23ffd36e3669aa9abeaa42d62d | 244971ae8af51184d278cdc2be1c80775413adae | /SSSoDetector.sci | 519cb8cd7b7bbf33a512148eee1595da4b9d774d | [] | no_license | MSCA-SIMFREE/748767 | 5879f1f139b608c7cd2f1bd62325b281c9c1e7d1 | 4726206e514f1e47e939e73b9339c056057866db | refs/heads/master | 2020-12-27T15:21:13.646362 | 2020-02-03T11:40:00 | 2020-02-03T11:40:00 | 237,951,088 | 1 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 1,627 | sci | SSSoDetector.sci | // The code was developed under Horizon2020 Framework Programme
// Project: 748767 — SIMFREE
function Iout=SSSoDetector(In,Ideal?)
// Photodetector
//
// Calling Sequence
// Iout=SSSoDetector(In,Ideal?)
//
// Parameters
// In : Optical Input
// Ideal? : if False (default) then ideal photodetector
// Iout : Electrical Output
//
// Description
// Converts Optical Input power to an Electrical Output waveform by taking the modulus-squared of the Optical Input field of both polarisations.
// An Optical Input of 1 mW produces an Electrical Output of 1.
// The photodetector does not add any electrical noise. Receiver noise, if desired, can be added by setting Ideal? = True.
// The photodetector has a flat bandwidth. An alternative frequency response can be obtained by simply following the photodetector with the appropriate electrical filter.
global MNT MSR MLA;
[lhs,rhs]=argn(0);
select rhs
case 0 then
error("Expect at least one argument");
case 1 then
Ideal?=%T;
end
Xin=fft(In(:,1),1);
Yin=fft(In(:,2),1);
x=real(Xin.*conj(Xin));
y=real(Yin.*conj(Yin));
Iout=(x+y)*MNT^2;
if ~Ideal? then
q=1.6E-19; c=299792458; h=6.62607e-34; kB=1.3806488E-23;
T=273; RT=20;
df=1e9*MSR*MNT/MNS;
R=q/(h*c/(1E-9*MLA));
Iout=R*Iout;
sh=sqrt(q*df);
ShotNoise=sqrt(1E-3*Iout).*grand(MNT,1,'nor',0,sh);
sT=sqrt(2*kB*T*df)/RT;
ThermalNoise=grand(MNT,1,'nor',0,sT);
Iout=Iout+1E3*(ShotNoise+ThermalNoise);
end
endfunction
|
08da9c6e927362c9a33a4cb0be96fb1defacc7f6 | 8217f7986187902617ad1bf89cb789618a90dd0a | /browsable_source/2.4/Unix-Windows/scilab-2.4/macros/fraclab/pseudoAW.sci | c77a3605e28af57db7bdc726f5d203ffb7cdea60 | [
"LicenseRef-scancode-public-domain",
"LicenseRef-scancode-warranty-disclaimer"
] | permissive | clg55/Scilab-Workbench | 4ebc01d2daea5026ad07fbfc53e16d4b29179502 | 9f8fd29c7f2a98100fa9aed8b58f6768d24a1875 | refs/heads/master | 2023-05-31T04:06:22.931111 | 2022-09-13T14:41:51 | 2022-09-13T14:41:51 | 258,270,193 | 0 | 1 | null | null | null | null | UTF-8 | Scilab | false | false | 4,743 | sci | pseudoAW.sci | function [tfr,a,f,wt] = pseudoAW(x,K,wave,tsmooth,fmin,fmax,N);
// This Software is ( Copyright INRIA . 1998 1 )
//
// INRIA holds all the ownership rights on the Software.
// The scientific community is asked to use the SOFTWARE
// in order to test and evaluate it.
//
// INRIA freely grants the right to use modify the Software,
// integrate it in another Software.
// Any use or reproduction of this Software to obtain profit or
// for commercial ends being subject to obtaining the prior express
// authorization of INRIA.
//
// INRIA authorizes any reproduction of this Software.
//
// - in limits defined in clauses 9 and 10 of the Berne
// agreement for the protection of literary and artistic works
// respectively specify in their paragraphs 2 and 3 authorizing
// only the reproduction and quoting of works on the condition
// that :
//
// - "this reproduction does not adversely affect the normal
// exploitation of the work or cause any unjustified prejudice
// to the legitimate interests of the author".
//
// - that the quotations given by way of illustration and/or
// tuition conform to the proper uses and that it mentions
// the source and name of the author if this name features
// in the source",
//
// - under the condition that this file is included with
// any reproduction.
//
// Any commercial use made without obtaining the prior express
// agreement of INRIA would therefore constitute a fraudulent
// imitation.
//
// The Software beeing currently developed, INRIA is assuming no
// liability, and should not be responsible, in any manner or any
// case, for any direct or indirect dammages sustained by the user.
//
// Any user of the software shall notify at INRIA any comments
// concerning the use of the Sofware (e-mail : FracLab@inria.fr)
//
// This file is part of FracLab, a Fractal Analysis Software
// TFRSPAW [tfr,t,f,wt] = TFRSPAW(X,K,WAVE,TSMOOTH,FMIN,FMAX,N) :
// Smoothed Pseudo Afine Wigner distributions.
// CHECK INPUT FORMATS
[nargout,nargin] = argn(0) ;
select nargin
case 1
error('at least two input parameters required') ;
case 2
wave = 0 ;
tsmooth = 0 ;
nargfixed = 4 ;
case 3
tsmooth = 0 ;
nargfixed = 4 ;
case {4,5,6}
nargfixed = 4 ;
case 7
nargfixed = 7 ;
end
[xr,xc] = size(x) ;
if xr ~= 1 & xc ~= 1
error('1-D signals only')
elseif xc == 1
x = conj(x)' ;
end
nt = size(x,2) ;
if nargfixed == 4
XTF = fft(mtlb_fftshift(x),-1) ;
sp = (abs(XTF(1:nt/2))).^2 ;
f = linspace(0,0.5,nt/2+1) ; f = f(1:nt/2) ;
plot2d(f,sp) ;
xtitle('Analyzed Signal Spectrum','frequency') ;
fmin = input('lower frequency bound = ') ;
fmax = input('upper frequency bound = ') ;
N = input('Frequency samples = ') ;
end
if length(wave) > 1,
error('Morlet or Mexican hat wavelet only') ;
elseif wave == 0 ,
tsupport = (length(mexhat(fmax))-1)/2 ;
elseif abs(wave) > 0 ,
tsupport = abs(wave) ;
end
Qte = fmax/fmin;
umax = log(Qte) ;
Teq = tsupport/(fmax*umax);
if Teq<2*tsupport
M0 = round((2*tsupport^2)/Teq-tsupport) ;
MU = tsupport+M0 ;
elseif Teq>=2*tsupport
MU = tsupport ;
end
k = 1:N ; q = (fmax/fmin)^(1/(N-1));
a = (exp((k-1).*log(q))) ; // a is an increasing scale vector.
geo_f(k) = fmin*a ; // geo_f is a geometrical increasing
// frequency vector.
// Wavelet computation
[wt] = contwt(x,geo_f(1),geo_f(N),N,wave) ;
wtnonorm = zeros(wt) ;
for ptr = 1:N,
wtnonorm(ptr,:) = wt(ptr,:).*sqrt(a(ptr)) ;
end ;
// Pseudo Affine Wigner distribution computation
tfr=zeros(wt);
umin = -umax ;
u=linspace(umin,umax,2*MU+1) ; u(MU+1) = 0;
k = 1:2*N;
beta(k) = -1/(2*log(q))+(k-1)./(2*N*log(q));
for m = 1:2*MU+1
l1(m,1:2*N) = exp(-(2*%i*%pi*beta).*log(lambdak(u(m),K)));
end
// NEW DETERMINATION OF G(T)
a_t = 3 ; // (attenuation of 10^(-a_t) at t = tmax)
sigma_t = tsmooth*fmax/sqrt(2*a_t*log(10)) ;
a_u = 2 * %pi^2 * sigma_t^2 * umax^2 / log(10) ;
if sigma_t
sigma_u = 1/(2 * %pi * sigma_t) ;
else
sigma_u = %inf ;
end
G = gauss(2*MU+1,a_u) ; G = G(1:2*MU) ;
if sigma_u < umax/MU
fenh = findobj('Tag','Fig_gui_fl_pseudoaw')
if isempty(fenh)
disp('maximum time-smoothing corresponding to the scalogram reached ') ;
end
end
G = G(ones(1,N),:)' ;
for ti = 1:nt
S = zeros(1,2*N) ;
S(N:-1:1) = conj(wtnonorm(:,ti)') ;
S(N+1:2*N) = zeros(1,N) ;
Mellin = mtlb_fftshift(fft(S,1)) ;
waf = zeros(2*MU,N) ;
MX1 = l1.*Mellin(ones(1,2*MU+1),:) ;
X1 = fft1d(conj(MX1'),-1) ; X1 = conj(X1(1:N,:)') ;
waf = real(X1(1:2*MU,:).*conj(X1(2*MU+1:-1:2,:)).*G) ;
tfr(N:-1:1,ti) = conj(sum(waf,'c').*geo_f)';
end;
f = sort(geo_f(:)) ;
|
c6b770831706d74a3168a43ad80b3fffea5859a7 | 449d555969bfd7befe906877abab098c6e63a0e8 | /1445/CH1/EX1.54/Ex1_54.sce | 78a174178a367aed1372100afbd4bdd4b58d1575 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 970 | sce | Ex1_54.sce | //CHAPTER 1- D.C. CIRCUIT ANALYSIS AND NETWORK THEOREMS
//Example 54
clc;
disp("CHAPTER 1");
disp("EXAMPLE 54");
//VARIABLE INITIALIZATION
v=5; //voltage source in Volts
r1=1; //LHS resistance in Ohms
r2=5; //in Ohms
r3=1; //in Ohms
r4=1; //RHS resistance in Ohms
I=10; //current source in Amperes
//SOLUTION
req1=r1+r3+r4; //on deactivating the current source, current I1 flows in the circuit
I1=v/req1;
vab1=v-(I1*r1); //(I1*r1) is voltage drop across 1Ω resistance
I2=I/req1;
vab2=vab1+(I2*r1); //(I2*r1) is voltage drop across 1Ω resistance
req=r1+((r3*r4)/(r3+r4)); //'req' is the same as 'Rth' mentioned in the book
I=vab2/(req+r2);
RTh=(6/5)+(3/4);
req2=10+2;
I3=9/12;
disp(sprintf("The value of the current is %f A",I3));
//END
|
4eb91a5b4ad913e79565c9517be9f69a80cca5d8 | 3592fbcb99d08024f46089ba28a6123aeb81ff3c | /main.sce | cb88a6cdc862e6b3dad8c2af1cb3538008459e4d | [] | no_license | clairedune/sciGaitanLib | a29ab61206b726c6f0ac36785ea556adc9ef03b9 | 7498b0d707a24c170fc390f7413359ad1bfefe9f | refs/heads/master | 2020-12-11T01:51:13.640472 | 2015-01-28T13:52:26 | 2015-01-28T13:52:26 | null | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 24 | sce | main.sce | clear
;exec('Load.sce'); |
4d289f5797ca68b77abbc0db83131026cb19e145 | aa78020331b2766d96648a66417d8a57911a6ad2 | /tp-camera-calibration/dimitri-charneux.sci | 857e81394b873bbc030f7afdbb67c65c220aaa97 | [] | no_license | DimitriCharneux/VISA | 1d3ec02f27ea9bfdb41ccce548e52d4ce375ae8e | 960361ea2d61ae9fd9db582419b96526cae695c7 | refs/heads/master | 2021-06-09T22:51:44.212184 | 2017-01-03T19:49:49 | 2017-01-03T19:49:49 | 68,818,771 | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 2,449 | sci | dimitri-charneux.sci | // -----------------------------------------------------------------------
/// \brief Calcule un terme de contrainte a partir d'une homographie.
///
/// \param H: matrice 3*3 définissant l'homographie.
/// \param i: premiere colonne.
/// \param j: deuxieme colonne.
/// \return vecteur definissant le terme de contrainte.
// -----------------------------------------------------------------------
function v = ZhangConstraintTerm(H, i, j)
v = rand(1, 6);
v=[H(1,i) * H(1,j);
H(1,i) * H(2,j) + H(2,i) * H(1,j);
H(2,i) * H(2,j);
H(3,i)*H(1,j) + H(1,i)*H(3,j) ;
H(3,i)*H(2,j) + H(2,i) * H(3,j) ;
H(3,i) * H(3,j)]';
endfunction
// -----------------------------------------------------------------------
/// \brief Calcule deux equations de contrainte a partir d'une homographie
///
/// \param H: matrice 3*3 définissant l'homographie.
/// \return matrice 2*6 definissant les deux contraintes.
// -----------------------------------------------------------------------
function v = ZhangConstraints(H)
v = [ZhangConstraintTerm(H, 1, 2); ...
ZhangConstraintTerm(H, 1, 1) - ZhangConstraintTerm(H, 2, 2)];
endfunction
// -----------------------------------------------------------------------
/// \brief Calcule la matrice des parametres intrinseques.
///
/// \param b: vecteur resultant de l'optimisation de Zhang.
/// \return matrice 3*3 des parametres intrinseques.
// -----------------------------------------------------------------------
function A = IntrinsicMatrix(b)
A = rand(3, 3);
v0 = (b(2) * b(4) - b(1) * b(5))/(b(1) * b(3) - b(2)^2);
lambda = b(6) - (b(4)^2 + v0*(b(2) * b(4) - b(1) * b(5))/b(1));
alpha = sqrt(lambda/b(1));
beta = sqrt(lambda * b(1)/(b(1)*b(3)-b(2)^2));
gamma = -b(2)*(alpha^2)*beta/lambda;
u0 = gamma * v0 / beta - b(4) * alpha^2/lambda;
A = [alpha,gamma,u0;0,beta,v0;0,0,1]
endfunction
// -----------------------------------------------------------------------
/// \brief Calcule la matrice des parametres extrinseques.
///
/// \param iA: inverse de la matrice intrinseque.
/// \param H: matrice 3*3 definissant l'homographie.
/// \return matrice 3*4 des parametres extrinseques.
// -----------------------------------------------------------------------
function E = ExtrinsicMatrix(iA, H)
E = rand(3, 4);
lambda = 1/norm(iA * H(:,1));
r1 = lambda*iA*H(:,1);
r2 = lambda*iA*H(:,2);
r3 = r1 .* r2;
t = lambda*iA*H(:,3);
E = [r1,r2,r3,t];
endfunction
|
42e1f7524609e9d96d52006929989d9a5d58957b | a62e0da056102916ac0fe63d8475e3c4114f86b1 | /set4/s_Digital_Communications_S._Sharma_1631.zip/Digital_Communications_S._Sharma_1631/CH9/EX9.3/Ex9_3.sce | 9a52e38ccbd7e44e609508a72849c949e7d89302 | [] | no_license | hohiroki/Scilab_TBC | cb11e171e47a6cf15dad6594726c14443b23d512 | 98e421ab71b2e8be0c70d67cca3ecb53eeef1df6 | refs/heads/master | 2021-01-18T02:07:29.200029 | 2016-04-29T07:01:39 | 2016-04-29T07:01:39 | null | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 348 | sce | Ex9_3.sce | errcatch(-1,"stop");mode(2);//Caption: Amount of Information
//Example 9.3
//page no 395
//Find Amount og Information
;
;
px1=1/2;
px2=1/2;
Ix1=log2(1/px1);//entropy
Ix2=log2(1/px2);
printf(" \n The amount of Information \n \n\t I(X1) = %.2d bit\n",Ix1);
printf(" \n The amount of Information \n \n\t I(X2) = %.2d bit",Ix2);
exit();
|
f61f7ff0e4fd068946464fc0b350d81338b617b8 | 449d555969bfd7befe906877abab098c6e63a0e8 | /1535/CH2/EX2.1/Ch02Ex1.sci | f7df1fa41f1c7e5911192055f59d9696778e5f11 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 373 | sci | Ch02Ex1.sci | // Scilab Code Ex2.1 : Page-46 (2010)
function V = f(t)
V = 0.2*sin(120*%pi*t);
endfunction
t = 0; // Time when peak value of current occurs
C = 10e-012; // Capacitance of the capacitor, farad
I = C*derivative(f,t);
printf("\nThe peak value of displacement current = %6.4e A", I);
// Result
// The peak value of displacement current = 7.5398e-010 A
|
ce877b069b76c38658ee73b7c68dcb5978f5e6e1 | 449d555969bfd7befe906877abab098c6e63a0e8 | /497/CH11/EX11.2/Chap11_Ex2.sce | a942045dca245112a6d5779823459bc616a271c4 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 1,821 | sce | Chap11_Ex2.sce | //Kunii D., Levenspiel O., 1991. Fluidization Engineering(II Edition). Butterworth-Heinemann, MA, pp 491
//Chapter-11, Example 2, Page 267
//Title: The Effect of m on Bubble-Emulsion Interchange
//==========================================================================================================
clear
clc
//INPUT
umf=0.12;//Velocity at minimum fluidization condition in cm/s
uo=40;//Superficial gas velocity in cm/s
ub=120;//Velocity of the bubble in cm/s
D=0.7;//Diffusion coefficient of gas in cm^2/s
abkbe1=1;//Bubble-emuslion interchange coefficient for non absorbing particles(m=0)
abkbe2=18;//Bubble-emuslion interchange coefficient for highly absorbing particles(m=infinity)
g=980;//Acceleration due to gravity in square cm/s^2
//CALCULATION
//For non absorbing particles m=0,etad=0
Kbc=(ub/uo)*(abkbe1);
dbguess=2;//Guess value of db
function[fn]=solver_func(db)//Function defined for solving the system
fn=abkbe1-(uo/ub)*(4.5*(umf/db)+5.85*(D^0.5*g^0.25)/(db^(5/4)));//Eqn.(10.27)
endfunction
[d]=fsolve(dbguess,solver_func,1E-6);//Using inbuilt function fsolve for solving Eqn.(10.27) for db
//For highly absorbing particles m=infinity, etad=1
M=abkbe2-(uo/ub)*Kbc;
//For intermediate condition
alpha=100;
m=10;
etad=1/(1+(alpha/m));//Fitted adsorption efficiency factor from Eqn.(23)
abkbe3=M*etad+(uo/ub)*Kbc;
//OUTPUT
mprintf('\nFor non absorbing particles:\n\tDiameter of bubble=%fcm\n\tBubble-cloud interchange coefficient=%fs^-1',d,Kbc);
mprintf('\nFor highly absorbing partilces:\n\tM=%f',M);
mprintf('\nFor intermediate condition:\n\tFitted adsorption efficiency factor:%f\n\tBubble-emuslion interchange coefficient:%fs^-1',etad,abkbe3);
//====================================END OF PROGRAM ====================================================== |
42f48141cc6c865461b8e3cc66fe8195c17c712b | 449d555969bfd7befe906877abab098c6e63a0e8 | /863/CH8/EX8.3/Ex8_3.txt | 6a61df93125f38190c51c49115c372c6cdff18e6 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 304 | txt | Ex8_3.txt | //Caption:Determine actual PRF and duty cycle
//Ex8.3
clc;
clear;
close;
C=0.082//Capacitance(in micro farad)
Ra=3.3//Resistance(in kilo ohm)
Rb=2.7//Resistance(in kilo ohm)
t1=0.693*C*(Ra+Rb)*1000
t2=0.693*C*Rb*1000
T=t1+t2
P=1000/T
d=t1*100/T
disp(P,d,'Duty cycle(in %) and PRF(in Khz)=') |
6f5d5c57a82eca10a7ba6d3aa42829fc9fae97f8 | 449d555969bfd7befe906877abab098c6e63a0e8 | /1664/CH2/EX2.1/Ex2_1.sce | 9f66f5479c9ce988ced0e00294fba6bf58c68c0c | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 550 | sce | Ex2_1.sce |
//Example No.2.1.
// Page No.59.
clc;clear;
p = 5*10^(-3);// output power -[W].
w = 632.8*10^(-9);//wavelength -[m].
h = 6.626*10^(-34);//Planck's constant.
c = (3*10^(8));//Velocity of light.
hv = ((h*c)/(w));// Energy of one photon
printf("\nThe energy of one photon in joules is %3.3e J", hv);
hv = hv/(1.6*10^(-19));
printf("\nThe energy of one photon in eV is %.2f eV",hv);
Np = (p/(3.14*10^(-19)));//Number of photons emitted
printf("\nThe number of photons emitted per second by He-Ne laser are %3.3e photons per second",Np);
|
ef1aa3880cd916f6227a549d4e8e89298d1d75e4 | 449d555969bfd7befe906877abab098c6e63a0e8 | /149/CH21/EX21.13.2/ques13_2.sce | 519d36c7dd39d2700453ed9cddbeca323d21805c | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 157 | sce | ques13_2.sce | //error no output
//ques11
disp('To find the inverse laplace transform of the function');
syms s t a
f=s/(s^4+4*a^4);
il=ilaplace(f,s,t);
disp(il);
|
363d53adbbe0d1b6fa50f12d8446466bb0e2295a | 449d555969bfd7befe906877abab098c6e63a0e8 | /3875/CH10/EX10.31/10_31.sce | a3e2a4cd5462133226edc442fb331b68610a1c73 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 293 | sce | 10_31.sce | clc;
clear;
delta_x=5*10^-14 //diameter of nucleus in m
h=6.63*10^-34 //plancks constant
m=1.675*10^-27 //mass in kg
//calculation
p_min=h/(4*%pi*delta_x) //minimum momentum in kg-m/s
E_min=((p_min)^2/(2*m))
mprintf("The minimum kinetic energy of the nucleon is = %0.2e J",E_min)
|
05a0097b92423a64e37f54e8a979ff861dcce08c | 449d555969bfd7befe906877abab098c6e63a0e8 | /3869/CH1/EX1.4/Ex1_4.sce | 3bf16c2198fd5143628a753beba80cbf26df8be9 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 357 | sce | Ex1_4.sce | clear
//
//
//
//Variable declaration
I1=10 //intensity(Wm**-2)
I2=25 //intensity(Wm**-2)
//Calculation
a1bya2=sqrt(I1/I2)
ImaxbyImin=(a1bya2+1)**2/(a1bya2-1)**2 //ratio of maximum intensity to minimum intensity
//Result
printf("\n ratio of maximum intensity to minimum intensity is %0.3f ",ImaxbyImin)
|
cdc8bb6a7a8e75ab74f7188d09824c7d1332ae81 | a62e0da056102916ac0fe63d8475e3c4114f86b1 | /set7/s_Electronics_Devices_And_Circuit_Theory_R._L._Boylestad_And_L._Nashelsky_69.zip/Electronics_Devices_And_Circuit_Theory_R._L._Boylestad_And_L._Nashelsky_69/CH5/EX5.28/5_28.sce | b605bd634ceed9d3cf6f5414df23078c656631bb | [] | no_license | hohiroki/Scilab_TBC | cb11e171e47a6cf15dad6594726c14443b23d512 | 98e421ab71b2e8be0c70d67cca3ecb53eeef1df6 | refs/heads/master | 2021-01-18T02:07:29.200029 | 2016-04-29T07:01:39 | 2016-04-29T07:01:39 | null | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 156 | sce | 5_28.sce | errcatch(-1,"stop");mode(2);; ;
Vcc = 6;
Vbe = 0.7;
Rx = 1.3*(10^(3));
Ix = (Vcc-Vbe)/Rx;
disp(Ix,"Current through each transistor :");
exit();
|
d6e053f15c6e10a04c854d073684f85358763576 | 449d555969bfd7befe906877abab098c6e63a0e8 | /608/CH24/EX24.07/24_07.sce | 862ea67d5cdde18d64ebedbeacd5e087fef546a2 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 636 | sce | 24_07.sce | //Problem 24.07: For the circuit shown in Figure 24.11, determine the value of impedance Z2.
//initializing the variables:
rv = 70; // in volts
thetav = 30; // in degrees
ri = 3.5; // in amperes
thetai = -20; // in degrees
//z1 consist of two resistance
R1 = 4.36; // in ohms
R2 = -2.1*%i; // in ohms
//calculation:
V = rv*cos(thetav*%pi/180) + %i*rv*sin(thetav*%pi/180)
I = ri*cos(thetai*%pi/180) + %i*ri*sin(thetai*%pi/180)
//impedance, Z
Z = V/I
//Total impedance Z = z1 + z2
Z1 = R1 + R2
Z2 = Z - Z1
x = real(Z2)
y = imag(Z2)
printf("\n\n Result \n\n")
printf("\n impedance Z2 is %.2f + (%.2f) ohm\n",x,y) |
c5544d16f4184d34b61cd3ab5319fa3b5c158b27 | 449d555969bfd7befe906877abab098c6e63a0e8 | /3831/CH16/EX16.2/Ex16_2.sce | 7f40f256fc2123d717dbbc191cc6b0919e09df7e | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 584 | sce | Ex16_2.sce | // Example 16_2
clc;funcprot(0);
// Given data
T=20+273.15;// K
V=25.0;// m/s
k=1.40;// The specific heat ratio
p=0.101;// MPa
g_c=1;// The gravitational constant
c_p=1.004;// kJ/kg.K
R=0.286;// kJ/kg.K
// Solution
p_os=p*(1+((V^2/1000)/(2*g_c*c_p*T)))^(k/(k-1));// The isentropic stagnation pressure in MPa
rho=(p*10^3)/(R*T);// kg/m^3
rho_os=rho*(1+((V^2/1000)/(2*g_c*c_p*T)))^(1/(k-1));// The isentropic stagnation density in kg/m^3
printf("\nThe isentropic stagnation pressure,p_os=%0.4f MPa \nThe isentropic stagnation density,rho_os=%1.4f kg/m^3",p_os,rho_os);
|
90ac19acc1e4e2cf2e79cb604ebe395f9f820651 | 449d555969bfd7befe906877abab098c6e63a0e8 | /2339/CH3/EX3.26.1/Ex3_26.sce | d391ecdb71facc580a195ce40062a3ca5fe530a5 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 572 | sce | Ex3_26.sce | clc
clear
//Inputs
//The Values in the program are as follows:
//Temperature in Celcius converted to Kelvin(by adding 273)
//Pressure in bar converted to kPa (by multiplying 100)
//Volume in m^3
//Value of R,Cp and Cv in kJ/kg K
V1=0.5;
P1=0.3;
V2=0.1;
P2=(P1*V1)/(V2);
printf('Final Pressure: %1.2f bar',P2);
printf('\n');
W=(P1*100*V1)*(log(V2/V1));
printf('Work Done: %1.2f kJ',W);
printf('\n');
printf('Change in Internal Energy: 0 kJ as it is Isothermal Process');
printf('\n');
printf('Change in Heat Energy: %1.2f kJ',W);
printf('\n');
|
199cc077d5d6827ba434ecdbb877be807daae290 | 449d555969bfd7befe906877abab098c6e63a0e8 | /1457/CH10/EX10.2/10_2.sce | 9fcc9494319e8c23a08eb15578b0db835369c338 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 460 | sce | 10_2.sce | clc
//Initialization of variables
nu=0.00015 //ft^2/s
L=35 //ft
U=88 //fps
g=32.2 //ft/s^2
b=10 //ft
w=8 //ft
rho=0.0725
//calculations
R=L*U/nu
Cf=0.455 /(log10(R))^2.58
B=2*b + w
Ff=Cf*rho/g *U^2 /2 *L*B
Rx=R/10^5
delta=L*0.377 /(b* Rx^(0.2))
T0=0.0587 *rho/g *U^2 /2 *(nu/(L*U))^(0.2)
//results
printf("Frictional drag = %.1f lb",Ff)
printf("\n Thickness of boundary layer = %.3f ft",delta)
printf("\n Shear stress = %.4f lb/ft^2",T0)
|
531329b818131e134529d3dc810fcdd41421f8ff | a72a0b668d399097c37190a9306c802a64d086d0 | /Sample/GroundwaterModel/sswFinish.sce | 7d333a7c6d7c3c13375fe589a1a93b36d7caa181 | [] | no_license | CNH-Hyper-Extractive/simple-script-wrapper | e3038039d0ae592293e99b6dd7fff819d9784956 | 0165df0b1d4cf21fd7de1d5bbff42c60fbe9aab4 | refs/heads/master | 2020-05-18T15:41:57.217472 | 2014-07-01T05:15:16 | 2014-07-01T05:15:16 | 16,794,069 | 2 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 107 | sce | sswFinish.sce |
//
// This function is called once at the end of the simulation.
//
function[] = sswFinish()
endfunction
|
282b04e07e1eeb03c4d977450f59b1e282a1724f | 449d555969bfd7befe906877abab098c6e63a0e8 | /1752/CH2/EX2.8/exa_2_8.sce | 150906d69ac205e503f67fc564a76d229a6cd135 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 895 | sce | exa_2_8.sce | //Exa 2.8
clc;
clear;
close;
//given data
k=0.175;// in W/mK
h_infinite=9.3;// in W/m^2K
T_infinite=30;// in degree C
T_s=70;// in degree C
d=10*10^-3;// in m
r=d/2;
L=1;// in m
rc=k/h_infinite;// in m
CriticalThickness = rc-r;// in meter
CriticalThickness=CriticalThickness*10^3;
disp(CriticalThickness,"Critical thickness in mm");
q1=2*%pi*r*L*h_infinite*(T_s-T_infinite);// in W/m
q2= (T_s-T_infinite)/(log(rc/r)/(2*%pi*k*L)+1/(2*%pi*rc*h_infinite));// in W/m
PerIncHeatDiss= (q2-q1)*100/q1;
disp(PerIncHeatDiss,"Percentage increase in heat dissipation rate in %")
//Also q1=I1^2*R with bare cable
// q2=I2^2*R with insulated cable
I2_by_I1 = sqrt(q2/q1);
// ( I2-I1 ) / I1 = (I2_by_I1 -1) / 1
// Percentage increase in current carrying capacity
PerIncCurrent = (I2_by_I1 -1) / 1 *100;
disp(floor(PerIncCurrent),"Increase in current carrying capacity in %")
|
c333deddde06262c1e456095c9720fdeced5756f | 449d555969bfd7befe906877abab098c6e63a0e8 | /1332/CH5/EX5.33/5_33.sce | 0c3c93eaf73427fd324a5f09decd8857e5868335 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 1,511 | sce | 5_33.sce | //Example 5.33
//Newton Raphson and Mullers Method
//Page no. 202
clc;clear;close;
deff('x=f(x)','x=x^4-8*x^3+18*x^2+0.12*x-24.24')
deff('x=f1(x)','x=4*x^3-24*x^2+36*x+0.12')
//newton raphson
x9=[1.5,2.5,2.7,3.1;4,5,14,10]
for h=1:4
x0=x9(1,h);e=0.00001
for i=1:x9(2,h)
x1=x0-f(x0)/f1(x0)
e1=abs(x0-x1)
x0=x1;
if abs(x0)<e then
break;
end
end
printf('\nThe solution of this equation by newton raphshon after %i Iterations is %.5f\n',i,x1)
end
//mullers method
zx=[1,2,2.7,3.1;2,3,3.7,4.1;3,4,4.7,5.1]
zi=[1;2;3];
s=["i","z0","z1","z2","f0","f1","f2","li","di","gi","li+1","hi","hi+1","zi+1","D+","D_"]
li(1)=(zi(3,1)-zi(2,1))/(zi(2,1)-zi(1,1))
hi(1)=zi(3,1)-zi(2,1);
for i=2:4
for j=1:3
fz(j,i-1)=f(zi(j,i-1))
end
di(i-1)=1+li(i-1)
gi(i-1)=fz(1,i-1)*li(i-1)^2-fz(2,i-1)*di(i-1)^2+fz(3,i-1)*(li(i-1)+di(i-1))
D1(i-1)=gi(i-1)+sqrt(gi(i-1)^2-4*fz(3,i-1)*di(i-1)*li(i-1)*(fz(1,i-1)*li(i-1)-fz(2,i-1)*di(i-1)+fz(3,i-1)))
D2(i-1)=gi(i-1)-sqrt(gi(i-1)^2-4*fz(3,i-1)*di(i-1)*li(i-1)*(fz(1,i-1)*li(i-1)-fz(2,i-1)*di(i-1)+fz(3,i-1)))
if abs(D1(i-1))>abs(D2(i-1)) then
li(i)=-2*fz(3,i-1)*di(i-1)/D1(i-1)
else
li(i)=-2*fz(3,i-1)*di(i-1)/D2(i-1)
end
hi(i)=li(i)*hi(i-1);
z(i-1)=zi(3,i-1)+hi(i)
for j=1:2
zi(j,i)=zi(j+1,i-1)
end
zi(3,i)=z(i-1)
end
printf('\n\nAt the end of the %ith iteration by mullers method, the root of the equation is %.10f',j+2,z(j)) |
a39a81f3f92db44efdc82e174acae72e92cc1dc8 | 36c5f94ce0d09d8d1cc8d0f9d79ecccaa78036bd | /bowtie.sce | 9eb21e331cabd05557add6204c7f6093a6ee7a21 | [] | no_license | Ahmad6543/Scenarios | cef76bf19d46e86249a6099c01928e4e33db5f20 | 6a4563d241e61a62020f76796762df5ae8817cc8 | refs/heads/master | 2023-03-18T23:30:49.653812 | 2020-09-23T06:26:05 | 2020-09-23T06:26:05 | null | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 27,404 | sce | bowtie.sce | Name=bowtie
PlayerCharacters=1
BotCharacters=2.bot
IsChallenge=true
Timelimit=90.0
PlayerProfile=1
AddedBots=2.bot
PlayerMaxLives=0
BotMaxLives=10
PlayerTeam=1
BotTeams=2
MapName=vertex.map
MapScale=4.0
BlockProjectilePredictors=true
BlockCheats=true
InvinciblePlayer=false
InvincibleBots=false
Timescale=1.0
BlockHealthbars=false
TimeRefilledByKill=0.0
ScoreToWin=1000.0
ScorePerDamage=1.0
ScorePerKill=0.0
ScorePerMidairDirect=0.0
ScorePerAnyDirect=0.0
ScorePerTime=1.0
ScoreLossPerDamageTaken=0.0
ScoreLossPerDeath=0.0
ScoreLossPerMidairDirected=0.0
ScoreLossPerAnyDirected=0.0
ScoreMultAccuracy=false
ScoreMultDamageEfficiency=false
ScoreMultKillEfficiency=false
GameTag=Tracking
WeaponHeroTag=Tracking Beam
DifficultyTag=2
AuthorsTag=faiNt`
BlockHitMarkers=false
BlockHitSounds=false
BlockMissSounds=true
BlockFCT=false
Description=HEADSHOTS ONLY // ADS
GameVersion=1.0.7.2
ScorePerDistance=0.0
[Aim Profile]
Name=At Feet
MinReactionTime=0.3
MaxReactionTime=0.4
MinSelfMovementCorrectionTime=0.001
MaxSelfMovementCorrectionTime=0.05
FlickFOV=30.0
FlickSpeed=1.5
FlickError=15.0
TrackSpeed=3.5
TrackError=3.5
MaxTurnAngleFromPadCenter=75.0
MinRecenterTime=0.3
MaxRecenterTime=0.5
OptimalAimFOV=30.0
OuterAimPenalty=1.0
MaxError=40.0
ShootFOV=15.0
VerticalAimOffset=-200.0
MaxTolerableSpread=5.0
MinTolerableSpread=1.0
TolerableSpreadDist=2000.0
MaxSpreadDistFactor=2.0
[Aim Profile]
Name=Low Skill At Feet
MinReactionTime=0.35
MaxReactionTime=0.45
MinSelfMovementCorrectionTime=0.001
MaxSelfMovementCorrectionTime=0.05
FlickFOV=30.0
FlickSpeed=1.5
FlickError=20.0
TrackSpeed=3.0
TrackError=5.0
MaxTurnAngleFromPadCenter=75.0
MinRecenterTime=0.3
MaxRecenterTime=0.5
OptimalAimFOV=30.0
OuterAimPenalty=1.0
MaxError=60.0
ShootFOV=25.0
VerticalAimOffset=-200.0
MaxTolerableSpread=5.0
MinTolerableSpread=1.0
TolerableSpreadDist=2000.0
MaxSpreadDistFactor=2.0
[Aim Profile]
Name=Low Skill
MinReactionTime=0.35
MaxReactionTime=0.45
MinSelfMovementCorrectionTime=0.001
MaxSelfMovementCorrectionTime=0.05
FlickFOV=30.0
FlickSpeed=1.5
FlickError=20.0
TrackSpeed=3.0
TrackError=5.0
MaxTurnAngleFromPadCenter=75.0
MinRecenterTime=0.3
MaxRecenterTime=0.5
OptimalAimFOV=30.0
OuterAimPenalty=1.0
MaxError=60.0
ShootFOV=25.0
VerticalAimOffset=0.0
MaxTolerableSpread=5.0
MinTolerableSpread=1.0
TolerableSpreadDist=2000.0
MaxSpreadDistFactor=2.0
[Aim Profile]
Name=Default
MinReactionTime=0.3
MaxReactionTime=0.4
MinSelfMovementCorrectionTime=0.001
MaxSelfMovementCorrectionTime=0.05
FlickFOV=30.0
FlickSpeed=1.5
FlickError=15.0
TrackSpeed=3.5
TrackError=3.5
MaxTurnAngleFromPadCenter=75.0
MinRecenterTime=0.3
MaxRecenterTime=0.5
OptimalAimFOV=30.0
OuterAimPenalty=1.0
MaxError=40.0
ShootFOV=15.0
VerticalAimOffset=0.0
MaxTolerableSpread=5.0
MinTolerableSpread=1.0
TolerableSpreadDist=2000.0
MaxSpreadDistFactor=2.0
[Bot Profile]
Name=2
DodgeProfileNames=Long Strafe FB
DodgeProfileWeights=1.0
DodgeProfileMaxChangeTime=2.0
DodgeProfileMinChangeTime=1.5
WeaponProfileWeights=1.0;1.0;2.0;1.0;0.0;0.0;0.0;0.0
AimingProfileNames=At Feet;Low Skill At Feet;Low Skill;Default;Default;Default;Default;Default
WeaponSwitchTime=3.0
UseWeapons=false
CharacterProfile=Watcher
SeeThroughWalls=false
NoDodging=false
NoAiming=false
[Character Profile]
Name=1
MaxHealth=300.0
WeaponProfileNames=gun;;;;;;;
MinRespawnDelay=1.0
MaxRespawnDelay=5.0
StepUpHeight=75.0
CrouchHeightModifier=0.5
CrouchAnimationSpeed=2.0
CameraOffset=X=0.000 Y=0.000 Z=80.000
HeadshotOnly=false
DamageKnockbackFactor=4.0
MovementType=Base
MaxSpeed=700.0
MaxCrouchSpeed=500.0
Acceleration=5000.0
AirAcceleration=16000.0
Friction=4.0
BrakingFrictionFactor=2.0
JumpVelocity=800.0
Gravity=3.0
AirControl=0.25
CanCrouch=true
CanPogoJump=false
CanCrouchInAir=true
CanJumpFromCrouch=false
EnemyBodyColor=X=0.771 Y=0.000 Z=0.000
EnemyHeadColor=X=1.000 Y=1.000 Z=1.000
TeamBodyColor=X=1.000 Y=0.888 Z=0.000
TeamHeadColor=X=1.000 Y=1.000 Z=1.000
BlockSelfDamage=false
InvinciblePlayer=false
InvincibleBots=false
BlockTeamDamage=false
AirJumpCount=0
AirJumpVelocity=0.0
MainBBType=Cylindrical
MainBBHeight=320.0
MainBBRadius=58.0
MainBBHasHead=false
MainBBHeadRadius=45.0
MainBBHeadOffset=0.0
MainBBHide=false
ProjBBType=Cylindrical
ProjBBHeight=320.0
ProjBBRadius=55.0
ProjBBHasHead=false
ProjBBHeadRadius=45.0
ProjBBHeadOffset=0.0
ProjBBHide=true
HasJetpack=false
JetpackActivationDelay=0.2
JetpackFullFuelTime=4.0
JetpackFuelIncPerSec=1.0
JetpackFuelRegensInAir=false
JetpackThrust=6000.0
JetpackMaxZVelocity=400.0
JetpackAirControlWithThrust=0.25
AbilityProfileNames=;;;
HideWeapon=true
AerialFriction=0.0
StrafeSpeedMult=1.0
BackSpeedMult=1.0
RespawnInvulnTime=0.0
BlockedSpawnRadius=0.0
BlockSpawnFOV=0.0
BlockSpawnDistance=0.0
RespawnAnimationDuration=0.5
AllowBufferedJumps=true
BounceOffWalls=false
LeanAngle=0.0
LeanDisplacement=0.0
AirJumpExtraControl=0.0
ForwardSpeedBias=1.0
HealthRegainedonkill=0.0
HealthRegenPerSec=0.0
HealthRegenDelay=0.0
JumpSpeedPenaltyDuration=0.0
JumpSpeedPenaltyPercent=0.0
ThirdPersonCamera=false
TPSArmLength=300.0
TPSOffset=X=0.000 Y=150.000 Z=150.000
BrakingDeceleration=2048.0
VerticalSpawnOffset=0.0
[Character Profile]
Name=Watcher
MaxHealth=100.0
WeaponProfileNames=;;;;;;;
MinRespawnDelay=0.1
MaxRespawnDelay=5.0
StepUpHeight=45.0
CrouchHeightModifier=0.69
CrouchAnimationSpeed=2.0
CameraOffset=X=0.000 Y=0.000 Z=20.000
HeadshotOnly=true
DamageKnockbackFactor=3.0
MovementType=Base
MaxSpeed=200.0
MaxCrouchSpeed=270.0
Acceleration=10000.0
AirAcceleration=16000.0
Friction=100.0
BrakingFrictionFactor=0.0
JumpVelocity=300.0
Gravity=1.0
AirControl=0.16
CanCrouch=true
CanPogoJump=false
CanCrouchInAir=true
CanJumpFromCrouch=false
EnemyBodyColor=X=0.000 Y=0.000 Z=0.000
EnemyHeadColor=X=1.000 Y=0.888 Z=0.000
TeamBodyColor=X=1.000 Y=0.888 Z=0.000
TeamHeadColor=X=1.000 Y=1.000 Z=1.000
BlockSelfDamage=false
InvinciblePlayer=false
InvincibleBots=false
BlockTeamDamage=false
AirJumpCount=0
AirJumpVelocity=0.0
MainBBType=Cylindrical
MainBBHeight=130.0
MainBBRadius=18.0
MainBBHasHead=true
MainBBHeadRadius=10.0
MainBBHeadOffset=40.0
MainBBHide=false
ProjBBType=Cylindrical
ProjBBHeight=160.0
ProjBBRadius=26.0
ProjBBHasHead=false
ProjBBHeadRadius=20.0
ProjBBHeadOffset=15.0
ProjBBHide=true
HasJetpack=false
JetpackActivationDelay=0.2
JetpackFullFuelTime=4.0
JetpackFuelIncPerSec=1.0
JetpackFuelRegensInAir=false
JetpackThrust=6000.0
JetpackMaxZVelocity=400.0
JetpackAirControlWithThrust=0.25
AbilityProfileNames=;;;
HideWeapon=true
AerialFriction=0.0
StrafeSpeedMult=1.0
BackSpeedMult=1.0
RespawnInvulnTime=0.0
BlockedSpawnRadius=0.0
BlockSpawnFOV=0.0
BlockSpawnDistance=0.0
RespawnAnimationDuration=0.1
AllowBufferedJumps=true
BounceOffWalls=false
LeanAngle=0.0
LeanDisplacement=0.0
AirJumpExtraControl=0.0
ForwardSpeedBias=1.0
HealthRegainedonkill=0.0
HealthRegenPerSec=0.0
HealthRegenDelay=0.0
JumpSpeedPenaltyDuration=0.0
JumpSpeedPenaltyPercent=0.0
ThirdPersonCamera=false
TPSArmLength=300.0
TPSOffset=X=0.000 Y=150.000 Z=150.000
BrakingDeceleration=2048.0
VerticalSpawnOffset=0.0
[Dodge Profile]
Name=Long Strafe FB
MaxTargetDistance=100000.0
MinTargetDistance=0.0
ToggleLeftRight=true
ToggleForwardBack=true
MinLRTimeChange=0.5
MaxLRTimeChange=2.0
MinFBTimeChange=1.0
MaxFBTimeChange=2.0
DamageReactionChangesDirection=false
DamageReactionChanceToIgnore=0.5
DamageReactionMinimumDelay=0.15
DamageReactionMaximumDelay=0.18
DamageReactionCooldown=1.0
DamageReactionThreshold=0.0
DamageReactionResetTimer=0.1
JumpFrequency=0.0
CrouchInAirFrequency=0.0
CrouchOnGroundFrequency=0.0
TargetStrafeOverride=Ignore
TargetStrafeMinDelay=0.125
TargetStrafeMaxDelay=0.25
MinProfileChangeTime=0.0
MaxProfileChangeTime=0.0
MinCrouchTime=0.3
MaxCrouchTime=0.6
MinJumpTime=0.3
MaxJumpTime=0.6
LeftStrafeTimeMult=1.0
RightStrafeTimeMult=1.0
StrafeSwapMinPause=0.0
StrafeSwapMaxPause=0.0
BlockedMovementPercent=0.8
BlockedMovementReactionMin=0.05
BlockedMovementReactionMax=0.1
[Weapon Profile]
Name=gun
Type=Hitscan
ShotsPerClick=1
DamagePerShot=1.0
KnockbackFactor=0.0
TimeBetweenShots=0.046
Pierces=false
Category=FullyAuto
BurstShotCount=1
TimeBetweenBursts=0.5
ChargeStartDamage=10.0
ChargeStartVelocity=X=500.000 Y=0.000 Z=0.000
ChargeTimeToAutoRelease=2.0
ChargeTimeToCap=1.0
ChargeMoveSpeedModifier=1.0
MuzzleVelocityMin=X=2000.000 Y=0.000 Z=0.000
MuzzleVelocityMax=X=2000.000 Y=0.000 Z=0.000
InheritOwnerVelocity=0.0
OriginOffset=X=0.000 Y=0.000 Z=0.000
MaxTravelTime=5.0
MaxHitscanRange=100000.0
GravityScale=1.0
HeadshotCapable=true
HeadshotMultiplier=1.0
MagazineMax=0
AmmoPerShot=1
ReloadTimeFromEmpty=0.5
ReloadTimeFromPartial=0.5
DamageFalloffStartDistance=100000.0
DamageFalloffStopDistance=100000.0
DamageAtMaxRange=7.0
DelayBeforeShot=0.0
HitscanVisualEffect=Tracer
ProjectileGraphic=Ball
VisualLifetime=0.05
WallParticleEffect=None
HitParticleEffect=None
BounceOffWorld=false
BounceFactor=0.0
BounceCount=0
HomingProjectileAcceleration=0.0
ProjectileEnemyHitRadius=1.0
CanAimDownSight=true
ADSZoomDelay=0.0
ADSZoomSensFactor=0.7
ADSMoveFactor=1.0
ADSStartDelay=0.0
ShootSoundCooldown=0.08
HitSoundCooldown=0.08
HitscanVisualOffset=X=0.000 Y=0.000 Z=-80.000
ADSBlocksShooting=false
ShootingBlocksADS=false
KnockbackFactorAir=0.0
RecoilNegatable=false
DecalType=0
DecalSize=30.0
DelayAfterShooting=0.0
BeamTracksCrosshair=true
AlsoShoot=
ADSShoot=
StunDuration=0.0
CircularSpread=true
SpreadStationaryVelocity=0.0
PassiveCharging=false
BurstFullyAuto=true
FlatKnockbackHorizontal=0.0
FlatKnockbackVertical=0.0
HitscanRadius=0.0
HitscanVisualRadius=1.0
TaggingDuration=0.0
TaggingMaxFactor=1.0
TaggingHitFactor=1.0
ProjectileTrail=None
RecoilCrouchScale=1.0
RecoilADSScale=1.0
PSRCrouchScale=1.0
PSRADSScale=1.0
ProjectileAcceleration=0.0
AccelIncludeVertical=true
AimPunchAmount=0.0
AimPunchResetTime=0.1
AimPunchCooldown=0.5
AimPunchHeadshotOnly=false
AimPunchCosmeticOnly=true
MinimumDecelVelocity=0.0
PSRManualNegation=false
PSRAutoReset=true
AimPunchUpTime=0.05
AmmoReloadedOnKill=0
CancelReloadOnKill=false
FlatKnockbackHorizontalMin=0.0
FlatKnockbackVerticalMin=0.0
ADSScope=No Scope
ADSFOVOverride=77.139999
ADSFOVScale=Apex Legends
ADSAllowUserOverrideFOV=true
IsBurstWeapon=false
ForceFirstPersonInADS=true
ZoomBlockedInAir=false
ADSCameraOffsetX=0.0
ADSCameraOffsetY=0.0
ADSCameraOffsetZ=0.0
QuickSwitchTime=0.1
Explosive=false
Radius=500.0
DamageAtCenter=100.0
DamageAtEdge=0.0
SelfDamageMultiplier=0.5
ExplodesOnContactWithEnemy=false
DelayAfterEnemyContact=0.0
ExplodesOnContactWithWorld=false
DelayAfterWorldContact=0.0
ExplodesOnNextAttack=false
DelayAfterSpawn=0.0
BlockedByWorld=false
SpreadSSA=1.0,1.0,-1.0,0.0
SpreadSCA=1.0,1.0,-1.0,0.0
SpreadMSA=1.0,1.0,-1.0,0.0
SpreadMCA=1.0,1.0,-1.0,0.0
SpreadSSH=1.0,1.0,-1.0,0.0
SpreadSCH=1.0,1.0,-1.0,0.0
SpreadMSH=1.0,1.0,-1.0,0.0
SpreadMCH=1.0,1.0,-1.0,0.0
MaxRecoilUp=0.0
MinRecoilUp=0.0
MinRecoilHoriz=0.0
MaxRecoilHoriz=0.0
FirstShotRecoilMult=1.0
RecoilAutoReset=false
TimeToRecoilPeak=0.05
TimeToRecoilReset=0.35
AAMode=0
AAPreferClosestPlayer=false
AAAlpha=0.05
AAMaxSpeed=1.0
AADeadZone=0.0
AAFOV=30.0
AANeedsLOS=true
TrackHorizontal=true
TrackVertical=true
AABlocksMouse=false
AAOffTimer=0.0
AABackOnTimer=0.0
TriggerBotEnabled=false
TriggerBotDelay=0.0
TriggerBotFOV=1.0
StickyLock=false
HeadLock=false
VerticalOffset=0.0
DisableLockOnKill=false
UsePerShotRecoil=false
PSRLoopStartIndex=0
PSRViewRecoilTracking=0.45
PSRCapUp=9.0
PSRCapRight=4.0
PSRCapLeft=4.0
PSRTimeToPeak=0.095
PSRResetDegreesPerSec=40.0
UsePerBulletSpread=false
PBS0=0.0,0.0
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faces
0.000000 0.000000 1.000000 1.000000 0.000000 0 1 2 3 0x00000000 internal/editor/textures/editor_clip
0.000000 0.000000 1.000000 1.000000 0.000000 6 5 4 7 0x00000000 internal/editor/textures/editor_clip
0.000000 0.000000 1.000000 1.000000 0.000000 2 1 5 6 0x00000000 internal/editor/textures/editor_clip
0.000000 0.000000 1.000000 1.000000 0.000000 0 3 7 4 0x00000000 internal/editor/textures/editor_clip
0.000000 0.000000 1.000000 1.000000 0.000000 3 2 6 7 0x00000000 internal/editor/textures/editor_clip
0.000000 0.000000 1.000000 1.000000 0.000000 1 0 4 5 0x00000000 internal/editor/textures/editor_clip
brush
vertices
614.000000 116.000000 1144.000000
614.000000 116.000000 1130.000000
550.000122 116.000000 1130.000000
550.000122 116.000000 1144.000000
614.000000 4.000000 1144.000000
614.000000 4.000000 1130.000000
550.000122 4.000000 1130.000000
550.000122 4.000000 1144.000000
faces
0.000000 0.000000 1.000000 1.000000 0.000000 0 1 2 3 0x00000000 internal/editor/textures/editor_clip
0.000000 0.000000 1.000000 1.000000 0.000000 6 5 4 7 0x00000000 internal/editor/textures/editor_clip
0.000000 0.000000 1.000000 1.000000 0.000000 2 1 5 6 0x00000000 internal/editor/textures/editor_clip
0.000000 0.000000 1.000000 1.000000 0.000000 0 3 7 4 0x00000000 internal/editor/textures/editor_clip
0.000000 0.000000 1.000000 1.000000 0.000000 3 2 6 7 0x00000000 internal/editor/textures/editor_clip
0.000000 0.000000 1.000000 1.000000 0.000000 1 0 4 5 0x00000000 internal/editor/textures/editor_clip
entity
type CameraPath
UInt8 posLerp 2
UInt8 angleLerp 2
entity
type PlayerSpawn
Vector3 position 582.000000 0.000000 1168.000000
Vector3 angles 630.000000 0.000000 0.000000
Bool8 teamB 0
Bool8 initialSpawn 0
Bool8 modeCTF 0
Bool8 modeFFA 0
Bool8 modeTDM 0
Bool8 mode1v1 0
Bool8 modeRace 0
Bool8 mode2v2 0
entity
type PlayerSpawn
Vector3 position 312.000000 6.000000 1040.000000
Vector3 angles 405.000000 0.000000 0.000000
Bool8 teamA 0
Bool8 initialSpawn 0
Bool8 modeCTF 0
Bool8 modeFFA 0
Bool8 modeTDM 0
Bool8 mode1v1 0
Bool8 modeRace 0
Bool8 mode2v2 0
entity
type PlayerSpawn
Vector3 position 316.000000 8.000000 1304.000000
Vector3 angles 495.000000 0.000000 0.000000
Bool8 teamA 0
Bool8 initialSpawn 0
Bool8 modeCTF 0
Bool8 modeFFA 0
Bool8 modeTDM 0
Bool8 mode1v1 0
Bool8 modeRace 0
Bool8 mode2v2 0
|
37e2f5387dabe87e8f1e0fca2bd9e9a43ea5ac8e | 449d555969bfd7befe906877abab098c6e63a0e8 | /2681/CH1/EX1.10/Ex1_10.sce | 49ccbf4670a73527ce654e10fd9bdbbf24b90b14 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 426 | sce | Ex1_10.sce | //FIND THE DIRECTION OF POWER FLOW OF MICROWAVE
//given
clc
function w=cross_prod(E,F)//function to determine the cross product of two vectors
D=[E(:),F(:)]
w(1)=det([[1;0;0],D])
w(2)=det([[0;1;0],D])
w(3)=det([[0;0;1],D])
endfunction
E=[0 1 0]
F=[1 0 0]
q=cross_prod(E,F)
disp(q','the cross product of the given fields')//towards az
//ERROR in book as cross product of two perpendicular vector gives the third
|
4eef74dd6ff9b14bebe57e0783d3e1dde9bf4577 | 27fecbbeb6c49dcf03b9bddf1b867c31e13a3825 | /Simulações/Relatório 03/t3_kiu.sci | 93027669e4cc9f45cc04ec7ccef4ab54de9f4f7e | [] | no_license | LucasHattoriCosta/Poli | 42c9fc2d34c31e01336265fbdac3e4921d56e096 | b1ac609c3675539b4e921909c35ea196ffc44df3 | refs/heads/master | 2023-03-15T12:22:03.745943 | 2020-06-29T17:32:48 | 2020-06-29T17:32:48 | null | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 1,156 | sci | t3_kiu.sci | //Condições iniciais
R = 0.001;
ro = 7850;
volume = 4*%pi*(R^3)/3;
m = ro*volume;
g = 9.8;
r = 1;
s0 = -4*r;
v0 = 0;
t = linspace(0,10,1000);
s= zeros(1,1000);
v = zeros(1,1000);
funcprot(0);
function [ds]=f(t, y)
ds1=y(2);
ds2=(-g/(4*r))*(y(1));
ds=[ds1;ds2];
endfunction
function [z]=h(t, y)
z1=16+f(1)^2;
z2=f(2);
z=[z1;z2]
endfunction
x = ode("root",[s0;v0],0,t,f,1,h);
s = x(1,:);
v = x(2,:);
t1 = linspace(0,10,999)
dv = diff(v)
dt = diff(t)
for i = 1:(length(dv))
a(i) = dv(i)/dt(i)
end
T = m*(v^2)/2;
V = m*g*(s^2)/(8*r);
E = T + V;
//Gráficos
f1=scf(1);
plot(t, s);
xtitle("posição em função do tempo", "t","s");
f2=scf(2);
plot(t, v);
xtitle("velocidade em função do tempo", "t","v");
f3=scf(3);
plot(t1, a');
xtitle("aceleração em função do tempo", "t", "a");
f4=scf(4);
plot(t, T);
xtitle("energia cinética em função do tempo", "t", "T")
f5=scf(5);
plot(t, V);
xtitle("energia potencial em função do tempo", "t", "V")
f6=scf(6);
plot(t, E);
xtitle("energia mecânica em função do tempo", "t", "E")
f7=scf(7);
plot(s, v);
xtitle("velocidade em função do espaço", "espaço", "velocidade")
|
eda1c3e932216d8a0ab56a775b1aafd073d6085b | 449d555969bfd7befe906877abab098c6e63a0e8 | /1247/CH5/EX5.19/example5_19.sce | 6c44386198da55e768eccfcbf1ac98dfe2e3067e | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 860 | sce | example5_19.sce | clear;
clc;
// Stoichiometry
// Chapter 5
// Energy Balances
// Example 5.19
// Page 245
printf("Example 5.19, Page 245 \n \n");
// solution
H1 = 482.9 // kJ/kg
H2 = 273.4
fi1 = 100*(H1-H2) // kJ/h
T1 = 313.15
T2 = 403.15
fi11 = 21.3655*(T2-T1)+64.2841*10^-3*(T2^2-T1^2)/2-41.0506*10^-6*(T2^3-T1^3)/3+9.7999*10^-9*(T2^4-T1^4)/4 // kJ/h
// at 20 MPa
h1 = 211.1
Ts = 277.6
H11 = 427.8
x = poly(0, 'x')
p = x*h1+(100-x)*H11-100*H2
a = roots(p)
fi2 = (100-a)*(H11-h1) // kJ/h
h2 = -148.39
H3 = 422.61
y = poly(0, 'y')
p1 = 100*176.18-(100-y)*H3+h2*y
b = roots(p1)
fi3 = 100*(h1-176.8)
H = fi3+24021
H4 = H/(100-43.16)
// from ref 23
T = 262.15
printf(" (a) \n \n Yield of dry ice = "+string(b)+" kg. \n \n \n (b) \n \n Percent liquifaction = "+string(a)+". \n \n \n (c) \n \n Temp of vented gas = "+string(T)+" K.")
|
abc451a89b63de60b0e0b8d28fd110a621e3bb6b | 449d555969bfd7befe906877abab098c6e63a0e8 | /2792/CH9/EX9.4/Ex9_4.sce | 95c5081b735411f2c7e1beb31ac401064a3bd4f8 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 1,849 | sce | Ex9_4.sce | clc
mu_n=600
disp("mu_n = "+string(mu_n)+"cm^2(Vs)^-1") //initializing value of mobility of electron
mu_p = 200
disp("mu_p = "+string(mu_p)+"cm^2(Vs)^-1") //initializing value of mobility of holes
kbT = 0.026
disp("kbT = "+string(kbT)+"eV") //initializing value of kbT at 300K
apsilen = 11.9*8.85*10^-14
disp("apsilen = "+string(apsilen)+"F/cm") //initializing value of relative permitivity
e = 1.6*10^-19
disp("e= "+string(e)+"C")//initializing value of charge of electron
Na=5*10^16
disp("Na = "+string(Na)+"cm^-3") //initializing value of doped carrier concentration
ni = 1.5*10^10
disp("ni= "+string(ni)+"cm^-3")//initializing value of intrinsic carrier concentration
Vfb = -0.5
disp("Vfb= "+string(Vfb)+"eV")//initializing value of flat band voltage
Eox = 1.583*8.85*10^-14
disp("Eox= "+string(Eox))//initializing value of relative permitivity of oxide
dox = 200*10^-8
disp("dox= "+string(dox)+"cm")//initializing value of thickness of oxide
sigma_1= Na*e*mu_p
disp("The channel conductivity under flat band sigma_1= Na*e*mu_p= "+string(sigma_1)+" ohm^-1cm^-1")//calculation
sigma_2= Na*e*mu_n
disp("The channel conductivity at inversion sigma_1= Na*e*mu_n= "+string(sigma_2)+" ohm^-1cm^-1")//calculation
phi_F= (-kbT*log(Na/ni))
disp("The potential phi_F= (-kbT*log(Na/ni))= "+string(phi_F)+" V")//calculation
Qs = sqrt((4*apsilen*(-phi_F))*(e*Na))
disp("The maximum depletion width is ,Qs = sqrt((4*apsilen*(-phi_F))*(e*Na))= "+string(Qs)+" C cm^-2")//calculation
Vs = -(2*phi_F)
disp("The surface potential is ,Vs = -(2*phi_F)= "+string(Vs)+" V")//calculation
VT = Vfb+Vs+((Qs*dox)/Eox)
disp("In the absence of any oxide charge, the threshold voltage is ,VT = Vfb+Vs+((Qs*dox)/Eox) = "+string(VT)+" V")//calculation
// Note : due to different precisions taken by me and the author ... my answer differ
|
6291b0dcad38f6431159a4d64f2b1820399ac6d1 | 449d555969bfd7befe906877abab098c6e63a0e8 | /147/CH8/EX8.6/Example8_6.sce | e147d21deb57d9051699a72b3675c1a765c66946 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 314 | sce | Example8_6.sce | close();
clear;
clc;
Beta = 100;
Ibq = 20*10^(-6);
Vcc = 15;//V
Rc = 3000;//ohm
Icbo = 0;
alpha = Beta/(Beta+1);
Icq = Beta*Ibq;
Ieq = Icq/alpha;
Vceq = Vcc-Icq*Rc;
//Part (c)
Rc = 6000;
Vceq_c = Vcc-Icq*Rc;
mprintf('(a):Ieq = %0.2f mA\n(b):Vceq = %0.0f V\n(c):Vceq = %0.0f V',Ieq*1000,Vceq,Vceq_c); |
799389292f24eb8808f70d39a02d3e0352838015 | 449d555969bfd7befe906877abab098c6e63a0e8 | /764/CH4/EX4.21.b/solution4_21.sce | 5181a08a8b392f7256e9c18e2d5cf001ace719ef | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 1,345 | sce | solution4_21.sce |
//Function to round-up a value such that it is divisible by 5
function[v] = round_five(w)
v = ceil(w)
rem = pmodulo(v,5)
if (rem ~= 0) then
v = v + (5 - rem)
end
endfunction
//Obtain path of solution file
path = get_absolute_file_path('solution4_21.sce')
//Obtain path of data file
datapath = path + filesep() + 'data4_21.sci'
//Clear all
clc
//Execute the data file
exec(datapath)
//Calculate permissible tensile stress sigma (N/mm2)
sigma = Sut/fs
//Assume value of t to be 1mm
t = 1
//All dimensions in mm
bi = 3 * t
h = 3 * t
Ri = 2 * t
Ro = 5 * t
ti = t
to = 0.75 * t
Rn = ((ti * (bi - to)) + (to * h))/((bi - to)*log((Ri + ti)/Ri)+(to * log(Ro/Ri)))
R = Ri + ((((1/2)*to*(h^2)) + ((1/2)*(ti^2)*(bi - to)))/((to*h) + (ti*(bi - to))))
//Calculate eccentricity e (mm)
e = R - Rn
hi = Rn - Ri
A = (bi * ti) + (to * Ri)
//Calculate the direct tensile stress T (N/mm2)
T = (P * 1000)/A
//The polynomial obtained is as follows
C = (((R * P * 1000 * hi)/(A * e * Ri)) + T)
D = (P * 1000 * l * hi)/(A * e * Ri)
p = [(-1 * sigma) 0 C D]
r = roots(p)
//Calculate the true value of t (mm)
real_part = real(r)
for i = 1:1:3
if(real_part(i)>0)
t = real_part(i)
break
end
end
t = round_five(t)
//Print results
printf('\nThe value of t = %f mm\n',t)
|
5e5eea88c8177ba62b94253a3c0158c22d5c8fdd | 449d555969bfd7befe906877abab098c6e63a0e8 | /3651/CH4/EX4.1/1.sce | fcf02c588551690ff937215b385190b43cdeeed4 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 490 | sce | 1.sce |
//Variable declaration
m=9.1*10**-31; //mass(kg)
nx=1;
ny=1
nz=1
n=6;
a=1; //edge(m)
h=6.63*10**-34; //planck's constant
k=1.38
//Calculation
E1=h**2*(nx**2+ny**2+nz**2)/(8*m*a**2);
E2=h**2*n/(8*m*a**2);
E=E2-E1; //energy difference(J)
T=(2*E2*10**37)/(3*k*10**-23)
//Result
printf('energy difference is%0.3f *10**-37 J \n ',(E*10**37))
printf('3/2*k*T = E2 =%0.3f *10**-37 J \n ',(E2*10**37))
printf('T =%0.3f *10**-14 K \n ',(T/10**23))
|
659f915b147f6bfd71512a771175e3384557f7da | 8d952a06e3809a06825a3be7b067201f3652f16a | /debug/bin/BackDoor/help/builder_help.sce | e0456a9f5cfbdc0eaddf3e9e94463426dd76b3d5 | [
"GPL-3.0-only",
"MIT"
] | permissive | andyLaurito92/haikunet | b771eaf6bd91292485f0a49698ce123b9308d676 | db44623b248c56735c28a5f589c3239dc7e9855e | refs/heads/master | 2021-06-14T12:38:38.996450 | 2021-05-05T18:26:02 | 2021-05-05T18:26:02 | 75,564,849 | 2 | 1 | MIT | 2021-05-05T18:26:26 | 2016-12-04T21:12:31 | C++ | UTF-8 | Scilab | false | false | 187 | sce | builder_help.sce | // Copyright INRIA 2008
// This file is released into the public domain
help_dir = get_absolute_file_path('builder_help.sce');
tbx_builder_help_lang("en_US", help_dir);
clear help_dir;
|
84b602334866f05ef769b839d142a986fa4f3e92 | 54cca39cd1cf7f62b001c8a4d64dcc3d29e3cb4e | /CentralLimitTheorem/randomwalk.sce | 7b931c2131cc593bf775ae854a38ed902fc7d9d3 | [] | no_license | hamling-ling/NumericalResearches | d2487c2566c24ba3dc674e7e17f1745c1020d542 | a824357d7650d3ed86220f1315ee37e577285a7d | refs/heads/master | 2021-01-25T08:36:58.455319 | 2015-04-22T15:17:21 | 2015-04-22T15:17:21 | 7,775,139 | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 371 | sce | randomwalk.sce | clear;
// sampling num
samplenum=500
// number of repetition
repeat=1000;
R=grand(repeat,samplenum,'uin',0,1);
R=1-R*2;
// avarage of repetition
X=sum(R,'c');
//plot2d(X);
xmin=-samplenum/10;
xmax=samplenum/10;
param=[xmin:1:xmax];
histplot(param,X)
n=repeat;
p=1/2;
avg=0;
s=sqrt(n*p*(1-p))
x=[-50:0.05:50];
plot(x,(1/(s*sqrt(2*%pi)))*exp(-((avg-x).^2)/(2*s^2)));
|
5eba3dad4313a2cf77ec5b904740cdb4b23d8344 | 449d555969bfd7befe906877abab098c6e63a0e8 | /905/CH1/EX1.21/1_21.sce | 1cbe3414095c4fcaa48433645da24dc20596fa1c | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 1,535 | sce | 1_21.sce | clear;
clc;
// Illustration 1.21
// Page: 60
printf('Illustration 1.21 - Page:60 \n\n');
// Solution
//*****Data*****//
// a-oxygen b-nitrogen
T = 293; // [K]
P = 0.1; // [atm]
d = 0.1*10^-6; // [m]
e = 0.305; // [porosity]
t = 4.39; // [tortuosity]
k = 1.3806*10^-23; // [J/K]
l = 2*10^-3; // [m]
R = 8.314; // [cubic m.Pa/mole.K]
x_a1 = 0.8;
x_a2 = 0.2;
M_a = 32; // [gram/mole]
M_b = 28; // [gram/mole]
//*****//
// Using data from Appendix B for oxygen and nitrogen, and equation (1.45)
sigma_a = 3.467; // [Angstrom]
sigma_b = 3.798; // [Angstrom]
sigma_AB = ((sigma_a+sigma_b)/2)*10^-10; // [m]
lambda = k*T/(sqrt(2)*3.14*(sigma_AB^2)*P*1.01325*10^5); // [m]
// From equation 1.101
K_n = lambda/d;
printf("The value of a dimensionless ratio, Knudsen number is %f\n\n",K_n);
// If K_n is greater than 0.05 then transport inside the pores is mainly by Knudsen diffusion
// Using equation 1.103
D_Ka = (d/3)*(sqrt(8*R*T)/sqrt(3.14*M_a*10^-3)); // [square m/s]
// Using equation 1.107
D_Kaeff = D_Ka*e/t; // [square m/s]
p_a1 = (x_a1*P)*1.01325*10^5; // [Pa]
p_a2 = (x_a2*P)*1.01325*10^5; // [Pa]
// Using equation 1.108
N_a = D_Kaeff*(p_a1-p_a2)/(R*T*l); // [mole/square m.s]
// Now using the Graham’s law of effusion for Knudsen diffusion
// N_b/N_a = -sqrt(M_a/M_b) ,therefore
N_b = -N_a*sqrt(M_a/M_b); // [mole/square m.s]
printf("The diffusion fluxes of both components oxygen and nitrogen are %e mole/square m.s and %e mole/square m.s respectively\n",N_a,N_b);
|
bc36f448dfe0d25c58a6edd057ba09276fd2c05c | 449d555969bfd7befe906877abab098c6e63a0e8 | /3866/CH6/EX6.7/Ex6_7.sce | 12b013a117e6c905c0b0f251fa98bc913ea5ce8e | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 483 | sce | Ex6_7.sce | clc; clear; close;
//a
Reff=12.5;//in kiloohm
r=2/4;
Cload=4.2;//in fermifarad
T=4*Reff*r*Cload;
disp(T,'total delay(in picoseconds)=');
//b
Reff1=30;//in kiloohm
Cfanout=2;//in fermifarad
Cself=1;//in fermifarad
r1=2/6;
Cload1=Cself+Cfanout;
PLH=Reff1*Cload1*r1;
PHL=Reff*r*Cload1;
T1=2*(PHL+PLH);
disp(PLH,'rise delay(in picoseconds)=');
disp(PHL,'fall delay(in picoseconds)=');
disp(T1,'total delay(in picoseconds)=');
//answers vary due to roundoff error
|
d2a14ccbd58e6a40945cd0cdeabbb200375a7eb6 | a5f0fbcba032f945a9ee629716f6487647cafd5f | /Machine_Learning/demos/Ensemble_Demo.sce | 90067678ee72f90e8221a347f4b712efcf9f0cd3 | [
"BSD-2-Clause"
] | permissive | SoumitraAgarwal/Scilab-gsoc | 692c00e3fb7a5faf65082e6c23765620f4ecdf35 | 678e8f80c8a03ef0b9f4c1173bdda7f3e16d716f | refs/heads/master | 2021-04-15T17:55:48.334164 | 2018-08-07T13:43:26 | 2018-08-07T13:43:26 | 126,500,126 | 1 | 1 | null | null | null | null | UTF-8 | Scilab | false | false | 743 | sce | Ensemble_Demo.sce | // Demo for Ensemble classifier -- Scilab
getd('../macros')
// Data preparation for gaussian
M = csvRead('Datasets/standard.csv')
x = M(:, [1,2,3,4,5,6,7,8]);
y = M(:, 9);
y(or(isnan(x),'c'),:) = []
x(or(isnan(x),'c'),:) = []
probMat = naiveBayes(x, y)
testx = x;
pred1 = naiveBayesGaussian(x, y, probMat, testx)
// Data preparation for multinomial
x = x(:, 1);
probMat = naiveMultBayes(x, y)
testx = x;
pred2 = naiveMultBayesGaussian(x, y, probMat, testx)
increment = 0.01
pred = ensemble(pred1, pred2, y, increment)
disp('Error through classifier 1 = ' + string(0.5*sqrt(norm(pred1 - y))))
disp('Error through classifier 2 = ' + string(0.5*sqrt(norm(pred2 - y))))
disp('Error through ensemble = ' + string(0.5*sqrt(norm(pred - y)))) |
c5025a9a53c771394495f052ff288a8c474cabe3 | 449d555969bfd7befe906877abab098c6e63a0e8 | /3821/CH13/EX13.8/Example13_8.sce | 6f64b20481ff7fc14bf4591b4bb6ddf1b04684f6 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 784 | sce | Example13_8.sce | ////Chapter 13 Steam Engines
////Example 13.8 Page No 288
////Find Diagram factor
//Input data
clc;
clear;
P1=10; //Inlet pressure
Pb=1; //Back pressure
rc=3; //Expansion ratio
a=12.1; //Area of indicator diagram
b=7.5; //Length of indicator diagram
S=3; //Pressure scale
//Calculation
Pm=round((P1/rc)*(1+log(rc))-Pb ); //Therotical mean effective pressure Pm
Pma=a/b*S; //Actual mean effective pressure Pma
K=Pma/Pm; //Diagram factor
///Output
printf('Therotical mean effective pressure= %f bar \n',Pm);
printf('Actual mean effective pressure= %f bar \n',Pma);
printf('Diagram factor= %f \n',K);
|
12c1926d909287562b8e04655d670f2072baf715 | 449d555969bfd7befe906877abab098c6e63a0e8 | /866/CH7/EX7.1/7_1.sce | d1d3da82ae896df06ae00f33370c1dc0823f0897 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 263 | sce | 7_1.sce | clc
//initialisation of variables
P= 800*10^3
sigmamax= 400
//CALCULATIONS
Amin= P/sigmamax
B= sqrt(Amin/2)
//RESULTS
printf ('Amin= %.2f mm^2',Amin)
printf (' \n B=%.2f mm(Therefore the min dimensions of the column cross section are 31.6mm*63.2mm)',B)
|
94f4c414acfb240ca14e04627b78ef633c0876a4 | 449d555969bfd7befe906877abab098c6e63a0e8 | /884/CH5/EX5.6/Example5_6.sce | b2ec2e6fcaf6eb461ceb53ceb46604a078766766 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 298 | sce | Example5_6.sce | //Ideal Gas Equation
clear;
clc;
printf("\t Example 5.6\n");
P1=1.2;// pressure initial, atm
T1=18+273;//temperature initial, K
T2=85+273;//temperature final, K
//volume is constant
P2=P1*T2/T1;// pressure final,atm
printf("\t the final pressure is : %4.2f atm\n",P2);
//End
|
0b0e24a3102931b9e2914ffa1179a6738e27d738 | 449d555969bfd7befe906877abab098c6e63a0e8 | /3669/CH3/EX3.2/2.sce | 7d2eef86bcf64c666e349164d0441a658c880dc3 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 457 | sce | 2.sce | //Variable declaration
n=1; //order of diffraction
theta1=8+(35/60); //angle(degrees)
d=0.282; //spacing(nm)
theta2=90;
//Calculation
theta1=theta1*%pi/180; //angle(radian)
lamda=2*d*sin(theta1)/n; //wavelength(nm)
theta2=theta2*%pi/180; //angle(radian)
nmax=2*d/lamda; //maximum order of diffraction
//Result
printf('wavelength is %0.3f nm \n',(lamda))
printf('maximum order of diffraction is %0.3f \n',(nmax)) |
e243260ef990f5cf39665aa5b3a66463809fa7ea | 449d555969bfd7befe906877abab098c6e63a0e8 | /1904/CH7/EX7.5/7_5.sce | 4d03b8b439e2cb1b3bbf71c80a4966342a38c9f7 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 1,044 | sce | 7_5.sce | //To Find the Total Load and Total steady state voltage drop
//Page 336
clc;
clear;
//Length in feet
Lsd=100; //Service Drop Line
Lsl=200; //Secondary Line
SB=75; //Transformer Capacity in kVA
pf=0.9; //Load Power Factor
//From the Tables
ISL=129.17; //Secondary Line Current
ISD=41.67; //Service Drop Current
KSD=0.01683; //Service Drop Cable Constant
KSL=0.0136; //Secondary Cable Constant
//for Transformer
R=0.0101; //Resistance in per unit
X=0.0143; //Reatance in per unit
//From the Diagram
ST=(3+2+8+6)+(5+6+7+4)+(6+7+8+10); //Total Load on transformer
STpu=ST/SB; //In Per unit;
//The Above value also corresponds to the Current as Well
I=STpu; //Current in Per Unit
VDT=I*((R*pf)+(X*sind(acosd(pf)))); //Voltage Drop in the Transformer
VDSL=KSL*(Lsl*ISL/(10^4)); //Secondary Line
VDSD=KSD*(Lsd*ISD/(10^4)); //Service Drop Line
VD=VDT+VDSD+VDSL; //Total Voltage Drop
printf('\na)The Load in transformer is %g kVA or %g pu\n',ST,STpu)
printf('b) The Total Voltage Drop is %g pu V\n',VD)
|
659143fa9767ac615ebed96003bcf5da8efe1350 | 449d555969bfd7befe906877abab098c6e63a0e8 | /1271/CH12/EX12.5/example12_5.sce | 3fe7fb7a39072bbc93c7d2e69268bf3aebe498c4 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 484 | sce | example12_5.sce | clc
// Given that
t = 15 // half-life of radioactive element in years
r = 0.025 // ratio of mass of element present in specimen to the intial mass of element
// Sample Problem 5 on page no. 12.33
printf("\n # PROBLEM 5 # \n")
printf("Standard formula used \n")
printf(" lambda = 0.693 / t_1/2 (Decay constant) \n N =N_0*e^(-lambda*t) \n")
lambda = 0.693 / t
T = (1 / lambda) * log(1 / r)
printf("\n Period in which 2.5 percent of the initial quantity left over is %f years.",T)
|
da9c57394e59904de8747a750c0320bf40047874 | 449d555969bfd7befe906877abab098c6e63a0e8 | /68/CH11/EX11.2/ex2.sce | 189d8aaba0e30bae0de86dcd0cedf9c5dbb7f3e1 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 741 | sce | ex2.sce | // Example 11.2 Design of two-stage CMOS op-amp
uC_n=50*10^-6; // u_n*C_ox (A/V^2)
uC_p=20*10^-6; // u_p*C_ox (A/V^2)
V_tn0=1; // (V)
V_tp0=-1; // (V)
fie_f=0.6/2; // (V)
y=0.5; // (V^1/2)
V_DD=5; // (V)
W_n=4*10^-6; // (m)
L_n=2*10^-6; // (m)
W_p=10*10^-6; // (m)
L_p=2*10^-6; // (m)
W=10*10^-6; // (m)
L=10*10^-6; // (m)
C_B=1*10^-12; // bit line capacitance (F)
deltaV=0.2; // 0.2 V decrement
WbyL_eq=1/(L_p/W_p+L_n/W_n); // WbyL_eq=(W/L)_eq
// Equivalent transistor will operate in saturation
I=(uC_n*WbyL_eq*(V_DD-V_tn0)^2)/2
r_DS=1/(uC_n*(W_n/L_n)*(V_DD-V_tn0));
v_Q=r_DS*I; // v_Q=r_DS*I
I_5=0.5*10^-3; // (A)
deltat=C_B*deltaV/I_5;
disp(deltat, "The time (s) required to develop an output voltage of 0.2V") |
26496c186662decc8d5bec4fe1fe09571d0302b8 | 449d555969bfd7befe906877abab098c6e63a0e8 | /3850/CH27/EX27.2/Ex27_2.sce | 3d6d4e2f5fd4aacf5555960821fd7d8e3c04b7a6 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 558 | sce | Ex27_2.sce |
//Find the Amount of Heat required to raise the temperature to 400 Kelvin
//Example 27.2
clc;
clear;
V=0.2;//Volume of tank in m^3
p=1*10^5;//Pressure of Helium Gas in N/M^2
T1=300;//Initial Temperature of Helium Gas in Kelvin
T2=400;//Final Temperature of Helium Gas in Kelvin
R=8.31;//Universal Gas Constant in J/mol-K
n=int((p*V)/(R*T1));//Amount of moles of Helium Gas
Cv=3;//Molar Heat Capacity at Constant Volume
Q=n*Cv*(T2-T1);//Amount of Heat Required in calories
printf("The amount of Heat required=%d cal",Q);
|
661b63365e21f79c6716cd2a287f944d93d988d8 | 449d555969bfd7befe906877abab098c6e63a0e8 | /1895/CH5/EX5.19/EXAMPLE5_19.SCE | 9ebd9021e9eb1269bf8bc809bdd155e8262203af | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 1,092 | sce | EXAMPLE5_19.SCE | //ANALOG AND DIGITAL COMMUNICATION
//BY Dr.SANJAY SHARMA
//CHAPTER 5
//ANGLE MODULATION
clear all;
clc;
printf("EXAMPLE 5.19(PAGENO 222)");
//given
f_m1 = 1*10^3//modulating frequency for first case
f_m2 = 500//modulating frequency for second case
V_m1 = 2//modulating voltage for first case
V_m2 = 8//modulating volatge for second case
delta_f1 = 4*10^3//frequency deviation for first case
//calculations
k = delta_f1/V_m1//constant
delta_f2 = k*V_m2//frequency deviation for second case
m_f1 = delta_f1/f_m1//modulation index for first case
m_f2 = delta_f2/f_m2//modulation index for second case
BW1 = 2*(delta_f1 + f_m1)//bandwidth for first case
BW2 = 2*(delta_f2 + f_m2)//bandwidth for second case
//results
printf("\n\ni.a.Modulation index for first case = %.2f",m_f1);
printf("\n\n b.Bandwidth for first case = %.2f Hz",BW1);
printf("\n\nii.a.Modulation index for second case = %.2f",m_f2);
printf("\n\n b .Bandwidth for second case = %.2f Hz",BW2);
printf("\n\nNote: Their is error in textbook in the calculation of second case bandwidth ");
|
e0da34931761018737534ea6d483e56c108df103 | 449d555969bfd7befe906877abab098c6e63a0e8 | /3871/CH5/EX5.11/Ex5_11.sce | 9b47481e0ad11deed921acc41ea04301adcdde47 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 603 | sce | Ex5_11.sce | //===========================================================================
//chapter 5 example 11
clc;clear all;
//variable declaration
V = 300; //voltage in V
R = 12000; //coil resistance in Ω
B = 6*10^-2; //flux density in Wb/m**2
l = 0.04; //length in m
r = 0.03; //width in m
N = 100;
Tc = 25*10^-7; //torque in Nm per degree
//calculations
i = V/(R); //current in A
Td = N*B*i*l*r; //deflecting Torque in Nm
//Tc=Td;
//Tc =(25*10^-7)*theta
theta = Td/(Tc); //defelction in °
//result
mprintf('defelction = %3.0f °",theta);
|
ae381047c45b0963be361f21cbbac7261c6563df | 449d555969bfd7befe906877abab098c6e63a0e8 | /3446/CH17/EX17.1/Ex17_1.sce | e8db09e657a7a22f282d1f570b64bf33341575e2 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 1,686 | sce | Ex17_1.sce | // Exa 17.1
//To calculate-
//(a) average busy-hour traffic per subscriber,
//(b) traffic capacity per cell,
//(c) required number of base stations per zone, and
//(d) the hexagonal cell radius for the zone.
clc;
clear all;
Susage=150;//subscriber usage per month in mins
days=24;//days per month
busyhrs=6;//in a day
BW=4.8*10^3; //in kHz
Freqreuse=4/12;//Frequency reuse plan
chwidth=200; //in kHz
subscriber=50000;//Present subscriber count
Sgrowth=0.05;//Growth rate per year
Area=500; //in km
BTScapacity=30; //in Erlangs
N=4; //Initial installation design years
//solution
Erlangspersub=Susage/(days*busyhrs*60);
printf('Average busy-hour traffic per subscriber is %.4f Erlangs \n ',Erlangspersub);
RFcarriers=BW/chwidth;
RFcarrier_percell=RFcarriers/((Freqreuse^-1)*4); //freq reuse factor of 4
//Assuming 2 control channels per cell
CC=2;//control channels
TC_percell=2*RFcarriers/3-CC;
//Referring Erlang-B table in Appendix A
disp("Referring Erlang-B table in Appendix A,Traffic capacity of a GSM cell at 2% GoS for 14 channels = 8.2 Erlangs ");
Tcapacity=8.2;// in Erlangs
disp("There are 3 cells per BTS");
BTS=3;
Traffic_perBTS=Tcapacity*BTS;
printf(' Traffic capacity per BTS is %.1f Erlangs ',Traffic_perBTS);
disp("Therefore, Traffic per BTS is less than BTS capacity(30 Erlangs)")
maxsubscriber=Traffic_perBTS/Erlangspersub;
initialsub=subscriber*(1+Sgrowth)^N;
BTS_perZone=initialsub/maxsubscriber;
printf(' The required number of base stations per zone are %d \n ',round(BTS_perZone));
cellRadius=(Area/(BTS_perZone*2.6))^0.5;
printf('The hexagonal cell radius is %.1f km \n ',cellRadius);
|
22dea54b829d9ff3d593b47b5b793174f9a80358 | 449d555969bfd7befe906877abab098c6e63a0e8 | /2414/CH4/EX4.7/Ex4_7.sce | 36e0b8a5ba96e482652c9a800fa09678ff350da2 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 384 | sce | Ex4_7.sce | clc;
clear all;
//chapter 4
//page no 125
//example 4.7
//misprinted example number
pulse_width=2*10^-6; //second
rise_time=10*10^-9; //second
B=.5/pulse_width; //in Hz
mprintf('(a) The aproximate bandwidth for coarse reproduction is B=%i KHz\n',B*10^-3)
B=.5/rise_time;
mprintf(' (b) The aproximate bandwidth for fine reproduction is B=%i MHz\n',B*10^-6)
|
200a3c7c45639a52b41926eec4353d6cea11e574 | 449d555969bfd7befe906877abab098c6e63a0e8 | /1928/CH4/EX4.15.19/ex_4_15_19.sce | c1d8995621a03a2fcb6d118482ae80ad771b4376 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 415 | sce | ex_4_15_19.sce | //Chapter-4,Example4_15_19,pg 4-36
t1=4*10^-3 //thickness of 1st crystal
n1=400*10^3 //frequency of 1st crystal
n2=500*10^3 //frequency of 2nd crystal
t2=n1*t1/n2 //since frquency is inversly proportional to thickness
printf("thickness of 2nd crystal =")
disp(t2)
printf("meter")
|
c372acb7ec4a5078a3aef9551078bcfb1830f0b1 | a1e35f4e84e806b2dc5831f403d9d0d2fe74674c | /winequality-white_teste2.sce | a11cc153b35aec3a9d67456667b22719221badd6 | [] | no_license | duartk/projeto_IN244 | 5f47f55682b4f8721571c5502998d88e3d303422 | 5873aad7aa2adb94b844e12005d9f4807ac0f78c | refs/heads/master | 2020-11-23T21:58:18.219727 | 2019-12-17T18:36:57 | 2019-12-17T18:36:57 | 227,838,315 | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 959 | sce | winequality-white_teste2.sce | clear
clc
M = csvRead('winequality-white_normalizado.csv')
P=M(2:700,2:12)'; //DADOS DE TREINAMENTO
T=M(2:700,13)'; //SAIDAS DESEJADAS
Q=M(701:1000,2:12)'; // Exemplos usados para teste
TQ=M(701:1000,13)'; // Valores desejados na saída para os exemplos de teste
N=[11 8 4 1];
//Tipos de funções de ativação:
//ann_logsig_activ
//ann_purelin_activ
//ann_tansig_activ
//ann_hardlim_activ
//Define a função de ativação da camada intermediária e da saída
//Se tiverem 2 intermediárias, tem que definir uma função para cada uma
af = ['ann_tansig_activ','ann_tansig_activ','ann_purelin_activ'];
lr = 0.03; //taxa de aprendizado
itermax = 1000; // número máximo de iterações
mse_min = 1e-5; //mínimo erro quadrático médio desejado
gd_min = 1e-5; // variação mínima do gradiente
W = ann_FFBP_gd(P,T,N,af,lr,itermax,mse_min,gd_min)
[y] = ann_FFBP_run(Q,W, af)
disp(y);
xpause(30000)
scf(1)
plot (y)
plot (TQ,'r-')
|
98037c8d582725ede587b1546a16d0aaaf6d7162 | 8217f7986187902617ad1bf89cb789618a90dd0a | /browsable_source/2.3.1/Unix-Windows/scilab-2.3/macros/scicos_blocks/CURV_f.sci | fe639676194aa68195f67ee77c801963f5b69fca | [
"MIT",
"LicenseRef-scancode-warranty-disclaimer",
"LicenseRef-scancode-public-domain"
] | permissive | clg55/Scilab-Workbench | 4ebc01d2daea5026ad07fbfc53e16d4b29179502 | 9f8fd29c7f2a98100fa9aed8b58f6768d24a1875 | refs/heads/master | 2023-05-31T04:06:22.931111 | 2022-09-13T14:41:51 | 2022-09-13T14:41:51 | 258,270,193 | 0 | 1 | null | null | null | null | UTF-8 | Scilab | false | false | 1,727 | sci | CURV_f.sci | function [x,y,typ]=CURV_f(job,arg1,arg2)
x=[];y=[];typ=[];
select job
case 'plot' then
standard_draw(arg1)
case 'getinputs' then
[x,y,typ]=standard_inputs(arg1)
case 'getoutputs' then
[x,y,typ]=standard_outputs(arg1)
case 'getorigin' then
[x,y]=standard_origin(arg1)
case 'set' then
x=arg1
model=arg1(3)
graphics=arg1(2)
[rpar,ipar]=model(8:9)
n=ipar(1)
xx=rpar(1:n);yy=rpar(n+1:2*n)
curwin=xget('window')
win=maxi(windows(:,2))+1
xset('window',win);xsetech([0 0 1 1])
gc=list(rpar(2*n+1:2*n+4),ipar(2:5))
while %t do
[xx,yy,ok,gc]=edit_curv(xx,yy,'axy',[' ',' ',' '],gc)
if ~ok then break,end
n=size(xx,'*')
if or(xx(2:n)-xx(1:n-1)<0) then
message('You have not defined a function')
ok=%f
end
if ok then
model(1)='intplt'
model(11)=[] //compatibility
rect=gc(1)
model(8)=[xx(:);yy(:);rect(:)]
axisdata=gc(2)
model(9)=[size(xx,'*');axisdata(:)]
x(2)=graphics;x(3)=model
break
end
end
xdel(win)
xset('window',curwin)
case 'define' then
xx=[0;1;2];yy=[-5;5;0]
rect=[0,-5,2,5];
axisdata=[2;10;2;10]
ipar=[size(xx,1);axisdata(:)]
rpar=[xx;yy;rect(:)]
model=list('intplt',[],1,[],[],[],[],rpar,ipar,'c',[],[%f %t],' ',list())
gr_i=['model=arg1(3);rpar=model(8);ipar=model(9);n=ipar(1);';
'thick=xget(''thickness'');xset(''thickness'',2);';
'xx=rpar(1:n);yy=rpar(n+1:2*n);';
'rect=rpar(2*n+1:2*n+4);';
'mxx=rect(3)-rect(1);';
'mxy=rect(4)-rect(2);';
'xx=orig(1)+sz(1)*(1/10+(4/5)*((xx-rect(1))/mxx));';
'yy=orig(2)+sz(2)*(1/10+(4/5)*((yy-rect(2))/mxy));';
'xpoly(xx,yy,''lines'');';
'xset(''thickness'',thick);']
x=standard_define([2 2],model,[],gr_i)
end
|
4861060e4f452cf8c5551ba482b6054e7c3df4a6 | 8217f7986187902617ad1bf89cb789618a90dd0a | /source/2.5/macros/percent/%r_o_p.sci | cb0195ae8f6100e64e339d1925b66346a722d9c1 | [
"LicenseRef-scancode-public-domain",
"LicenseRef-scancode-warranty-disclaimer"
] | permissive | clg55/Scilab-Workbench | 4ebc01d2daea5026ad07fbfc53e16d4b29179502 | 9f8fd29c7f2a98100fa9aed8b58f6768d24a1875 | refs/heads/master | 2023-05-31T04:06:22.931111 | 2022-09-13T14:41:51 | 2022-09-13T14:41:51 | 258,270,193 | 0 | 1 | null | null | null | null | UTF-8 | Scilab | false | false | 169 | sci | %r_o_p.sci | function r=%r_o_p(l1,l2)
// l1==l2 with l1 rational and l2 polynomial
//!
// Copyright INRIA
r=degree(l1('den'))==0
if r then r=l1('num')./coeff(l1('den'))==l2,end
|
7f9f5f3e0238c2070e2763e7207f4664e1a24a69 | 1bc06fa90b5425d41347c90d0c73bb82eb4cbbfe | /utils/afficherLogs.sci | 7e6a4245396cacad54eb69300a4d80ab0488b3b1 | [] | no_license | madox35/Filtre-Canny | a0a527ad6be5a1dc5984b2533008f95b1c9663ee | 3a54da9b0ce917c995ea5fbd48e0ed5c3f36748d | refs/heads/master | 2020-03-08T08:57:27.702111 | 2018-04-21T19:39:39 | 2018-04-21T19:39:39 | null | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 104 | sci | afficherLogs.sci | function afficherLogs(something)
if AFFICHER_LOGS then
disp(something);
end
endfunction
|
60b149044b8723023573daa751559d895ae51a05 | 06a62d768e69fd9dda11b30011c252807e301813 | /pgm5.sci | dea7c9e85e692a8661ab0dc29db0699befc5f4cf | [] | no_license | vikram-niit/matlab | 36ce3d9539629128251eab060164ce81c03aa690 | da8aeb4d727c47474d37676650664bd028d7e41d | refs/heads/master | 2020-03-18T13:40:37.068765 | 2018-05-25T03:51:55 | 2018-05-25T03:51:55 | 134,800,217 | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 80 | sci | pgm5.sci | function y = pgm5(x)
y = exp(-2 * x) + 3 * sqrt(x);
endfunction
|
817386e2fba1a2a4ffc12a8dc6eace95a67e2abc | 449d555969bfd7befe906877abab098c6e63a0e8 | /62/CH7/EX7.50/ex_7_50.sce | c8dd51bcd6378e3727f99b8a1bcf2055a0fe17a2 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 375 | sce | ex_7_50.sce | clc;
A=[0 1;2 1];
b=[1;-1];
c=[1 -1];
d=[0];
e=spec(A);
if real(e(1))>0 |real(e(2))>0 then
disp("the sytem is not asymptotically stable")
else
disp("the system is asymptotically stable")
end
Hs=ss2tf(syslin('c',A,b,c,d));
disp(Hs,"H(s)=")
disp("there is only one pole and it is located at -1 which is in the LHP hence the system is BIBO stable")
|
21624c48699df89bfd0c719f4943e1da16e8a94e | cb952289471732053d3db787d93f249ea37a7e55 | /6º PERÍODO/Otimizacao/UNIDADE 2/main.sce | 532f3d5aadd373e176b5319b9ea31b70f580320f | [] | no_license | kaikecc/UFRN | 647d09e6beeadfeabfb59f479cd77a5c2ff7bebc | 821cce2e36808e890a75714d71b7cc1a24e52c27 | refs/heads/master | 2022-08-09T19:23:52.552924 | 2022-06-23T21:27:05 | 2022-06-23T21:27:05 | 177,469,993 | 1 | 1 | null | null | null | null | UTF-8 | Scilab | false | false | 840 | sce | main.sce |
clc
clear all
disp("MAXIMIZAÇÃO - [1]");
disp("MINIMIZAÇÃO - [2]");
disp("DETERMINAÇÃO PARA UMA SOLUÇÃO ÓTIMA - [3]");
opc = input("ESCOLHA UMA OPÇÃO: ");
arq = uigetfile("*.txt","C:\Users\kaike\Desktop\UFRN\Otimizacao\UNIDADE 1\Exercicios\","Escolha um arquivo .txt: "); // Funcao para pegar um arquivo
matriz_aumentada = fscanfMat(arq);// pega o arquivo de formato especificado
function metodo = main(matriz_aumentada)
select opc
case 1 then
// [Zo, A, b] = maximizacao(matriz_aumentada);
disp("ENTROU EM MAX");
case 2 then
// [Zo, A, b] = minimizacao(matriz_aumentada);
disp("ENTROU EM MIN");
case 3 then
else
break;
end
metodo = 0;
endfunction
main(matriz_aumentada)
|
3036ca0d276d6c25f493e7b0f8f254649525ac1f | 0896afb25280a9d27c93c0c8e9d07e608426fbea | /scilab_prof/ballon_a_sculpter.sce | a34c071353d946a9b6c7a3c04d292e7fd8f0f8f1 | [] | no_license | netixx/projet_meca | 9a7c932ba4188a1ee6462effd5671e128ccc524f | a1d5794e2eeef61efadd7cbb8d8c477676610eec | refs/heads/master | 2020-12-30T14:56:13.306855 | 2012-12-12T13:51:34 | 2012-12-12T13:51:34 | null | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 2,917 | sce | ballon_a_sculpter.sce | // /////////////////////
// Enveloppe cylindrique
// /////////////////////
// //////////
// Invariants // Question 5
// //////////
function [I1,I2]=Invariants(lambda, mu)
I1 = lambda^2 + mu^2 + 1/(lambda*mu)^2;
I2 = 1/lambda^2 + 1/mu^2 + (lambda*mu)^2;
endfunction
// ///////////
// Contraintes // Question 6
// ///////////
function y = sigtt(Loi, AddI2,lambda, mu)
[I1,I2] = Invariants(lambda, mu);
[dWdI1,dWdI2]=dWdI(Loi, AddI2, I1, I2);
y = (dWdI1 + dWdI2* mu^2)*(lambda^2 - 1./(lambda*mu)^2);
endfunction
function y = sigzz(Loi, AddI2, lambda, mu)
[I1,I2] = Invariants(lambda, mu);
[dWdI1,dWdI2]=dWdI(Loi, AddI2, I1, I2);
y = (dWdI1 + dWdI2* lambda^2)*(mu^2 - 1./(lambda * mu)^2);
endfunction
// //////////////
// Delta pression // Question 7
// //////////////
function y = DeltaPression(Loi, AddI2, Epais, A, lambda, mu)
y = Epais / (mu * lambda^2 ) * sigtt (Loi, AddI2, lambda, mu);
endfunction
// ///////////////////////////
// charge axiale additionnelle // Question 7
// ///////////////////////////
function y = AxialAdd(Loi, AddI2, Epais, A, lambda, mu)
y = pi * A^2 * (2. * Epais / mu * sigzz (Loi, AddI2, lambda, mu) - lambda^2 * DeltaPression(Loi, AddI2, Epais, A, lambda, mu) );
endfunction
// ///////////////////////////////////
// pression normalisee par E/A = Epais
// ///////////////////////////////////
function y = DeltaPressionNorm(Loi, AddI2, Epais, A, lambda, mu)
y = 1. / (mu * lambda^2 ) * sigtt (Loi, AddI2, lambda, mu);
endfunction
// ////////////////////////////////////////////////////////////////
// charge axiale additionnelle normalisee par pi E A = Pi Epais A^2
// ////////////////////////////////////////////////////////////////
function y = AxialAddNorm(Loi, AddI2, Epais, A, lambda, mu)
y = 2. * sigzz (Loi, AddI2, lambda, mu) / mu - lambda^2 * DeltaPressionNorm(Loi, AddI2, Epais, A, lambda, mu) ;
endfunction
//
// //////////////////////////////////////////////////////////////////
// Solve Ballon : Calcul de DP, MU, I1, I2 et Vol=V/V_ini=mu*lambda^2
// //////////////////////////////////////////////////////////////////
function [DP, Mu, Vol, I1, I2]=SolveBallon(lambda, Ta, Epais, A, AddI2)
NomLoi = ['NH', 'Gent', 'Langevin']; NbLoi = size(NomLoi,"c");
DP = zeros(size(lambda,"c"), size(Ta,"c"), NbLoi);
Mu = zeros(size(lambda,"c"), size(Ta,"c"), NbLoi);
Vol = zeros(size(lambda,"c"), size(Ta,"c"), NbLoi);
I1 = zeros(size(lambda,"c"), size(Ta,"c"), NbLoi);
I2 = zeros(size(lambda,"c"), size(Ta,"c"), NbLoi);
for kk=1:NbLoi,
loi =NomLoi(kk);
j = 0;
for Tai=Ta,
j = j+1;
i = 0;
for lambdai=lambda,
i = i+1;
deff('y=fsol(x)','y=AxialAddNorm(loi, AddI2, Epais, A, lambdai, x)-Tai');
mui = fsolve (1,fsol);
DP(i,j,kk) = DeltaPression(loi, AddI2, Epais, A, lambdai, mui);
Mu(i,j,kk) = mui;
Vol(i,j,kk) = mui*lambdai^2;
[I1(i,j,kk),I2(i,j,kk)]=Invariants(lambdai,mui);
end;
end;
end;
endfunction;
|
5c3e29ef2867f17437087bda23eb62b2380f46b7 | 59b742e36fbe9d77cb51ec949c6625f665133d2b | /Resultados/results_LocGlo_16/results/16/l20-2/result2s0.tst | 3bc555d6a31cfa030f255fa589facf86310bcf93 | [] | no_license | Tiburtzio/TFG | 3132fd045de3a0e911e2c9e23e9c46e1075a3274 | 864ce4dd00b7f8fe90eafa65b11d799c5907177e | refs/heads/master | 2023-01-03T12:44:56.269655 | 2020-10-24T18:37:02 | 2020-10-24T18:37:02 | 275,638,403 | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 1,891 | tst | result2s0.tst | @relation unknow
@attribute sp11 integer[0,255]
@attribute sp12 integer[0,255]
@attribute sp13 integer[0,255]
@attribute sp14 integer[0,255]
@attribute sp15 integer[0,255]
@attribute sp16 integer[0,255]
@attribute sp17 integer[0,255]
@attribute sp18 integer[0,255]
@attribute sp19 integer[0,255]
@attribute sp21 integer[0,255]
@attribute sp22 integer[0,255]
@attribute sp23 integer[0,255]
@attribute sp24 integer[0,255]
@attribute sp25 integer[0,255]
@attribute sp26 integer[0,255]
@attribute sp27 integer[0,255]
@attribute sp28 integer[0,255]
@attribute sp29 integer[0,255]
@attribute sp31 integer[0,255]
@attribute sp32 integer[0,255]
@attribute sp33 integer[0,255]
@attribute sp34 integer[0,255]
@attribute sp35 integer[0,255]
@attribute sp36 integer[0,255]
@attribute sp37 integer[0,255]
@attribute sp38 integer[0,255]
@attribute sp39 integer[0,255]
@attribute sp41 integer[0,255]
@attribute sp42 integer[0,255]
@attribute sp43 integer[0,255]
@attribute sp44 integer[0,255]
@attribute sp45 integer[0,255]
@attribute sp46 integer[0,255]
@attribute sp47 integer[0,255]
@attribute sp48 integer[0,255]
@attribute sp49 integer[0,255]
@attribute class{1,2,3,4,5,6,7}
@inputs sp11,sp12,sp13,sp14,sp15,sp16,sp17,sp18,sp19,sp21,sp22,sp23,sp24,sp25,sp26,sp27,sp28,sp29,sp31,sp32,sp33,sp34,sp35,sp36,sp37,sp38,sp39,sp41,sp42,sp43,sp44,sp45,sp46,sp47,sp48,sp49
@outputs class
@data
3 3
3 3
3 3
3 3
4 3
3 3
4 7
2 2
3 3
3 3
3 3
3 3
7 7
7 7
2 5
3 3
3 3
7 7
3 3
7 7
7 7
2 2
7 7
7 2
2 2
5 7
3 3
7 3
7 7
7 7
5 7
3 3
2 2
7 7
2 2
2 2
4 7
4 3
2 2
7 7
7 7
7 7
7 7
4 7
4 3
4 7
5 5
4 7
1 1
7 7
5 5
5 5
5 5
7 7
1 1
1 1
1 1
1 1
7 7
7 7
1 1
7 7
3 3
3 3
1 1
1 1
1 1
7 7
1 1
7 7
7 5
1 1
7 3
1 1
1 1
3 3
3 3
7 3
1 1
2 2
1 1
1 7
1 1
1 1
5 1
2 2
1 1
1 1
3 3
3 3
1 1
1 1
1 7
1 1
5 1
3 3
3 3
3 3
2 5
3 3
4 1
2 2
7 7
2 3
2 2
3 3
7 7
5 5
7 7
5 5
4 3
3 3
7 7
7 7
4 7
1 1
4 7
5 5
3 3
5 7
1 1
1 1
1 1
1 1
1 1
1 5
5 5
5 5
5 5
|
2b7002d29b09610933cbbbaa11893b5c80506900 | 449d555969bfd7befe906877abab098c6e63a0e8 | /2021/CH4/EX4.5/EX4_5.sce | 5660bbd6752272bd453ab6507e5b617c0ea605aa | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 169 | sce | EX4_5.sce | //Finding of Density
//Given
h1=0.4;
h2=0.6;
rho=1000;
rho1=13600;
g=9.81;
wd=rho*0.6;
md=rho1*0.4;
rho2=wd+md;
disp("Density is = "+string(rho2)+" Kg/m^3");
|
499b38f410e110cae5931928b64b5305bfb66671 | 8217f7986187902617ad1bf89cb789618a90dd0a | /source/2.4.1/macros/sci2for/ins2for.sci | 3b721f55b63562596dc1c473eb401e967f77d7fb | [
"LicenseRef-scancode-public-domain",
"LicenseRef-scancode-warranty-disclaimer"
] | permissive | clg55/Scilab-Workbench | 4ebc01d2daea5026ad07fbfc53e16d4b29179502 | 9f8fd29c7f2a98100fa9aed8b58f6768d24a1875 | refs/heads/master | 2023-05-31T04:06:22.931111 | 2022-09-13T14:41:51 | 2022-09-13T14:41:51 | 258,270,193 | 0 | 1 | null | null | null | null | UTF-8 | Scilab | false | false | 424 | sci | ins2for.sci | function [txt,vnms,vtps,nwrk]=ins2for(lst,ilst,vnms,vtps,nwrk)
// traduit un ensemble d'instructions debutant a l'adresse ilst de la
// liste courante lst
//!
// Copyright INRIA
nlst=size(lst)
txt=[]
while ilst<=nlst then
if type(lst(ilst))==15 then
[t1,vnms,vtps,nwrk]=cla2for(lst(ilst),vnms,vtps,nwrk)
ilst=ilst+1
else
[t1,ilst,vnms,vtps,nwrk]=cod2for(lst,ilst,vnms,vtps,nwrk)
end
txt=[txt;t1]
end
|
79eceff2ac6b3eb77cfdcc83f4c3cb38d79e3a7a | f934e15695c77d0a1015c230c5ed65c4f16a2425 | /lpf using wfir.sce | e3b364cf8906688ae2ea29ffe9a05defaa311b59 | [] | no_license | manasdas17/Scilab-for-Signal-Processing- | 6efc5adb507243c7302f7b4f3f12d12060112038 | 5f6e6ce941c0a11212a83674b5d35d97a2cf4396 | refs/heads/master | 2021-01-10T07:49:58.006357 | 2016-04-07T07:45:26 | 2016-04-07T07:45:26 | 55,673,271 | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 198 | sce | lpf using wfir.sce | //By Manas,FOSSEE,IITB
[wft,wfm,fr]=wfir('lp',33,[.23 0],'kr',[5.6 0]);//Linear phase FIR filters
plot2d(fr,20*log10(wfm));//Plots filter response against grid fr
xgrid();
xtitle("LPF using wfir");
|
063581a817daf2108bc78fbb3d632b7e761ab5d0 | 449d555969bfd7befe906877abab098c6e63a0e8 | /1931/CH11/EX11.5/5.sce | 81b83e1dfed665b8f113b1ed8c689a5df1284e5e | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 1,056 | sce | 5.sce | clc
clear
//INPUT DATA
ni=1.5*10^16//intrinsic charge carriers in m^-3
r1=10*10^-2//resistivity of p-type silicon in ohm m
r2=10*10^-2//resistivity of n-type silicon in ohm m
me=1350*10^-4//The mobility of the charge carrier in m^2 V^-1 s^-1
mh=480*10^-4//The hole charge carrier in m^2 V^-1 s^-1
e=1.6*10^-19//charge of electron in coulombs
//CALCULATION
Na=(1/(r1*e*mh))/10^21//The density of the intrinsic crystal for p-type in m^-3*10^21
ne=((ni^2)/(Na*10^21))/10^11//The minor carrier concentration for p-type in electrons/m^3*10^11
Nd=(1/(r2*e*me))/10^20//The density of the intrinsic crystal for n-type in m^-3*10^20
nh=((ni^2)/(Nd*10^20))/10^11//The minor carrier concentration for n-type in electrons/m^3*10^11
//OUTPUT
printf('The density of the intrinsic crystal for p-type is %3.4f*10^21 m^-3 \n The minor carrier concentration for p-type is %3.3f*10^11 electrons/m^3 \n The density of the intrinsic crystal for n-type is %3.3f*10^20 m^-3 \n The minor carrier concentration for n-type is %3.4f*10^11 holes/m^3',Na,ne,Nd,nh)
|
8524ecb1322e1888332518ac1905565c4fc4ec96 | b12941be3faf1fd1024c2c0437aa3a4ddcbbfd67 | /normal2/pretest.tst | 4ea72f3c3e8e5a4afd59874f9d8cc61dd3ca0b1b | [] | no_license | JanWielemaker/optica | 950bd860825ab753236ce1daa399ee7a0b31b3ee | 3a378df314b5a60926b325089edac89c00cc8c6d | refs/heads/master | 2020-06-12T14:22:46.567191 | 2019-06-21T11:24:41 | 2019-06-21T11:24:41 | 194,328,239 | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 13,360 | tst | pretest.tst | /* Questionaire created by optica toolkit
Date: Tue Mar 24 16:23:20 1998
*/
question(1, 'pre1.11',
'Wanneer komt het snijpunt van de uittredende lichtstraal met de hoofdas verder van de lens te liggen?',
[ 'Als je de hoek die de invallende straal met de hoofdas maakt vergroot.',
'Als je de lamp een stukje naar rechts beweegt.',
'Als je de lens een stukje naar rechts beweegt.'
],
state(state, '',
[ m6 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(3),
sfere_left(10),
sfere_right(10),
breaking_index(1.51),
pos_x(7),
show_gauge(false),
instrument_name(lens)),
l2 = lamp1(switch(true),
angle(10),
pos_y(0),
pos_x(0),
instrument_name(lamp1))
])).
question(2, 'pre1.12',
'Wanneer komt het snijpunt van de uittredende lichtstraal met de hoofdas dichter bij de lens te liggen?',
[ 'Als je de hoek die de invallende lichtstraal met de hoofdas maakt verkleint.',
'Als je de lamp een stukje naar links beweegt.',
'Als je de lens vervangt door een platbolle lens.'
],
state(state, '',
[ m6 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(3),
sfere_left(10),
sfere_right(10),
breaking_index(1.51),
pos_x(10),
show_gauge(false),
instrument_name(lens)),
l2 = lamp1(switch(true),
angle(10),
pos_y(0),
pos_x(2),
instrument_name(lamp1))
])).
question(3, 'pre1.13',
'Wanneer zal de uittredende lichtstraal meer naar boven schijnen?',
[ 'Als je de hoek die de invallende lichtstraal met de hoofdas maakt verkleint.',
'Als je de lens meer naar links beweegt.',
'Als je de lens vervangt door een dubbelbolle lens.'
],
state(state, '',
[ m1 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(6),
sfere_left(0),
sfere_right(10),
breaking_index(1.51),
pos_x(5),
show_gauge(false),
instrument_name(lens)),
l1 = lamp1(switch(true),
angle(10),
pos_y(0),
pos_x(2),
instrument_name(lamp1))
])).
question(4, 'pre1.14',
'De uittredende lichtstraal loopt evenwijdig met de hoofdas.
Wanneer zal de uittredende lichtstraal meer naar boven schijnen?',
[ 'Als je de hoek die de invallende lichtstraal met de hoofdas maakt vergroot.',
'Als je de lens naar rechts beweegt.',
'Als je de lens vervangt door een platbolle lens.'
],
state(state, '',
[ m6 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(3),
sfere_left(10),
sfere_right(10),
breaking_index(1.51),
pos_x(5),
show_gauge(false),
instrument_name(lens)),
l2 = lamp1(switch(true),
angle(10),
pos_y(0),
pos_x(2),
instrument_name(lamp1))
])).
question(5, 'pre1.15',
'De uittredende lichtstraal loopt evenwijdig met de hoofdas.
Wanneer zal de uittredende lichtstraal meer naar beneden schijnen?',
[ 'Als je de hoek die de invallende lichtstraal met de hoofdas maakt verkleint',
'Als je de lens een stukje naar rechts beweegt.',
'Als je de lens vervangt door een holle lens.'
],
state(state, '',
[ m6 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(3),
sfere_left(10),
sfere_right(10),
breaking_index(1.51),
pos_x(5),
show_gauge(false),
instrument_name(lens)),
l2 = lamp1(switch(true),
angle(10),
pos_y(0),
pos_x(2),
instrument_name(lamp1))
])).
question(6, 'pre2.11',
'Wanneer komt het snijpunt van de uittredende lichtstralen dichter bij de lens te liggen?',
[ 'Als je de invallende lichtstralen meer naar beneden richt.',
'Als je de lamp een stukje naar rechts beweegt.',
'Als je de lens vervangt door een lens met een kleinere brandpuntsafstand.'
],
state(state, '',
[ m1 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(6),
sfere_left(0),
sfere_right(0),
breaking_index(1.51),
pos_x(7),
show_gauge(false),
instrument_name(lens)),
l2 = parlamp(switch(true),
angle(0),
separation(1),
pos_x(2),
pos_y(0),
instrument_name(parlamp))
])).
question(7, 'pre2.12',
'Wanneer komt het snijpunt van de uittredende lichtstralen verder van de lens af te liggen?',
[ 'Als je de invallende lichtstralen iets naar boven richt.',
'Als je de lamp een stukje naar links beweegt.',
'Als je de lens vervangt door een lens met een grotere brandpuntsafstand.'
],
state(state, '',
[ m1 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(3),
sfere_left(0),
sfere_right(0),
breaking_index(1.51),
pos_x(10),
show_gauge(false),
instrument_name(lens)),
l2 = parlamp(switch(true),
angle(0),
separation(1),
pos_x(2),
pos_y(0),
instrument_name(parlamp))
])).
question(8, 'pre2.13',
'Wanneer komt het snijpunt van de uittredende lichtstralen boven de hoofdas te liggen?',
[ 'Als je de invallende lichtstralen meer naar boven richt.',
'Als je de lamp een stukje naar beneden beweegt.',
'Als je de lens een stukje naar rechts beweegt.'
],
state(state, '',
[ m1 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(3),
sfere_left(0),
sfere_right(0),
breaking_index(1.51),
pos_x(10),
show_gauge(false),
instrument_name(lens)),
l2 = parlamp(switch(true),
angle(0),
separation(1),
pos_x(2),
pos_y(0),
instrument_name(parlamp))
])).
question(9, 'pre2.14',
'Wanneer komt het snijpunt van de uittredende lichtstralen onder de hoofdas te liggen?',
[ 'Als je de stralen van de invallende lichtstralen naar beneden richt.',
'Als je de lamp een stukje naar boven beweegt.',
'Als je de lens een stukje naar links beweegt.'
],
state(state, '',
[ m1 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(6),
sfere_left(0),
sfere_right(0),
breaking_index(1.51),
pos_x(7),
show_gauge(false),
instrument_name(lens)),
l2 = parlamp(switch(true),
angle(0),
separation(1),
pos_x(2),
pos_y(0),
instrument_name(parlamp))
])).
question(10, 'pre3.21',
'Wanneer komt het snijpunt van de uittredende lichtstralen boven de hoofdas te liggen?',
[ 'Als je de invallende lichtstralen naar boven richt.',
'Als je de lamp een stukje naar beneden beweegt.',
'Als je de lens een stukje naar rechts beweegt.'
],
state(state, '',
[ m1 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(3),
sfere_left(0),
sfere_right(0),
breaking_index(1.51),
pos_x(20),
show_gauge(true),
instrument_name(lens)),
l1 = lamp3(switch(true),
angle(0),
divergence(5),
pos_x(3),
pos_y(0),
instrument_name(lamp3))
])).
question(11, 'pre3.22',
'Wanneer komt het snijpunt van de uittredende lichtstralen onder de hoofdas te liggen?',
[ 'Als je de invallende lichtstralen naar boven richt.',
'Als je de lamp een stukje naar boven beweegt.',
'Als je de lens een stukje naar links beweegt.'
],
state(state, '',
[ m1 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(6),
sfere_left(0),
sfere_right(0),
breaking_index(1.51),
pos_x(16),
show_gauge(true),
instrument_name(lens)),
l4 = lamp3(switch(true),
angle(0),
divergence(5),
pos_x(2),
pos_y(0),
instrument_name(lamp3))
])).
question(12, 'pre3.23',
'Wanneer komt het virtueel beeldpunt onder de hoofdas te liggen?',
[ 'Als je de invallende lichtstralen meer naar beneden richt.',
'Als je lamp een stukje naar boven beweegt.',
'Als je de lamp een stukje naar beneden beweegt.'
],
state(state, '',
[ m1 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(-6),
sfere_left(0),
sfere_right(0),
breaking_index(1.51),
pos_x(16),
show_gauge(true),
instrument_name(lens)),
l5 = lamp3(switch(true),
angle(0),
divergence(5),
pos_x(4),
pos_y(0),
instrument_name(lamp3))
])).
question(13, 'pre3.24',
'De lamp wordt 2 cm boven de hoofdas geplaatst.
Hoever komt het beeldpunt van de hoofdas te liggen?',
[ '2 cm',
'4 cm',
'8 cm'
],
state(state, '',
[ m1 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(3),
sfere_left(0),
sfere_right(0),
breaking_index(1.51),
pos_x(9),
show_gauge(true),
instrument_name(lens)),
l1 = lamp3(switch(true),
angle(0),
divergence(5),
pos_x(3),
pos_y(0),
instrument_name(lamp3)),
d2 = ruler(from(centerline), to(m1), offset(-2))
])).
question(14, 'pre3.25',
'De lamp wordt 2 cm boven de hoofdas geplaatst.
Hoever komt het beeldpunt van de hoofdas te liggen?',
[ '2 cm',
'3 cm',
'4 cm'
],
state(state, '',
[ m1 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(3),
sfere_left(0),
sfere_right(0),
breaking_index(1.51),
pos_x(7.5),
show_gauge(true),
instrument_name(lens)),
l1 = lamp3(switch(true),
angle(0),
divergence(5),
pos_x(3),
pos_y(0),
instrument_name(lamp3)),
d1 = ruler(from(centerline),
to(m1),
offset(-2.4))
])).
question(15, 'pre3.26',
'De lamp wordt 4 cm boven de hoofdas geplaatst.
Hoever komt het virtueel beeldpunt van de hoofdas te liggen?',
[ '1 cm.',
'2 cm.',
'4 cm.'
],
state(state, '',
[ m1 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(-6),
sfere_left(0),
sfere_right(0),
breaking_index(1.51),
pos_x(10),
show_gauge(true),
instrument_name(lens)),
l5 = lamp3(switch(true),
angle(0),
divergence(5),
pos_x(4),
pos_y(0),
instrument_name(lamp3)),
d8 = ruler(from(centerline),
to(m1),
offset(-2.1))
])).
question(16, 'pre3.27',
'Een lamp met een divergerende lichtbundel wordt geplaatst op de afgebeelde hulplijn.
Wat wordt dan de beeldsafstand?',
[ '4,5 cm.',
'6 cm.',
'9 cm.'
],
state(state, '',
[ m1 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(6),
sfere_left(0),
sfere_right(0),
breaking_index(1.51),
pos_x(18.65),
show_gauge(true),
instrument_name(lens)),
c3 = construction_line(orientation(vertical),
value(0.65),
instrument_name(consline)),
d6 = ruler(from(c3), to(m1), offset(3.6))
])).
question(17, 'pre3.28',
'Een lamp met een divergerende lichtbundel wordt geplaatst op de afgebeelde hulplijn.
Wat wordt dan de beeldsafstand?',
[ '2,25 cm.',
'4,5 cm.',
'12 cm.'
],
state(state, '',
[ m1 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(3),
sfere_left(0),
sfere_right(0),
breaking_index(1.51),
pos_x(10.85),
show_gauge(true),
instrument_name(lens)),
c2 = construction_line(orientation(vertical),
value(1.85),
instrument_name(consline)),
d2 = ruler(from(c2), to(m1), offset(3))
])).
question(18, 'pre3.29',
'Een lamp met een divergerende bundel wordt geplaatst op de afgebeelde hulplijn.
Wat wordt dan de beeldsafstand?',
[ '9 cm.',
'-3 cm.',
'-6 cm.'
],
state(state, '',
[ m1 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(6),
sfere_left(0),
sfere_right(0),
breaking_index(1.51),
pos_x(13.75),
show_gauge(true),
instrument_name(lens)),
c4 = construction_line(orientation(vertical),
value(10.75),
instrument_name(consline)),
d7 = ruler(from(c4), to(m1), offset(3.2))
])).
question(19, 'pre3.30',
'Een lamp met een divergerende lichtbundel wordt geplaatst op de afgebeelde hulplijn.
Wat wordt dan de beeldsafstand?',
[ '-4,5 cm.',
'-6 cm.',
'12 cm.'
],
state(state, '',
[ m1 = lens(label(''),
radius(5),
thickness(0.1),
focal_distance(-6),
sfere_left(0),
sfere_right(0),
breaking_index(1.51),
pos_x(22.05),
show_gauge(true),
instrument_name(lens)),
c5 = construction_line(orientation(vertical),
value(4.05),
instrument_name(consline)),
d1 = ruler(from(c5), to(m1), offset(2.85))
])).
|
5c0716f7af875e32d7bb1be86b47a252eef1d72d | 38012281b6334f56780d83d57af821a009c37ebe | /out/20_02_2019/Final_LrFijo_Repeticiones/Barcelona_TEST_3.tst | 0f7e0a8b6c25800d65c214943735726d82d29449 | [] | no_license | uo232368/TripAdvisor | 2140422daa42fbae57b2eeb17d8829ff2378a822 | 74fa0131da52162d2f0bbcf6ceff91caa47ae220 | refs/heads/master | 2020-03-29T09:23:12.984191 | 2019-04-24T09:26:40 | 2019-04-24T09:26:40 | 149,755,513 | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 3,161 | tst | Barcelona_TEST_3.tst | Using TensorFlow backend.
[94mObteniendo datos...[0m
[93m[AVISO] Usuarios: 33537[0m
[93m[AVISO] Restaurantes: 5881[0m
[93m[AVISO] Cargando datos generados previamente...[0m
[94mCreando modelo...[0m
##################################################
MODELV4
##################################################
modelv4d2
##################################################
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/usr/lib/python3/dist-packages/xlsxwriter/worksheet.py:833: DeprecationWarning: invalid escape sequence \w
if re.match('\w:', url) or re.match(r'\\', url):
/usr/lib/python3/dist-packages/xlsxwriter/worksheet.py:962: DeprecationWarning: invalid escape sequence \s
if re.search('^\s', token) or re.search('\s$', token):
/usr/lib/python3/dist-packages/xlsxwriter/worksheet.py:962: DeprecationWarning: invalid escape sequence \s
if re.search('^\s', token) or re.search('\s$', token):
/usr/lib/python3/dist-packages/xlsxwriter/worksheet.py:3610: DeprecationWarning: invalid escape sequence \|
elif re.match('(or|\|\|)', conditional):
/usr/lib/python3/dist-packages/xlsxwriter/worksheet.py:3840: DeprecationWarning: invalid escape sequence \.
name = re.sub('\..*$', '', name)
/usr/lib/python3/dist-packages/xlsxwriter/worksheet.py:5136: DeprecationWarning: invalid escape sequence \s
if re.search('^\s', string) or re.search('\s$', string):
/usr/lib/python3/dist-packages/xlsxwriter/worksheet.py:5136: DeprecationWarning: invalid escape sequence \s
if re.search('^\s', string) or re.search('\s$', string):
/usr/lib/python3/dist-packages/xlsxwriter/sharedstrings.py:103: DeprecationWarning: invalid escape sequence \s
if re.search('^\s', string) or re.search('\s$', string):
/usr/lib/python3/dist-packages/xlsxwriter/sharedstrings.py:103: DeprecationWarning: invalid escape sequence \s
if re.search('^\s', string) or re.search('\s$', string):
/usr/lib/python3/dist-packages/xlsxwriter/comments.py:160: DeprecationWarning: invalid escape sequence \s
if re.search('^\s', text) or re.search('\s$', text):
/usr/lib/python3/dist-packages/xlsxwriter/comments.py:160: DeprecationWarning: invalid escape sequence \s
if re.search('^\s', text) or re.search('\s$', text):
----------------------------------------------------------------------------------------------------
N_FOTOS_TRAIN (>=) N_ITEMS %ITEMS RND-MOD AC CNT-MOD AC MODELO
9 1987 0.22846958721398183 0.10230984578418019 0.2385226560771158 0.16153024985961978
5 3522 0.4049672300793377 0.09442727273830982 0.21646069359661552 0.18546804169907952
4 4881 0.561228009658503 0.0890243310348925 0.20124543661136085 0.19463313742005212
2 6982 0.8028055651374038 0.08792472026371356 0.19823361684304652 0.21051694367396673
1 8697 1.0 0.08328745296547176 0.19270345670093156 0.22721703661762813
----------------------------------------------------------------------------------------------------
50 0.0308 14.2589 0.2965 0.2272
|
381b46a87208f653fb924f43c0f512ac72810674 | 0e1b45c07f0938ba9c8a003d6ae1cf2d8315efdb | /templates/idea/test-01.tst | 235ac46c1994d2de1ab1de87c415a19c91258007 | [] | no_license | Kot-Angens/acm | c85d8582c3e84f218415321743864b9680e01f2e | 05472eaa0fff7abb6679826085da5e0c990df4cb | refs/heads/master | 2021-01-24T22:36:05.159612 | 2012-10-02T13:51:56 | 2012-10-02T13:51:56 | null | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 48 | tst | test-01.tst | ...given
~~~~~~~~~~~~~~~~~~~~~~~~~~
...expected
|
e348674fbb9aa55ac58610caec6c5c5de7d4043f | 449d555969bfd7befe906877abab098c6e63a0e8 | /2741/CH10/EX10.7/ExampleA7.sce | 0e46a8f5cbbd6f722daca55751c6bfd3a035ace3 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 591 | sce | ExampleA7.sce | clc
clear
//Page number 472
//Input data
d=9000;//The density of copper in kg/m^3
w=63.5;//The atomic weight of copper in kg
N=6.023*10^26;//Avogadros number
pi=3.14;//Mathematical constant of pi
h=6.624*10^-34;//Planks constant in Js
//Calculations
V=w/d;//The volume of copper in m^3
Ef=((h^2/(8*9*10^-31))*((3/pi)*(N/V))^(2/3))/(1.6*10^-19);//The fermi energy in eV
P=(2/3)*(N/V)*Ef;//The pressure at absolute zero for copper in N/m^2
//Output
printf('(a)The Fermi energy is E = %3.3f eV \n (b)The pressure at absolute zero for copper is P = %3.6g N/m^2 ',Ef,P)
|
6862595b8331c6a3a9fa0255c42d4e00815172fb | 449d555969bfd7befe906877abab098c6e63a0e8 | /2489/CH5/EX5.2/5_2.sce | 884c400f6a01d67fd3e93dc816efecc6288716c8 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 344 | sce | 5_2.sce | clc
//Intitalisation of variables
clear
p= 27.17 //mm
T= 99.5 //C
T1= 100.5 //C
T2= 100 //C
sv1= 1674 //cc per gram
sv2= 1.04 //cc per gram
g= 980.7 //cm/sec^2
d= 13.595 //kg/m^3
//CALCULATIONS
r= (p/10)*d*g
lv= (273.2+T2)*(sv1-sv2)*(p/10)*d*g/(4.184*10^7)
//RESULTS
printf ('Heat of vapourisation of water = %.1f cal g^-1',lv)
|
be7c7a334b0fc7dbf4301e9147f6d3ce17de18c0 | 449d555969bfd7befe906877abab098c6e63a0e8 | /1373/CH12/EX12.11/Chapter12_Example11.sce | 8ecdff01b84ec85ef6313a7d099cd721f91de41a | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 1,918 | sce | Chapter12_Example11.sce | //Chapter-12, Example 12.11, Page 518
//=============================================================================
clc
clear
//INPUT DATA
mc=4;//Mass flow rate of cold water in kg/s
Tci=38;//Inlet Temperature of cold water in degree C
Tco=55;//Outlet Temperature of cold water in degree C
D=0.02;//Diameter of the tube in m
v=0.35;//Velocity of water in m/s
Thi=95;//Inlet Temperature of hot water in degree C
mh=2;//Mass flow rate of hot water in kg/s
L=2;//Length of the tube in m
U=1500;//Overall heat transfer coefficient in W/m^2.K
c=4186;//Specific heat of water in J/kg.K
d=1000;//Density of water in kg/m^3
//CALCULATIONS
Q=(mc*c*(Tco-Tci));//Heat transfer rate for cold fluid in W
Tho=(Thi-(Q/(mh*c)));//Outlet temperature of hot fluid in degree C
T=Thi-Tco;//Difference of temperature between hot water inlet and cold water outlet in degree C
t=Tho-Tci;//Difference of temperature between hot water outlet and cold water inlet in degree C
Tlm=((T-t)/log(T/t));//LMTD for counterflow heat exchanger
A=(Q/(U*Tlm));//Area of heat exchanger in m^2
A1=(mc/(d*v));//Total flow area in m^2
n=((A1*4)/(3.14*D^2));//Number of tubes
L=(A/(36*3.14*D));//Length of each tube taking n=36 in m
N=2;//Since this length is greater than the permitted length of 2m, we must use more than one tube pass. Let us try 2 tube passes
P=((Tco-Tci)/(Thi-Tci));//P value for calculation of correction factor
R=((Thi-Tho)/(Tco-Tci));//R value for calculation of correction factor
F=0.9;//Corrction Factor from Fig.12.9 on page no. 514
A2=(Q/(U*F*Tlm));//Total area required for one shall pass,2 tube pass exchanger in m^2
L1=(A2/(2*36*3.14*D));//Length of tube per pass taking n=36 in m
//OUTPUT
mprintf('Number of tubes per pass is %i \n Number of passes is %i \n Length of tube per pass is %3.3f m',n,N,L1)
//=================================END OF PROGRAM==============================
|
16501614b921c8264f89a427559755ad4f5302e6 | 449d555969bfd7befe906877abab098c6e63a0e8 | /1106/CH8/EX8.8/ex8_8.sce | df417770a36e7a19022537b346ec12f0baf76934 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 433 | sce | ex8_8.sce | // Example 8.8, Page No-380
clear
clc
Vref=7.15
Vo=5
k=Vref/Vo
printf('(R1b+R2)/R2= %.2f', k)
k1=k-1
printf('\nR1 = %.2f * R2', k1)
// For min voltage of 2V
Vom=2
km=Vref/Vom
printf('\n(R1a+R1b+R2)/R2= %.3f', km)
km1=km-1.43
printf('\nR1a = %.3f * R2', km1)
R1a=10000
R1b=2000
R2=R1a/2.145
R2n=R2/1000
printf('\nR2= %.2f kohm', R2n)
R1=6000
R3=(R1*R2)/(R1+R2)
R3n=R3/1000
printf('\nR3= %.2f kohm', R3n)
|
d7ef3a77a9482f81ddb2c65ac009f80af98db068 | 449d555969bfd7befe906877abab098c6e63a0e8 | /2087/CH5/EX5.1/example5_1.sce | ac6693a716cdccf844b03c06c3f19bed6d79d1c4 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 440 | sce | example5_1.sce |
//example 5.1
//design an open wellin fine sand
clc;
//given
Q=0.003; //required discharge
H=2.5; //depression head
A=Q*3600/(0.5*H);
d=(4*A/%pi)^0.5;
d=round(d*100)/100
mprintf("Well diameter=%f m.",d);
//Alternative solution
C=7.5D-5; //permeability constant from table 5.2
A=Q/(C*H);
d=(16*3/%pi)^0.5;
d=round(d*10)/10;
mprintf("\nBy alternative solution:")
mprintf("\nWell diameter=%f m",d);
|
7b95c82a10557edf16963e5ac340fcc791e2b7ec | 089894a36ef33cb3d0f697541716c9b6cd8dcc43 | /NLP_Project/test/blog/bow/bow.14_17.tst | e91c288f7c3933612c8c444747a3b7d4f91072b9 | [] | no_license | mandar15/NLP_Project | 3142cda82d49ba0ea30b580c46bdd0e0348fe3ec | 1dcb70a199a0f7ab8c72825bfd5b8146e75b7ec2 | refs/heads/master | 2020-05-20T13:36:05.842840 | 2013-07-31T06:53:59 | 2013-07-31T06:53:59 | 6,534,406 | 0 | 1 | null | null | null | null | UTF-8 | Scilab | false | false | 6,028 | tst | bow.14_17.tst | 14 1:0.046511627906976744 3:0.6666666666666666 8:0.3333333333333333 20:0.5 33:0.2 44:0.25 55:0.25 63:2.0 91:0.16666666666666666 102:1.0 162:1.0 166:1.0 199:0.5 203:0.5 293:0.16666666666666666 318:1.0 388:0.5 575:1.0 622:0.2 634:1.0 753:1.0 1157:1.0
14 1:0.023255813953488372 3:0.3333333333333333 15:0.2 17:0.05 55:0.25 63:1.0 68:1.0 71:1.0 270:0.5 317:1.0 333:1.0 732:1.0 755:1.0 1765:1.0
14 5:0.25 8:0.6666666666666666 11:0.09090909090909091 15:0.2 33:0.4 55:0.25 63:1.0 83:0.5 199:0.5 289:1.0 290:1.0 311:1.0 313:0.5 350:1.0 351:1.0 388:0.5 423:1.0 634:1.0 732:1.0 753:1.0 773:1.0 866:1.0 980:0.5
14 23:0.3333333333333333 673:1.0
14 1:0.06976744186046512 3:0.6666666666666666 5:0.25 8:0.6666666666666666 9:1.0 11:0.18181818181818182 13:0.6666666666666666 15:1.0 17:0.05 20:0.5 23:0.3333333333333333 32:0.8 33:0.2 35:2.0 36:1.0 55:0.5 91:0.5 165:1.0 169:1.0 176:1.0 250:1.0 307:2.0 312:1.0 313:0.5 398:1.0 431:0.3333333333333333 484:1.0 489:1.0 527:1.0 576:1.0 618:1.0 627:1.0 681:1.0 757:1.0 819:0.3333333333333333 896:1.0 918:1.0 930:1.0 1139:2.0 1143:1.0 1157:1.0 1498:1.0
14 1:0.023255813953488372 3:0.3333333333333333 37:0.14285714285714285 56:1.0 166:1.0 204:0.5 779:1.0 819:0.3333333333333333
14 1:0.023255813953488372 3:0.3333333333333333 8:0.3333333333333333 11:0.18181818181818182 17:0.1 20:1.5 55:0.25 63:2.0 84:0.5 91:0.16666666666666666 118:1.0 203:1.5 204:0.5 212:1.0 228:1.0 234:0.6666666666666666 307:2.0 313:0.5 340:1.0 350:2.0 383:1.0 388:0.5 421:1.0 440:1.0 492:0.5 556:1.0 634:1.0 673:1.0 700:2.0 801:1.0 865:1.0 990:1.0 1791:1.0
14 17:0.05 58:1.0 204:0.5 234:0.3333333333333333 319:1.0 386:1.0
14 778:1.0
14 5:0.25 33:0.4 55:0.25 63:1.0 303:0.125 470:1.0 673:1.0
14 1:0.046511627906976744 5:0.25 8:0.3333333333333333 11:0.09090909090909091 33:0.2 176:1.0 351:1.0 380:1.0 558:1.0 1299:1.0
14 1:0.023255813953488372 5:0.25 8:1.0 11:0.18181818181818182 15:0.6 17:0.1 36:1.0 84:0.5 93:1.0 162:1.0 318:1.0 522:1.0 587:1.0 765:1.0 815:1.0 1001:0.5 1562:1.0
14 1:0.023255813953488372 11:0.09090909090909091 15:0.2 19:1.0 63:1.0 75:1.0 282:1.0 365:1.0 743:1.0 893:1.0
14 5:0.25 15:0.2 20:0.5 204:0.5 340:1.0 484:1.0 919:1.0
14 1:0.023255813953488372 8:0.3333333333333333 9:1.0 11:0.2727272727272727 15:0.6 17:0.1 19:1.0 20:1.0 33:0.4 37:0.14285714285714285 83:0.5 91:0.16666666666666666 119:1.0 135:1.0 140:1.0 293:0.16666666666666666 294:1.0 307:1.0 318:1.0 333:1.0 340:1.0 425:1.0 516:2.0 530:1.0 541:0.5 575:1.0 980:0.5 1056:1.0 1434:1.0
14 1:0.023255813953488372 8:1.0 11:0.09090909090909091 17:0.1 20:1.5 73:1.0 91:0.16666666666666666 204:0.5 294:1.0 350:2.0 390:1.0 440:1.0 442:2.0 751:1.0 773:1.0 855:1.0 991:1.0 1093:0.5 1176:1.0 1738:1.0
14 3:0.3333333333333333 5:0.25 17:0.2 62:1.0 73:1.0 203:0.5 258:1.0 307:1.0 319:1.0 333:1.0 335:1.0 359:1.0 383:2.0 424:1.0 444:0.5 487:1.0 860:1.0
14 8:0.3333333333333333 15:0.4 17:0.05 18:1.0 93:1.0 159:0.25 294:1.0 333:1.0 383:3.0 401:0.3333333333333333 515:1.0 566:1.0 614:0.3333333333333333 712:1.0 713:1.0 737:1.0 1252:1.0 1323:1.0
14 5:0.25 8:0.3333333333333333 17:0.05 24:2.0 62:1.0 135:1.0 203:1.0 359:1.0 860:1.0 882:1.0
14 1:0.13953488372093023 4:0.3333333333333333 8:1.0 11:0.18181818181818182 13:0.3333333333333333 15:0.8 17:0.15 33:0.2 36:2.0 44:0.25 63:1.0 64:0.2 76:1.0 87:1.0 91:0.5 100:1.0 102:1.0 123:1.0 162:1.0 187:0.2 257:1.0 258:1.0 284:1.0 378:1.0 383:1.0 464:1.0 558:2.0 604:0.5 612:1.0 660:1.0 711:1.0 753:1.0 994:1.0 1235:1.0 1261:1.0 1329:1.0 1570:1.0
14 15:0.4 17:0.05 33:0.4 36:1.0 83:0.5 135:1.0 277:1.0 430:1.0 471:1.0 484:1.0
14 1:0.023255813953488372 15:0.2 32:0.2 33:0.2 73:1.0 91:0.16666666666666666 161:1.0 227:0.2 368:1.0 509:1.0 1093:0.5 1157:1.0
14 55:0.25 84:0.5 199:0.5 234:0.3333333333333333 840:1.0
14 1:0.046511627906976744 3:0.3333333333333333 36:1.0 37:0.14285714285714285 55:0.25 91:0.16666666666666666 94:1.0 199:0.5 350:1.0 392:1.0 470:1.0 558:1.0 872:1.0
14 1:0.09302325581395349 3:0.3333333333333333 5:0.25 11:0.09090909090909091 15:0.2 32:0.2 40:0.1111111111111111 63:1.0 71:1.0 91:0.16666666666666666 166:1.0 173:1.0 212:1.0 227:0.2 284:1.0 307:1.0 401:0.3333333333333333 425:1.0 755:1.0 892:1.0
14 1:0.046511627906976744 3:0.6666666666666666 5:0.25 17:0.05 37:0.14285714285714285 558:1.0 673:1.0 1654:1.0 1793:1.0
14 1:0.023255813953488372 4:0.3333333333333333 8:0.3333333333333333 15:0.2 33:0.2 55:0.5 73:1.0 162:1.0 388:0.5 518:1.0 678:1.0 819:0.3333333333333333 1498:1.0
14 1:0.046511627906976744 5:0.25 11:0.09090909090909091 15:0.4 33:0.4 37:0.2857142857142857 63:1.0 83:0.5 260:1.0 263:1.0 297:1.0 369:1.0 471:1.0 484:1.0 700:1.0 892:1.0 980:0.5 1060:1.0 1157:1.0
14 15:0.2 203:0.5 396:1.0 501:1.0 978:1.0 1157:1.0 1721:1.0
14 1:0.023255813953488372 91:0.16666666666666666 234:0.3333333333333333 254:1.0 492:0.5
14 4:0.3333333333333333 8:0.6666666666666666 11:0.09090909090909091 17:0.05 19:1.0 20:0.5 33:0.4 84:0.5 91:0.3333333333333333 189:1.0 204:0.5 254:1.0 390:1.0 669:1.0 860:1.0 1255:1.0 1289:1.0 1535:1.0
14 1:0.023255813953488372 8:0.6666666666666666 11:0.18181818181818182 15:0.2 17:0.05 33:0.2 87:1.0 91:0.3333333333333333 203:0.5 204:0.5 254:1.0 1144:1.0 1757:1.0
14 8:0.3333333333333333 15:0.2 17:0.1 254:1.0 1665:1.0 1811:1.0
14 1:0.023255813953488372 15:0.2 37:0.14285714285714285
14 1:0.046511627906976744 8:0.3333333333333333 11:0.09090909090909091 15:0.2 20:0.5 33:0.2 40:0.1111111111111111 91:0.16666666666666666 93:1.0 135:1.0 173:1.0 190:0.5 254:1.0 282:1.0 284:1.0 637:1.0
14 1:0.046511627906976744 11:0.18181818181818182 17:0.05 20:0.5 91:0.16666666666666666 165:1.0 431:0.3333333333333333 826:1.0 1410:1.0 1482:1.0
14 1:0.046511627906976744 8:0.3333333333333333 11:0.09090909090909091 17:0.1 40:0.1111111111111111 67:1.0 70:0.2 76:1.0 91:0.16666666666666666 119:1.0 227:0.2 254:2.0 418:0.5 627:1.0 1032:1.0 1204:1.0
14 1:0.023255813953488372 3:0.3333333333333333 162:1.0 379:1.0
14 1:0.023255813953488372 2:1.0 3:0.6666666666666666 8:0.6666666666666666 9:1.0 11:0.09090909090909091 20:0.5 56:1.0 73:1.0 91:0.3333333333333333 135:1.0 161:1.0 204:0.5 253:0.5 383:1.0 734:1.0 1560:1.0
|
56167c01ac644fade043cd6fd4684cc0dbbd1b8b | 8217f7986187902617ad1bf89cb789618a90dd0a | /browsable_source/2.4.1/Unix-Windows/scilab-2.4.1/macros/m2sci/sci_diag.sci | 6df4e71d51076a11154fac8f010a4fb0fb15cf4d | [
"LicenseRef-scancode-public-domain",
"LicenseRef-scancode-warranty-disclaimer"
] | permissive | clg55/Scilab-Workbench | 4ebc01d2daea5026ad07fbfc53e16d4b29179502 | 9f8fd29c7f2a98100fa9aed8b58f6768d24a1875 | refs/heads/master | 2023-05-31T04:06:22.931111 | 2022-09-13T14:41:51 | 2022-09-13T14:41:51 | 258,270,193 | 0 | 1 | null | null | null | null | UTF-8 | Scilab | false | false | 441 | sci | sci_diag.sci | function [stk,txt,top]=sci_diag()
// Copyright INRIA
txt=[]
if rhs==2 then
stk=list('diag('+stk(top-1)(1)+','+stk(top)(1)'+')','0','?','?','1')
top=top-1
else
if stk(top)(3)=='1' then
stk=list('diag('+stk(top)(1)+')','0',stk(top)(4),stk(top)(4),'1')
elseif stk(top)(4)=='1' then
stk=list('diag('+stk(top)(1)+')','0',stk(top)(3),stk(top)(3),'1')
else
stk=list('diag('+stk(top)(1)+')','0','?','?','1')
end
end
|
3a803854787acbca3151d23cb6ae241b360c6776 | 449d555969bfd7befe906877abab098c6e63a0e8 | /3845/CH12/EX12.2/Ex12_2.sce | 188a322d27bd699243ea41bf99463e4e8e2a7d46 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 579 | sce | Ex12_2.sce | //Example 12.2
r1=0.9*10^-2;//Radius of garden hose (m)
A1=%pi*r1^2;//Cross-sectional area of hose (m^2)
Q=0.5;//Flow rate (L/s)
Q=Q/10^3;//Flow rate (m^3/s)
v1=Q/A1;//Speed of water in the hose (m/s)
printf('a.Speed of water in the hose = %0.2f m/s',v1)
r2=0.25*10^-2;//Radius of nozzle (m)
A2=%pi*r2^2;//Cross-sectional area of nozzle (m^2)
v2=A1*v1/A2;//Speed of water in the nozzle from continuity equation (m/s)
printf('\nb.Speed of water in the nozzle = %0.1f m/s',v2)
//Openstax - College Physics
//Download for free at http://cnx.org/content/col11406/latest
|
836878ac87146dd2c6d10e8733626425dd670737 | 66106821c3fd692db68c20ab2934f0ce400c0890 | /test/disassembler/ldd.instr.tst | 1f809b42beb8201239c77b1f4470cf1a565e1e48 | [] | no_license | aurelf/avrora | 491023f63005b5b61e0a0d088b2f07e152f3a154 | c270f2598c4a340981ac4a53e7bd6813e6384546 | refs/heads/master | 2021-01-19T05:39:01.927906 | 2008-01-27T22:03:56 | 2008-01-27T22:03:56 | 4,779,104 | 2 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 2,669 | tst | ldd.instr.tst | ; @Harness: disassembler
; @Result: PASS
section .text size=0x00000068 vma=0x00000000 lma=0x00000000 offset=0x00000034 ;2**0
section .data size=0x00000000 vma=0x00000000 lma=0x00000000 offset=0x0000009c ;2**0
start .text:
label 0x00000000 ".text":
0x0: 0x0f 0x8c ldd r0, Y+31 ; 0x1f
0x2: 0x1f 0x8c ldd r1, Y+31 ; 0x1f
0x4: 0x2f 0x8c ldd r2, Y+31 ; 0x1f
0x6: 0x3f 0x8c ldd r3, Y+31 ; 0x1f
0x8: 0x4f 0x8c ldd r4, Y+31 ; 0x1f
0xa: 0x5f 0x8c ldd r5, Y+31 ; 0x1f
0xc: 0x6f 0x8c ldd r6, Y+31 ; 0x1f
0xe: 0x7f 0x8c ldd r7, Y+31 ; 0x1f
0x10: 0x8f 0x8c ldd r8, Y+31 ; 0x1f
0x12: 0x9f 0x8c ldd r9, Y+31 ; 0x1f
0x14: 0xaf 0x8c ldd r10, Y+31 ; 0x1f
0x16: 0xbf 0x8c ldd r11, Y+31 ; 0x1f
0x18: 0xcf 0x8c ldd r12, Y+31 ; 0x1f
0x1a: 0xdf 0x8c ldd r13, Y+31 ; 0x1f
0x1c: 0xef 0x8c ldd r14, Y+31 ; 0x1f
0x1e: 0xff 0x8c ldd r15, Y+31 ; 0x1f
0x20: 0x0f 0x8d ldd r16, Y+31 ; 0x1f
0x22: 0x1f 0x8d ldd r17, Y+31 ; 0x1f
0x24: 0x2f 0x8d ldd r18, Y+31 ; 0x1f
0x26: 0x3f 0x8d ldd r19, Y+31 ; 0x1f
0x28: 0x4f 0x8d ldd r20, Y+31 ; 0x1f
0x2a: 0x5f 0x8d ldd r21, Y+31 ; 0x1f
0x2c: 0x6f 0x8d ldd r22, Y+31 ; 0x1f
0x2e: 0x7f 0x8d ldd r23, Y+31 ; 0x1f
0x30: 0x8f 0x8d ldd r24, Y+31 ; 0x1f
0x32: 0x9f 0x8d ldd r25, Y+31 ; 0x1f
0x34: 0xaf 0x8d ldd r26, Y+31 ; 0x1f
0x36: 0xbf 0x8d ldd r27, Y+31 ; 0x1f
0x38: 0xcf 0x8d ldd r28, Y+31 ; 0x1f
0x3a: 0xdf 0x8d ldd r29, Y+31 ; 0x1f
0x3c: 0xef 0x8d ldd r30, Y+31 ; 0x1f
0x3e: 0xff 0x8d ldd r31, Y+31 ; 0x1f
0x40: 0x0f 0x8c ldd r0, Y+31 ; 0x1f
0x42: 0x07 0x8c ldd r0, Z+31 ; 0x1f
0x44: 0x0f 0xac ldd r0, Y+63 ; 0x3f
0x46: 0x08 0x80 ld r0, Y
0x48: 0x0f 0x8c ldd r0, Y+31 ; 0x1f
0x4a: 0x0f 0x84 ldd r0, Y+15 ; 0x0f
0x4c: 0x0f 0x80 ldd r0, Y+7 ; 0x07
0x4e: 0x0b 0x80 ldd r0, Y+3 ; 0x03
0x50: 0x09 0x80 ldd r0, Y+1 ; 0x01
0x52: 0x0c 0xac ldd r0, Y+60 ; 0x3c
0x54: 0x0e 0x8c ldd r0, Y+30 ; 0x1e
0x56: 0x0b 0xa8 ldd r0, Y+51 ; 0x33
0x58: 0x09 0x8c ldd r0, Y+25 ; 0x19
0x5a: 0x0c 0x84 ldd r0, Y+12 ; 0x0c
0x5c: 0x0e 0x80 ldd r0, Y+6 ; 0x06
0x5e: 0x0a 0xa4 ldd r0, Y+42 ; 0x2a
0x60: 0x0d 0x88 ldd r0, Y+21 ; 0x15
0x62: 0x0a 0x84 ldd r0, Y+10 ; 0x0a
0x64: 0x0d 0x80 ldd r0, Y+5 ; 0x05
0x66: 0x0a 0x80 ldd r0, Y+2 ; 0x02
start .data:
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841149c78ef14a463f18dac12b65d944f541a50a | 449d555969bfd7befe906877abab098c6e63a0e8 | /1619/CH2/EX2.2.8/Example2_2_8.sce | 44ac40e4f45361849792a1b4da27e523ea949a8d | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 454 | sce | Example2_2_8.sce | //Example 2.2.8 page 2.15
clc;
clear;
Tf = 1400; //fictive temperature
BETA = 7*10^-11;
n= 1.46; //RI
p= 0.286; //photo elastic constant
Kb = 1.381*10^-23; //Boltzmann's constant
lamda = 850*10^-9; //wavelength
alpha_scat = 8*%pi^3*n^8*p^2*Kb*Tf*BETA/(3*lamda^4);
l= 1000; //fibre length
TL = exp(-alpha_scat*l); //transmission loss
attenuation = 10*log10(1/TL);
printf("The attenuation is %.3f dB/Km",attenuation);
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d8f9e5ccccb3913dbdfc0c71b0666c3a0b53b3ff | 449d555969bfd7befe906877abab098c6e63a0e8 | /2783/CH8/EX8.11/Ex8_11.sce | 3e634e24c0ac936cd7e2e779cbff7b4611afaeb2 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 229 | sce | Ex8_11.sce | clc
//initialization of new variables
clear
u=20 //km/h
Cd=0.15
S=4 //m^2
r=1025 //kg/m^3
//calculations
D=Cd*1/2*r*(u/3.6)^2*(S)
P=D*u/3.6
//results
printf('Drag force = %d N',D)
printf('\n Power = %.2f KW',P/1000)
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de38c09a6b6ef2121fa27a755cd38efc2e616645 | 449d555969bfd7befe906877abab098c6e63a0e8 | /3875/CH1/EX1.6/Ex1_6.sce | f22eb016173544a078a2f2ceb8ccb8ea6510b082 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 603 | sce | Ex1_6.sce | clc;
clear;
R=50 //resistance in ohm
C=25 //capacitance in micro-F
L=0.15 //inductance in H
V=230 //voltage in Volts
f=50 //frequency in Hz
//calculation
XL=2*%pi*f*L //in ohm
XC=(10^6)/(2*%pi*f*C) //in ohm
X=XL-XC //in ohm
Z=sqrt(R^2+X^2)
I=V/Z
pf=R/Z
power_consumed=V*I*pf
mprintf("(i)Impedance = %2.1f ohm\n",Z) //The answers vary due to round off error
mprintf("(ii)Current = %1.2f A\n",I) //The answers vary due to round off error
mprintf("(iii)Power Factor = %1.2f (Lead)\n",pf)
mprintf("(iv)Power Consumed = %d W",power_consumed) //The answers vary due to round off error
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d5730fb17829fbed33faee47f47df554a438d633 | 449d555969bfd7befe906877abab098c6e63a0e8 | /1445/CH6/EX6.4/Ex6_4.sce | 98bc14ab645fee30c1c96ad7b81e6aefd1fbccd3 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 1,359 | sce | Ex6_4.sce | //CHAPTER 6- MAGNETIC CIRCUITS
//Example 4
clc;
disp("CHAPTER 6");
disp("EXAMPLE 4");
//VARIABLE INITIALIZATION
di=10; //diameter of iron ring in cm
dr=1.5; //diameter of iron rod in cm
mui=900; //relative permeability of rod
mu0=4*%pi*10^(-7); //absolute permeability in Henry/m
lg=5/10; //length of air-gap in cm
N=400; //number of turns
I=3.4; //current through the winding in Amperes
//SOLUTION
li=(di*%pi)-lg; //length of iron path
area=((dr^2)*%pi)/4; //area of iron cross-section
//solution (a)
mmf=(4*%pi*N*I)/10; //in gilberts, since 1 AT=(4*pi)/10
mmf=round(mmf); //to round off the value
disp(sprintf("(a) MMF is %d Gilberts",mmf));
//solution (b)
//tot reluctance = iron reluctance + air gap reluctance(mur=1 for air)
totR=(li/(area*mu0*mui))+(lg/(area*mu0*1));
disp(sprintf("(b) The total reluctance is %E Gilberts/Maxwell",totR));
//solution (c)
phi=mmf/totR;
disp(sprintf("(c) The flux in the circuit is %f Maxwell",phi));
//solution (d)
b=phi/area;
disp(sprintf("(d) The flux density in the circuit is %f Gauss",b));
//Answers of (b), (c) & (d) are different because absolute permeability is not included in (b)
//END
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01a4b3fe3e338941550df518c48cff5728b2e95d | 089894a36ef33cb3d0f697541716c9b6cd8dcc43 | /NLP_Project/test/tweet/bow/bow.9_11.tst | 4675e105b36bcaea061c555433fdbe611f6b1c54 | [] | no_license | mandar15/NLP_Project | 3142cda82d49ba0ea30b580c46bdd0e0348fe3ec | 1dcb70a199a0f7ab8c72825bfd5b8146e75b7ec2 | refs/heads/master | 2020-05-20T13:36:05.842840 | 2013-07-31T06:53:59 | 2013-07-31T06:53:59 | 6,534,406 | 0 | 1 | null | null | null | null | UTF-8 | Scilab | false | false | 43,910 | tst | bow.9_11.tst | 9 5:0.18181818181818182 24:1.0 26:1.0 28:0.5 29:0.16666666666666666 31:0.1111111111111111 37:0.125 47:0.5 53:2.0 57:0.25 59:1.0 60:2.0 63:0.5 81:0.6666666666666666 115:1.0 130:0.5 132:1.0 154:0.1 160:0.5 170:2.0 175:0.05263157894736842 189:0.3333333333333333 199:1.0 206:1.0 216:0.6666666666666666 229:2.0 233:1.0 273:0.14285714285714285 306:0.3333333333333333 321:1.0 367:0.09090909090909091 421:0.5 459:1.0 485:1.0 496:0.5 534:0.3333333333333333 535:1.0 544:0.3333333333333333 580:1.0 626:2.0 672:1.0 767:1.0 804:1.0 856:1.0 869:1.0 962:1.0 998:1.0 1031:1.0 1498:0.5 1548:1.0 1585:1.0 1586:1.0 1907:1.0 1977:1.0 2871:0.5 3156:1.0 3948:1.0 4100:1.0 4105:1.0 4647:1.0 5062:1.0 5067:0.3333333333333333 6286:1.0
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0.569277 0.148062
0.251984 0.055688
-0.113951 0.012650
0.742789 0.110866
-0.014617 0.000214
-0.594152 0.147768
-0.518732 0.143755
0.685407 0.132070
0.275105 0.064661
-0.320924 0.082870
0.654100 0.140060
0.117614 0.013453
0.563375 0.147890
-0.621497 0.145495
-0.651451 0.140612
-0.859291 0.050538
0.211985 0.040990
0.102092 0.010207
-0.899258 0.029605
-0.182306 0.031063
-0.501076 0.140826
-0.648037 0.141295
-0.654111 0.140057
-0.562162 0.147843
-0.753899 0.105892
-0.073546 0.005351
0.799309 0.083310
-0.915118 0.022130
-0.305032 0.076536
-0.078897 0.006148
-0.250004 0.054933
0.023452 0.000549
0.297032 0.073346
0.680171 0.133592
-0.787823 0.089310
-0.405170 0.114688
0.444413 0.127192
-0.508355 0.142117
-0.338018 0.089639
0.060343 0.003615
0.194074 0.034881
-0.391096 0.109743
0.022941 0.000526
-0.952376 0.007841
0.046709 0.002172
-0.785731 0.090385
0.617860 0.145917
0.905489 0.026591
0.244021 0.052666
-0.612017 0.146518
-0.572340 0.148115
0.381054 0.106096
-0.668694 0.136668
-0.211116 0.040686
0.032299 0.001041
0.423023 0.120634
0.729971 0.116281
-0.095075 0.008877
0.777914 0.094347
-0.474517 0.135183
-0.085741 0.007244
0.056530 0.003175
0.925432 0.017654
0.017172 0.000295
-0.577745 0.148148
0.027944 0.000780
-0.590060 0.147931
0.598993 0.147516
0.088206 0.007660
-0.809306 0.077969
-0.077244 0.005896
-0.527312 0.144924
0.535411 0.145869
-0.497124 0.140077
0.398030 0.112205
0.266273 0.061204
-0.579040 0.148144
0.623018 0.145308
0.971033 0.003074
0.234222 0.049006
0.450459 0.128921
0.976874 0.001995
0.681453 0.133226
-0.890987 0.033735
-0.065861 0.004300
-0.624817 0.145078
-0.167079 0.026379
-0.915943 0.021759
-0.500406 0.140701
-0.376577 0.104442
-0.839969 0.061172
0.613032 0.146421
-0.642562 0.142323
-0.044319 0.001957
-0.876643 0.041185
-0.360852 0.098511
-0.560785 0.147786
-0.404404 0.114424
0.424036 0.120959
-0.430025 0.122853
0.067764 0.004550
0.150374 0.021601
-0.215379 0.042184
-0.892144 0.033149
0.362450 0.099121
-0.865373 0.047228
0.831443 0.065879
-0.905624 0.026527
0.630433 0.144301
-0.077770 0.005975
-0.826946 0.068355
0.005260 0.000028
0.329770 0.086382
-0.154040 0.022616
0.501498 0.140904
0.045135 0.002029
0.769562 0.098475
-0.657540 0.139313
-0.879051 0.039912
-0.753943 0.105872
-0.223342 0.045030
-0.974323 0.002440
-0.762766 0.101748
-0.265677 0.060972
-0.439554 0.125761
-0.077226 0.005893
0.825198 0.069315
0.300651 0.074789
0.917142 0.021225
0.522509 0.144290
-0.580339 0.148136
0.573762 0.148131
0.233826 0.048860
-0.077056 0.005867
-0.830543 0.066375
0.337610 0.089478
0.330432 0.086644
-0.322456 0.083479
-0.535286 0.145855
0.125917 0.015356
0.454498 0.130042
0.855738 0.052483
0.302767 0.075632
-0.201444 0.037353
0.261146 0.059213
0.381045 0.106093
-0.912413 0.023357
0.118394 0.013627
-0.766156 0.100125
-0.820919 0.071661
-0.551397 0.147265
0.767199 0.099622
-0.782766 0.091898
0.920212 0.019877
0.267573 0.061710
0.921317 0.019399
0.219161 0.043528
0.239197 0.050855
-0.438524 0.125454
0.394626 0.111003
0.573390 0.148127
-0.376022 0.104236
0.720520 0.120036
0.860288 0.049994
-0.274633 0.064475
0.789299 0.088549
0.338029 0.089643
0.626132 0.144904
-0.881023 0.038876
0.366010 0.100475
0.668335 0.136758
0.503223 0.141218
0.517191 0.143527
-0.756583 0.104653
-0.407491 0.115483
-0.539674 0.146302
0.013548 0.000183
-0.549662 0.147144
0.637273 0.143236
-0.795973 0.085069
-0.223167 0.044966
-0.665072 0.137564
-0.643337 0.142183
-0.340948 0.090790
0.919511 0.020182
-0.425341 0.121376
-0.512043 0.142726
-0.942443 0.011102
-0.138018 0.018330
-0.325527 0.084699
0.564613 0.147933
0.081654 0.006579
0.800303 0.082784
-0.526541 0.144826
-0.627544 0.144712
0.031873 0.001014
-0.171699 0.027768
0.562680 0.147864
0.829134 0.067151
-0.307875 0.077669
0.737018 0.113349
0.142435 0.019473
0.011117 0.000124
0.128406 0.015949
0.532188 0.145511
-0.110473 0.011908
0.989264 0.000446
0.068224 0.004611
-0.277132 0.065458
-0.728589 0.116843
0.172376 0.027974
0.162560 0.025048
0.046844 0.002185
-0.665491 0.137463
-0.347669 0.093419
-0.201319 0.037311
0.868242 0.045677
0.546055 0.146869
0.387511 0.108452
0.452670 0.129538
-0.337562 0.089459
-0.984408 0.000928
0.104808 0.010745
0.033145 0.001096
0.302661 0.075590
-0.818031 0.073238
-0.620394 0.145627
-0.223093 0.044940
-0.378853 0.105285
0.927936 0.016621
-0.097128 0.009257
0.364432 0.099876
0.859230 0.050571
-0.665394 0.137486
0.435878 0.124655
0.440148 0.125938
-0.331777 0.087176
0.913021 0.023080
0.730680 0.115991
0.891742 0.033352
0.465155 0.132867
-0.487803 0.138183
0.076968 0.005854
0.711146 0.123552
0.134612 0.017470
-0.229305 0.047197
-0.861699 0.049225
0.031031 0.000961
-0.176597 0.029272
0.246143 0.053467
-0.283776 0.068081
-0.808925 0.078174
0.136590 0.017967
|
121a3e0b15997564448c65011024dbf8c8839076 | e9d5f5cf984c905c31f197577d633705e835780a | /GED/linear/scilab/P2_multi_GE/ged_P2_sim_multi_GE.sce | 2e7db33d7625f4dd18dee166e35247f228ca9abd | [] | no_license | faiz-hub/dr-ged-benchmarks | 1ad57a69ed90fe7595c006efdc262d703e22d6c0 | 98b250db9e9f09d42b3413551ce7a346dd99400c | refs/heads/master | 2021-05-18T23:12:18.631904 | 2020-03-30T21:12:16 | 2020-03-30T21:12:16 | null | 0 | 0 | null | null | null | null | UTF-8 | Scilab | false | false | 5,194 | sce | ged_P2_sim_multi_GE.sce | // Data Reconciliation Benchmark Problems From Lietrature Review
// Author: Edson Cordeiro do Valle
// Contact - edsoncv@{gmail.com}{vrtech.com.br}
// Skype: edson.cv
// Authors
//Dovì, V G, and C Solisio. 2001. Reconciliation of censored measurements in chemical processes: an alternative approach. Chemical Engineering Journal 84, no. 3 (December): 309-314. http://www.sciencedirect.com/science/article/B6TFJ-45KNHB1-F/2/199f358469628f600f10b394d2b55a8b.
//Bibtex Citation
//@article{Dovi2001,
//annote = { The importance of considering the censoring of measured data in the reconciliation of process flow rates has been shown in a previous paper [Chem. Eng. Sci. 52 (17) (1997) 3047]. The purpose of the present paper is to introduce a new technique for carrying out the actual reconciliation procedure and compare its significance and performance with those of previous methods. A numerical example shows how nontrivial differences are to be expected.},
//author = {Dov\`{\i}, V G and Solisio, C},
//isbn = {1385-8947},
//journal = {Chemical Engineering Journal},
//keywords = {Censored data,Data reconciliation,Detection limits},
//month = dec,
//number = {3},
//pages = {309--314},
//title = {{Reconciliation of censored measurements in chemical processes: an alternative approach}},
//url = {http://www.sciencedirect.com/science/article/B6TFJ-45KNHB1-F/2/199f358469628f600f10b394d2b55a8b},
//volume = {84},
//year = {2001}
//}
// 6 Streams
// 3 Equipments
getd('../functions/');
getd('../jacobians/');
clear xr sd sds x_sol xfinal jac jac_col jac_col rj sigma sigam_inv res V V_inv diag_diag_V Wbar gama zr_nt adj zadj Wbar_alt adjustability detect resi Qglr betaglr xchiglr ge_glr op_glr;
clear avti_gt_mt op_gt_mt op_gt_nt_tmp avt1_mt1 avt1_mt2 op_mt1 op_mt2 avti_glr op_glr_mt aee_mt aee_nt_tmp op_glr_nt_tmp avti_glr_nt_tmp avti_gt_mt_tmp op_gt_mt_tmp op_gt_nt avt1_nt1 avt1_nt2 op_nt1 op_nt2 avti_glr_tmp op_glr_mt_tmp aee_mt_tmp aee_nt op_glr_nt avti_glr_nt;
//stacksize('max');
tic;
xr =[11;10;21;11;5.5;5.5];
szx = size(xr,1);
runsize = 1000;
//the variance proposed by this work
sd =[0.032
0.026
0.120
0.033
0.052
0.015].^(0.5);
sds = sd;
var=sd.^2;
jac=jacP2();
rj=rank(jac);
jac_col = size(jac,2);
jac_row = size(jac,1);
sigma=diag(sds.^2);
[adj, detect, V, V_inv, sigma_inv, diag_diag_V, Wbar] = adjust(sigma, jac);
bias_min = 2;
bias_max = 7;
leak_min = 0.02;
leak_max = 0.07;
bias_multi_error = [0 0 1 1 0 0 ];
leak_multi_error = [ 0 1 1];
sum_bias_and_leak = 0;
[xfinal, resRand, resGrossErrorNodalRand]=generate_data(xr, sd, jac, runsize, bias_min, bias_max, leak_min, leak_max);
[xfinal2, resRand2, resGrossErrorNodalRand2]=generate_data_multiple(xfinal(1:runsize,:), sd, jac, 2, 10, 0.5, 0.9,bias_multi_error,leak_multi_error, sum_bias_and_leak);
xfinal = xfinal2;
resGrossErrorNodalRandFi2 = [ resRand2;resGrossErrorNodalRand2];
//observability/redundancy tests
//user can set unmeasured streams here, if this vector is empty, all streams are measured
umeas_P2 = [];
[red_P2, just_measured_P2, observ_P2, non_obs_P2, spec_cand_P2] = qrlinclass(jac,umeas_P2);
measured_P2 = setdiff([1:length(xr)], umeas_P2);
red = measured_P2;//
// to run robust reconciliation,, one must choose between the folowing objective functions to set up the functions path and function parameters:
//WLS analytical = -1 WLS numerical = 0 ; Absolute sum of squares = 1 ; Cauchy = 2 ;Contamined Normal = 3 ; Fair = 4
//Hampel = 5 Logistic = 6 ; Lorenztian = 7 ; Quasi Weighted = 8
// run the configuration functions with the desired objective function type
obj_function_type = -1;
[x_sol] = calc_results_DR(xfinal2, jac, sigma, resGrossErrorNodalRandFi2, obj_function_type);
[res, gamaMeasuremts,gamaNodal,zr_nt_nodal, zr_nt_nodal_rand, zadj ] = calc_results_index(x_sol, jac, sigma, resGrossErrorNodalRandFi);
// user must implemment the multiple gross error routines bellow with (or without the indexes above calculated)
// global test for multi GE
[avti_gt_mt, op_gt_mt, op_gt_nt] = global_test_multi(0.1, 0.1, gamaMeasuremts, runsize, rj, jac_col, jac_row);
runtime=toc();
//streamNames =generateStreamName(szx);
//prettyprinttable([tokens(streamNames), string([xr, rrn(4,sd), rrn(3,adj), rrn(3,detect), rrn(3,op_mt1), rrn(3,op_mt2), rrn(3,op_glr_mt), rrn(7,aee_mt)])],"latex")
//eqpNames = generateEqpName('', jac_row);
//prettyprinttable([tokens(eqpNames), string([rrn(3,op_nt1), rrn(3,op_nt2), rrn(3,op_glr_nt), rrn(7,aee_nt)])],"latex")
//[ op_gt_mt avti_gt_mt avt1_mt1 avt1_mt2 avti_glr avt1_nt1 avt1_nt2 avti_glr_nt runtime ]
//prettyprinttable(string([rrn(3,avt1_mt1), rrn(3,avt1_mt2), rrn(3,avti_glr), rrn(3,avt1_nt1), rrn(3,avt1_nt2), rrn(7,avti_glr_nt)]))
//[rrn(3,op_mt1), rrn(3,op_mt2), rrn(3,op_glr_mt), rrn(7,aee_mt)]
//[rrn(3,op_nt1), rrn(3,op_nt2), rrn(3,op_glr_nt), rrn(7,aee_nt)]
//
////saving results
//aa = clock();
//nowtime = '_' + string(aa(4)) + '-'+ string(aa(5));
//save ('P_resumed_' + date() + nowtime +'.sav', runtime, adj, detect, op_nt1, op_nt2, avt1_nt1, avt1_nt2, op_mt1, op_mt2, avt1_mt1, avt1_mt2, op_gt_mt, op_gt_nt, avti_gt_mt, op_glr_mt, op_glr_nt, avti_glr, avti_glr_nt, aee_nt, aee_mt);
//
|
30c368d59c5c2ad0fd9fd5712ab976e1d5169232 | 449d555969bfd7befe906877abab098c6e63a0e8 | /2333/CH3/EX3.8/8.sce | 03eadd65f408632dc1f3bf7c1dc8071aa2d2be07 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 593 | sce | 8.sce | clc
// Given that
lambda = 6000 // wavelength of light in angstrom
e = 0.3 // Width of slit in mm
m = 1 // Order for first dark band
n = 3/2 // Order for first bright band
// Sample Problem 8 on page no. 143
printf("\n # PROBLEM 8 # \n")
printf(" Standard formula used \n")
printf(" lambda = e*sin(theta) \n")
theta_d = m*asin(lambda*1e-10/(e*1e-3)) // Calculation of angle in radian
theta_b = n*asin(lambda*1e-10/(e*1e-3)) // Calculation of angle in radian
printf("\n First dark band is formed at angle %e rad. \n First bright band is formed at angle %e rad.",theta_d,theta_b)
|
00f78fdb6f1646723afed61a598a01afc5fbfae8 | 449d555969bfd7befe906877abab098c6e63a0e8 | /1172/CH3/EX3.15/Example3_15.sce | 0f4573ed34002aeb23a9798a3b873a439b6fdee2 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 545 | sce | Example3_15.sce | clc
//Given that
m = 2e-3 // mass of linear harmonic oscillator in kg
k = 100 // spring constant in N/m
h = 6.6e-34 // Plank's constant
//Sample Problem 15 page No. 142
printf("\n\n\n # Problem 15 # \n")
printf("\n Standard formula Used \n f = sqrt(k / m ) \n U = 1/2* h * nu ")
nu = sqrt(k / m ) / (2 * %pi) //calculation of frequency of linear harmonic oscillator
U = 1/2* h * nu //calculation of Zero point energy of a linear harmonic oscillator
printf ("\n Zero point energy of a linear harmonic oscillator is %e J.", U )
|
0bed22e91ab5574975352a7ec929df4ede1836d0 | 449d555969bfd7befe906877abab098c6e63a0e8 | /1511/CH1/EX1.11/ex1_11.sce | 903ee1903fa423d0692beaebe54bdd496031199f | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 420 | sce | ex1_11.sce | // Example 1.11 page no-33
clear
clc
l=2 //cm
D=18 //cm
s=0.5 //cm
//(a)
va1=500 //volts
ds1=l*D/(2*s*va1)//Deflection Sensitivity
//(b)
va2=1000 //Volts
ds2=l*D/(2*s*va2)
//(c)
va3=1500 //Volts
ds3=l*D/(2*s*va3)
printf("\n(a)Va=%dV\nDeflection Sensitivity S_E=%.3f cm/V \n\n(b)Va=%dV\nDeflection Sensitivity S_E=%.3f cm/V\n\n(c)Va=%dV\nDeflection Sensitivity S_E=%.3f cm/V",va1,ds1,va2,ds2,va3,ds3)
|
e9cc2c08d00a09c2fda1d59e80e9842b401e9ab2 | 12d276a808c8403c4dd3b13dea1edb8720127311 | /one-back_end.sce | 13d5fdda06a809a64d6ee3d0209d5f5cdf54ca0d | [] | no_license | npytabitha/VOT3 | 85b317ae4c120eb2bda125b28c1ad27243d40eab | 51032662c4a6f0960393aad4ebf9b3289c641155 | refs/heads/develop | 2021-01-10T05:44:31.715364 | 2015-10-01T13:34:47 | 2015-10-01T13:34:47 | 43,233,510 | 0 | 1 | null | 2015-10-02T09:05:14 | 2015-09-27T03:56:10 | Scilab | UTF-8 | Scilab | false | false | 705 | sce | one-back_end.sce | scenario = "One-Back"; # This name is recorded in the log file
scenario_type = trials;
response_matching = simple_matching;
no_logfile = true;
active_buttons = 3;
button_codes = 1, 2, 3; # These values will be used to code participant responses
default_font_size = 56;
default_font = "Arial";
default_background_color = 0,0,0; #Black#
default_text_color = 255,255,255; #White#
begin;
#Thank you screen at end of experiment
trial{
trial_duration=forever;
trial_type=specific_response;
terminator_button = 3;
picture{
text{font_size = 20; caption = "Ende des Experiments
Vielen Dank!";
};
x = 0; y = 0;
};
time = 0;
}thankyou;
begin_pcl;
thankyou.present();
output_file rating = new output_file; |
106c17d7141e859690363fcb4cb99c9fab92890f | 449d555969bfd7befe906877abab098c6e63a0e8 | /1682/CH8/EX8.10/Exa8_10.sce | a1bbed274d21b100534789fb49a2474e1b34fdd6 | [] | no_license | FOSSEE/Scilab-TBC-Uploads | 948e5d1126d46bdd2f89a44c54ba62b0f0a1f5e1 | 7bc77cb1ed33745c720952c92b3b2747c5cbf2df | refs/heads/master | 2020-04-09T02:43:26.499817 | 2018-02-03T05:31:52 | 2018-02-03T05:31:52 | 37,975,407 | 3 | 12 | null | null | null | null | UTF-8 | Scilab | false | false | 1,623 | sce | Exa8_10.sce | //Exa 8.10
clc;
clear;
close;
//Given data :
p1=(100-96)/100;//unitless
p2=(96-89)/100;//unitless
p3=(89-68)/100;//unitless
p4=(68-37)/100;//unitless
p5=(37-13)/100;//unitless
p6=(13-0)/100;//unitless
N0=1000;//no. of resistors
N1=N0*p1;//no. of resistors
N2=N0*p2+N1*p1;//no. of resistors
N3=N0*p3+N1*p2+N2*p1;//no. of resistors
N4=N0*p4+N1*p3+N2*p2+N3*p1;//no. of resistors
N5=N0*p5+N1*p4+N2*p3+N3*p2+N4*p1;//no. of resistors
N6=N0*p6+N1*p5+N2*p4+N3*p3+N4*p2+N5*p1 ;//no. of resistors
//Calculation of individual replacement cost
Life=0;//in months
p=[p1 p2 p3 p4 p5 p6];//Unitless
for i=1:6
Life=Life+i*p(i);
end
disp(Life,"Expected life of each transistor in months : ")
disp(round(1000/Life),"Average No. of failures/month : ");
disp(round(1000/Life)*10,"Therefore, cost of individual replacement in Rs. : ")
//Calculation of group replacement cost
disp("Cost/transistor when replaced simultaneously = Rs. 4");
disp("Cost/transistor when replaced individually = Rs. 10");
disp("The cost of group replacement policy for several replacement periods are summarized in Table 8.7. This table can be seen from the book.");
disp("From table it is clear that the avg cost/month is minimum for the 3rd month. Hence, the group replacement period is 3 months.");
disp("Individual replacement cost/month = Rs. 2480");
disp("Minimum group replacement ost/month = Rs. 2426.67");
disp("Since the min group replacement cost/month is less than the individual replacement cost/month, the group replacement policy is the best, and hence all the transistors should be replaced in 3 months.") |
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