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// Scilab Code Ex11.1: Page-249 (2010) h = 6.626e-034; // Planck's constant, Js c = 3e+08; // Speed of light in free space, m/s k = 1.38e-023; // Boltzmann constant, J/K T = 300; // Temperature at absolute scale, K lambda = 5500e-010; // Wavelength of visible light, m rate_ratio = exp(h*c/(lambda*k*T))-1; // Ratio of spontaneous emission to stimulated emission printf("\nThe ratio of spontaneous emission to stimulated emission for visible region = %1.0e", rate_ratio); lambda = 1e-02; // Wavelength of microwave, m rate_ratio = exp(h*c/(lambda*k*T))-1; // Ratio of spontaneous emission to stimulated emission printf("\nThe ratio of spontaneous emission to stimulated emission for microwave region = %6.4f", rate_ratio); // Result // The ratio of spontaneous emission to stimulated emission for visible region = 8e+037 // The ratio of spontaneous emission to stimulated emission for microwave region = 0.0048
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errcatch(-1,"stop");mode(2);; ; format('v',6); R=0,G=0,a=0,Ro=70,B=3,f=100*10^6; w=2*%pi*f; C=B/(w*Ro); disp(C*10^12,'Capacitance per meter of line in pF') L=Ro*Ro*C; disp(L*10^9,'Inductance per meter in nHz') exit();
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//Ex:2.14 clc; clear; close; V2=50;// in micro volt G=5;// voltage gain in dB G1=10^(G/20);// voltage gain V1=V2*G1;// signal at receiving station in volt printf("The signal at receiving station = %f micro volts", V1);
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// Grob's Basic Electronics 11e // Chapter No. 13 // Example No. 13_3 clc; clear; // With a flux of 400 uWb through an area of 0.0005 sqm, what is the flux density B in tesla units? // Given data A = 0.0005; // Area=0.0005 sqm flux = 400*10^-6; // Total Flux=400 uWb B = flux/A; disp (B,'The Flux Density in Tesla (T)')
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//example 14.4 clc; clear; v1 = input('Enter the value of V1 in volts :'); //part a : v1 =0 ; part b : v1 =5v if (v1==0) then // checking for V1 disp('V2 = 5 V'); disp('I = 0 mA'); else disp('V2 = 0 V'); disp('I = 0.5 mA '); end
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// Copyright (C) 2012 - Prateek Papriwal // // This file must be used under the terms of the CeCILL. // This source file is licensed as described in the file COPYING, which // you should have received as part of this distribution. The terms // are also available at // http://www.cecill.info/licences/Licence_CeCILL_V2-en.txt function [M,V] = distfun_poissstat(lambda) // Poisson mean and variance // // Calling Sequence // M = distfun_poissstat(lambda) // [M,V] = distfun_poissstat(lambda) // // Parameters // lambda : a 1x1 or nxm matrix of doubles, the average rate of occurrence // M : a matrix of doubles, the mean // V : a matrix of doubles, the variance // // Description // Computes statistics from the Poisson distribution. // // Any scalar input argument is expanded to a matrix of // doubles of the same size as the other input arguments. // // The Mean and Variance of the Poisson Distribution are // //<latex> //\begin{eqnarray} // M &=& lambda \\ // V &=& lambda //\end{eqnarray} //</latex> // // Examples // // Test with expanded lambda //[m,v] = distfun_poissstat((1:6)) //me = [ 1 2 3 4 5 6 ]; //ve = [ 1 2 3 4 5 6 ]; // // //Accuracy test //lambda = [ 11 22 33 ]; //[M,V] = distfun_poissstat ( lambda ) //ve = [ 11 22 33 ]; //me = [ 11 22 33 ]; // // Bibliography // http://en.wikipedia.org/wiki/Poisson_distribution // // Authors // Copyright (C) 2012 - Prateek Papriwal // [lhs,rhs] = argn() apifun_checkrhs("distfun_poissstat",rhs,1) apifun_checklhs("distfun_poissstat",lhs,1:2) // Check type // apifun_checktype("distfun_poissstat",lambda,"lambda",1,"constant") //Check content // apifun_checkgreq("distfun_poissstat",lambda,"lambda",1,1) // [lambda] = apifun_expandvar(lambda) M = lambda V = lambda endfunction
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#Property Sensor Example $thermo = VirtualMaterials.Advanced_Peng-Robinson / -> $thermo thermo + WATER TRIETHYLENE_GLYCOL #generate WATER/TEG bubble temperature curve units Field s = Stream.Stream_Material() s.In.P = 1 atm s.In.VapFrac = 0.0 ps = Sensor.PropertySensor() s.Out -> ps.In ps.SignalType = H s.In.Fraction = 0.0 1.0 s.Out.T s.In.Fraction = 0.1 0.9 s.Out.T s.In.Fraction = 0.2 0.8 s.Out.T s.In.Fraction = 0.3 0.7 s.Out.T s.In.Fraction = 0.4 0.6 s.Out.T s.In.Fraction = 0.5 0.5 s.Out.T s.In.Fraction = 0.6 0.4 s.Out.T s.In.Fraction = 0.7 0.3 s.Out.T s.In.Fraction = 0.8 0.2 s.Out.T s.In.Fraction = 0.9 0.1 s.Out.T s.In.Fraction = 1.0 0.0 s.Out.T ps.Signal
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//Chapter 15: Environmental Pollution and Control //Problem: 2 clc; //Declaration of Variables v0 = 30 // cm cube, effluent v1 = 9.8 // cm cube, K2Cr2O7 M = 0.001 // M, K2Cr2O7 // Solution Oeff = 6 * 8 * v1 * M mprintf("30 cm cube of effluent contains =:%.4f mg of O2\n",Oeff) cod = Oeff * 1000 / 30. mprintf(" 1l of the effluent requires %.2f mg of O2\n",cod) mprintf(" COD of the effluent sample=%.2f ppm",cod)
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//caption:root_locus //example 7.24.4 //page 301 clc; s=%s; syms K; GH=K/(s*(s+4)*(s^2+4*s+13)) disp("the characterstics eq. is determined as:") CH=(s*(s+4)*(s^2+4*s+13))+K CH=sym('(s*(s+4)*(s^2+4*s+13))+K'); disp('=0',CH,"characterstics_eq,CH=") c0=coeffs(CH,'s',0); c1=coeffs(CH,'s',1); c2=coeffs(CH,'s',2); c3=coeffs(CH,'s',3); c4=coeffs(CH,'s',4); b=[c0 c1 c2 c3 c4 ] routh=[b([5,3,1]);b([4,2]),0] routh=[routh;-det(routh(1:2,1:2))/routh(2,1),routh(1,3),0] routh(3,1)=simple(routh(3,1)) t=routh(2:3,1:2) l=simple(-det(t)/t(2,1)) routh=[routh;l,0,0] routh=[routh;K,0,0] K=sym('(s*(s+4)*(s^2+4*s+13))') d=diff(K,s) e=(-4*s^3+24*s^2+58*s+52) r=roots(e) disp("since -2 lies on root locus so complex breakaway point is -2+i1.58 and -2-i1.58") disp(routh,"routh=") disp("for given system to be marginally stable:"); disp("((20-4K)/5)=0 "); disp("which gives:"); disp("K=5"); K=5; k=5 a=5*s^2+5//intersection of root locus with s plane r=roots(a) g=k/(s*(s+2)*(s^2+2*s+2)) G=syslin('c',g) evans(g,200) xgrid(2) eq=(s*(s+4)*(s^2+4*s+13)) p=roots(eq) disp(p,"open loop poles are:") phi1=180-(atan(3/2)*180/%pi) phi2=atan(3/2)*180/%pi phi3=90 phi_p2=180-(phi1+phi2+phi3) phi_p3=-phi_p2 disp(phi_p2,"angle of departure for -2+3i=") disp(phi_p3,"angle of departure for -2-3i=")
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// To convert area in metre to feet // Modern Electronic Instrumentation And Measurement Techniques // By Albert D. Helfrick, William D. Cooper // First Edition Second Impression, 2009 // Dorling Kindersly Pvt. Ltd. India // Example 2-1 in Page 29 clear; clc; close; // Given data A_m = 5000; // area in metre^2 unit //Calculation A_ft = A_m * (1/0.3048)^2; // As 1ft = 0.3048m printf("The area in feet = %d sq.ft",round(A_ft)); //Result // The area in feet = 53820 sq.ft
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// exa 7.7 Pg 208 clc;clear;close; // Given Data d=50;// mm tau=42;// MPa sigma_c=72;// MPa printf('for key to be equally strong in shear & crushing - \n') b=d/4;// mm printf(' b= %.2f mm. Use b=15 mm.',b) b=15;//mm //2*b/t=sigma_c/tau for key to be equally strong in shear & crushing t=2*b/(sigma_c/tau);// mm printf('\n t=%.2f mm. Use t=20 mm',t) l= %pi*d**2/8/b;// mm (for key to be equally strong in shear as shaft) printf('\n for key to be equally strong in shear as shaft - \n') printf(' l=%.2f mm. Use l=70 mm',l)
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RI# Name Components Type Interlace Dimensions Attributes 0 Image Array 1 2 Int16 MFGR_INTERLACE_PIXEL 10, 5 0 1 Image Array 2 3 Char8 MFGR_INTERLACE_PIXEL 6, 4 2
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//Script to model influence of uniform e and b field //on charged particle motion clear(); exec('lorentz.sce'); m=1.6*(10^(-27)); q=1.6*(10^(-19)); dt=5.0*(10^(-9)); it=1:1:1000; r=zeros(3,1); v=zeros(3,1); v(2,1)=1.0*(10^6); b=zeros(3,1); e=zeros(3,1); //bfield in z direction b(3,1)=0.1; //efield in y direction //e(2,1)=0.2; //e(3,1)=10*(10^4); ns=200; labels=["v(1)";"v(2)";"v(3) "]; [ok,v(1,1),v(2,1),v(3,1)]=getvalue("define velocity values",labels,... list("vec",1,"vec",1,"vec",1),["0.0";"1.0*(10^6)";"0.0"]); iv=v; labels=["b(1)";"b(2)";"b(3) "]; [ok,b(1,1),b(2,1),b(3,1)]=getvalue("define b field values",labels,... list("vec",1,"vec",1,"vec",1),["0.0";"0.0";"0.1"]); labels=["e(1)";"e(2)";"e(3) "]; [ok,e(1,1),e(2,1),e(3,1)]=getvalue("define e field values",labels,... list("vec",1,"vec",1,"vec",1),["0.0";"0.0";"0.0"]); ar=zeros(ns,3); // xsetech([0,0,0.5,0.5]); //elseif plotid==2 then // xsetech([0.5,0.5,0.5,0.5]); //elseif plotid==3 then // xsetech([0.0,0.5,0.5,0.5]); for it=2:1:ns dv=lorentzf(q,m,v,e,b); newv=v+dv*dt; newr=r+v*dt; v=newv; r=newr; ar(it,:)=r(1:3,1)'; end; // title by default text=x_dialog('Plot Title?',''); pictitle=sprintf("%s velocity %f %f %f bfield %f %f %f efield %f %f %f ",text,iv(1,1),iv(2,1),iv(3,1),b(1,1),b(2,1),b(3,1),e(1,1),e(2,1),e(3,1)); //pictitle=sprintf("%s ",text); clf(); da=gda(); // get the handle on axes model to view and edit the fields //da.title.text=pictitle; da.title.text=pictitle; param3d(ar(:,1),ar(:,2),ar(:,3),35,45,"X@Y@Z"); l1=list('Save plot?',2,['yes','no']); saverep=x_choices('Save plot?',list(l1)) if saverep==1 then graphicsfile=xgetfile("*.scg", title="Choose a graphics file name"); xsave(graphicsfile); end;
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//Caption:calculate the speed of a d.c. shunt generator when it running as d.c. motor and taking 50 KW power at 250 volt //Exam:2.32 clc; clear; close; //calculation when machine is running as generator V=250;//applied voltage to d.c. shunt generator P_1=50000;//power delivers by d.c. shunt generator at V_1 N_1=400;//generator running at V_1 ,P_1 R_a=0.02;//armature resistance(in Ohm) R_sh=50;//field resistance(in Ohm) I_l=P_1/V;//load current(in Amp) I_sh=V/R_sh;//field current(in Amp) I_a1=I_l+I_sh;//armature current when machine working as a generator(in Amp) C_d=1;//contact drop (in volt per brush) E_1=V+I_a1*R_a+2*C_d;//induced emf by machine when working as a generator(in V) //calculation when machine is running as motor I_a2=I_l-I_sh//armature current when machine working as a motor(in Amp) E_2=V-I_a2*R_a-2*C_d;//induced emf by machine when working as a motor(in V) N_2=(E_2/E_1)*N_1;//speed of the machine when running as shunt motor(in r.p.m.) disp(N_2,'speed of the machine when running as shunt motor and taking 50 KW power at 250 volt(in r.p.m.)=');
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clc // initialization of variables T1=350+273 // initial temperature in kelvin P1=1200 // initial pressure in kPa P2=140 // final pressure in kPa k=1.4 // polytopic index for air //solution // The values are taken from table E.1 Pr660=23.13// relative pressure @ 660K Pr620=18.36// relative pressure @ 620K Pr1=((Pr660-Pr620)*3/40)+Pr620 // relative pressure by interpolation Pr2=Pr1*(P2/P1) // relative pressure at state 2 Pr340=2.149 // relative pressure @ 340K Pr380=3.176 // relative pressure @ 380K T2=((Pr2-Pr340)/(Pr380-Pr340))*40+340 // interpolating final temperature from table E.1 // now interpolating u1 AND u2 from table E.1 u620=451.0// specific internal energy @ 620k u660=481.0// specific internal energy @ 660k u1=(u660-u620)*(3/40)+u620 // initial internal energy u380=271.7 //specific internal energy @ 380k u340=242.8 //specific internal energy @ 340k u2=((Pr2-Pr340)/(Pr380-Pr340))*(u380-u340)+u340 // final internal energy w=u2-u1 // work= change in internal energy printf(" The work done by gas is %.0f kJ/kg",w) // The answer is slightly different as values are approximated in textbook
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function result=hrtTypeHex2UInt(strUInt) number = hex2dec(tokens(strUInt,' ')); result = number(1)*256+number(2); endfunction
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PL/SQL Developer Test script 3.0 10 declare --local variables e_id number :=6; v_f number; BEGIN v_f := get_Edad(e_id); dbms_output.put_line(v_f); End; 0 0
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// sum 8-10 clc; clear; A=1783; m=0.190; d=1.5; D=15; M=300; E=20800; k=30; //sigult= ultimate strength of the material // sigy= yield strength of the material sigult=A/(d^m); sigy=0.7*sigult; //siga= allowable yield strength of the material siga=sigy/2; C=D/d; Ki=(4*(C^2)-C-1)/(4*C*(C-1)); Z=%pi*(d^3)/32; //sigb=bending strength of the material; sigb=Ki*M/Z; while (sigb>=siga) d=d+0.15; D=15; C=D/d; sigult=A/(d^m); sigy=0.7*sigult; siga=sigy/2; Ki=(4*(C^2)-C-1)/(4*C*(C-1)); Z=%pi*(d^3)/32; sigb=Ki*M/Z; end d=2;// rounding off the value of the diameter. D; Na=(d^4)*E/(64*D*k); // printing data in scilab o/p window printf("d is %0.1f mm ",d); printf("\n D is %0.1f mm ",D); printf("\n Na is %0.2f mm ",Na);
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function block=ota_c(block,flag) if flag==1 block.outptr(1)=block.x(1) elseif flag==0 block.xd(1)=tanh((block.inptr(1)(1)-block.x(1)))/block.rpar; end endfunction
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//clear// clc clear k=0.1 cao=8; z0=0; z = 0:1:200; function w=f(z,x) w =zeros(1,1); lam=200-z; ca=cao*(1-x) E1=4.44658e-10*(lam^4)-1.1802e-7*(lam^3)+1.35358e-5*(lam^2)-.00086 5652*lam+.028004; E2=-2.64e-9*(lam^3)+1.3618e-6*(lam^2)-.00024069*lam+.015011 F1=4.44658e-10/5*(lam^5)-1.1802e-7/4*lam^4+1.35358e-5/3*lam^3-.000865652/2*lam^2+.028004*lam; F2=-(-9.3076e-8*lam^3+5.02846e-5*lam^2-.00941*lam+.61823-1) ra=-k*ca^2; if lam&lt; =70 E=E1 else E=(E2) end if(lam&lt; =70) F=F1 else F=F2 end EF=E/(1-F) w(1)=-(ra/cao+E/(1-F)*x) endfunction X=ode([0],z0,z,f); plot2d(z,X);
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prod_txt = ['No companies';'Nominal';'Maturité';'Fréquence';'Tranche(s)']; if exists('product') && size(product,'*')==5 then prod_def = product; else prod_def = ['100';'0.01';'5';'0.25';'[0;0.03;0.06;0.1;1]']; end; prod_def = ['100';'0.01';'5';'0.25';'[0;0.03;0.06;0.1;1]']; product = x_mdialog('Produit', prod_txt, prod_def); if (product == []) then product = prod_def; abort; else n_comp = evstr(product(1)); test_nom = execstr('evstr(product(2))',errcatch=%t); if ~test_nom then nominal = read(product(2), n_comp, 1); else nominal = evstr(product(2)); end; if (size(nominal,'*') == 1) then nominal=nominal*ones(n_comp,1); end; dates = [evstr(product(4)):evstr(product(4)):evstr(product(3))]'; tranches = evstr(product(5)); end;
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//Chapter 2 //page no 56 //given clc; clear ; Is=0.12; //in pAmp V=0.6; //in V T=293; //in Kelvin k=1.38*10^-23; //Boltzmann's Constant in J/K q=1.6*10^-19; // charge of electron in C Vt=k*T/q; //thermal voltage printf("\n VT(20 deg Cel) is %0.5f V \n",Vt);//result in book is misprint T1=373; //in Kelvin n=1.25; Vt1=k*T1/q; //thermal voltage printf("\n VT(100 deg Cel) is %0.5f V \n",Vt1); I=Is*(exp(V/(n*Vt1))-1); //forward biasing current in mircoA printf("\n I(100 deg Cel) is %0.2f microA \n",I/10^6);//result
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function [] = kiks_gui_getsenslistbox() // Display mode mode(0); // Display warning for floating point exception ieee(1); // ----------------------------------------------------- // (c) 2000-2004 Theodor Storm <theodor@tstorm.se> // http://www.tstorm.se // ----------------------------------------------------- global("KIKS_GUI_HDL","KIKS_SENS_LIST","KIKS_PROX_ACCURACY"); // !! L.9: Matlab function findobj not yet converted, original calling sequence used // L.9: Name conflict: function name changed from findobj to %findobj h = %findobj(KIKS_GUI_HDL,"Tag","proxsens_popup"); // !! L.10: Matlab function get not yet converted, original calling sequence used // L.10: Name conflict: function name changed from get to %get nr = %get(h,"Value"); KIKS_PROX_ACCURACY = mtlb_e(KIKS_SENS_LIST,nr); endfunction
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clc; p=10000; // rated power of SCIM v=420; // rated voltage of SCIM p=4; // number of poles f=50; // frequency of SCIM // results of blocked rotor test vb=210; // applied voltage ib=20; // applied current pb=5000; // power dissipated l=300; // stator core loss rs=0.6; // dc stator resistance m=3; // number of phases R=(rs*3)/2; // per phase stator resistance Rs=1.2*R; // Effective stator resistance per phase pi=pb*(v/vb)^2; // power input at rated voltage during block rotor test is=ib*(v/vb); // stator current at rated voltage during block rotor test pg=pi-m*(is/sqrt(3))^2*Rs-l; // air gap power ws=(4*%pi*f)/p; printf('synchronous speed is %f rad/sec\n',ws); T=pg/ws; printf('Starting torque is %f Nm',T);
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// Scilab Code Ex4.26:: Page-4.42 (2009) clc; clear; lambda = 6600e-010; // Wavelength of circularly polarized light, cm mu_R = 1.53914; // Refractive index of right-handed circularly polarized light mu_L = 1.53920; // Refractive index of left-handed circularly polarized light t = 0.0005; // Thickness of polarimeter plate, m theta = %pi/lambda*(mu_L-mu_R)*t; // Angle of rotation produced by the polarimeter plate, radian printf("\nThe angle of rotation produced by the polarimeter plate = %4.2f degrees", theta*180/%pi); // Result // The angle of rotation produced by the polarimeter plate = 8.18 degrees
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clear; clc; //page no. 524 c = 6;//ft b = 36;//ft AR1 = 6;//aspect ratio Cd = 0.0543;//drag coefficient Cl = 0.960;//lift coefficient alpha1 = 7.2;//degrees AR2 = 8; //for aspect ratio = 8 CL = 0.960;//negligible change of lift coefficient //for aspect ratio = 6 C_Di = Cl^2 /(%pi*AR1); //for aspect ratio = infinity C_D0 = Cd - C_Di; //for AR = 8 C_D = C_D0 + Cl^2 /(%pi*AR2); //for AR = 6 alpha_i = (180/%pi)*Cl/(%pi*AR1); //for AR = infinty alpha_0 = alpha1 - alpha_i; //for AR = 8 alpha = alpha_0 + Cl/(AR2*%pi) *(360/(2*%pi)); printf('Lift coefficient = %.3f (negligible change of lift coefficient)',CL); printf('\n Drag coefficient = %.4f',C_D); printf('\n Angle of attack = %.1f degress',alpha);
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//caption:root_locus_and_value_of_K //example 12.49 //page 576 s=%s; syms K; GH=(K*(s+4))/(s+2)^2 disp("the characterstics eq. is determined as:") CH=(s+2)^2+(K*(s+4)) CH=sym('((s+2)^2)+K*(s+4)'); disp('=0',CH,"characterstics_eq,CH=") K=sym('((s+2)^2/(s+4))') d=diff(K,s) e=(s+2)*(s+6) r1=roots(e) disp(r1,"roots=") disp("-2 and -6 is break away point") g=(s+4)/((s+2)^2) G=syslin('c',g) clf(); evans(g,10) xgrid(2) disp("for wd=2rad/sec,the point on root locus is s=-4+j2") disp("the value of K at s=-4+j2 is 4") K=4 k=4 g=k*(s+4)/((s+2)^2) cl=g/(1+g) disp(cl,"C(s)/R(s)=")
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pyImport jupyter_client py = pyBuiltin() jc = jupyter_client km = jc.KernelManager() km.start_kernel() cmd = ("a =1") c = km.client() msg_id = c.execute(cmd) state ='' c.start_channels() msg = c.get_iopub_msg(timeout =1) py.print('') py.print(msg) km.shutdown_kernel()
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//******************************************************** // animation d'un pendule élastique //******************************************************** // fonction pour créer la matrice de rotation function M=rot(a) M=[cos(a),sin(a);-sin(a),cos(a)]; endfunction // quelques constantes n=40; // nombre de spires du ressort T=5; // durée de la simulation g=9.81; // g (gravitation) k=10; // k (raideur du ressort) dt=0.01; // dt (pas de temps) //******************************************************** // lancement de l'affichage //******************************************************** // titre de la fenêtre xtitle("(clic gauche pour démarrer l''animation, clic droit pour arrêter)") // page de titre (en LaTeX) titlepage(["résolution numérique d''une EDO le pendule à ressort : "; " "; "$$\Large r{d^2\over dt^2}a+2{d\over dt}r \times {d\over dt}a=g\times \sin(a)$$"; " "; "$$\Large {d^2\over dt^2}r-{k\over m}(r-r_0)=r\left({d\over dt} a\right)^2+g\times \cos(a)$$"; " "; " avec les conditions initiales : "; "$$\Large a(0)=? \;\;\;\;\;\; {d\over dt}a(0)=0 \;\;\;\;\;\; r(0)=r_0=? \;\;\;\;\;\; {d\over dt}r(0)=0 $$"]) //******************************************************** // traitement des interactions avec la fenêtre graphique //******************************************************** [c_i,c_x,c_y,c_w]=xclick(); // attente d'un clic de souris dans la fenêtre while (c_i<>2)&(c_i<>5) // tant qu'on n'a pas fait un clic droit clf() //effacer la fenêtre //******************************************************** // récupération des données initiales de l'animation //******************************************************** // titre de la fenêtre xtitle("(un click pour initialiser la position du pendule, a(0) et r(0) )") // paramétrage du handle Axes de la fenêtre plot(0,0,'.k');A=gca();A.x_location="origin";A.y_location="origin"; A.auto_scale="off";A.isoview="on";A.data_bounds=[-1 -1; 1,0];xgrid(3) //récupération des coordonnées de la position initiale du pendule [c_i,x,y,c_w]=xclick(); // calcul des données initiales a=sign(x)*abs(atan(x/y));a0=a;da=0; // calcul de l'angle a(0) l=sqrt(x^2+y^2);r=l;,dr=0; // calcul de r(0) //adapter la taille de la fenêtre à la taille maximale du pendule A.data_bounds=[-1.5,-max(4*l,4);1.5,max(l,0.5)]; //******************************************************** // boucle créant l'animation //******************************************************** for t=0:dt:T //******************************************************** // calcul des nouvelles positions //******************************************************** // résolution des équations différentielles sur a et r par la méthode d'Euler dda=-(g*sin(a)+2*dr*da)/r; ddr=r*(da)^2-k*(r-l)+g*cos(a); da=da+dt*dda; dr=dr+dt*ddr; a=a+dt*da; r=r+dt*dr; // calcul de la ligne traçant le ressort ressortr=linspace(0,r,n)'; // étirement du ressort ressorta=[0;(-1).^[0:n-3]';0]*(l/10); // coordonnées transversales à l'axe du ressort -> /\/\/\ //rotation de l'image du ressort selon l'angle a x=[x;r*sin(a)]; y=[y;-r*cos(a)]; M=-rot(-a); N=[ressortr,ressorta]*M; ressorty=N(:,1);ressortx=N(:,2); //******************************************************** // affichage du pendule //******************************************************** drawlater() // écriture dans le buffer graphique clf() // effacer la fenêtre plot(ressortx,ressorty) // affichage du ressort du pendule xstring(0,0.1,["t=" string(t)]) // temps écoulé xfarc(r*sin(a)-0.05,-r*cos(a)+0.05,0.1,0.1,0,360*64) // la boule du prendule // redimensionnement de la fenêtre graphique A=gca();A.data_bounds=[-1.5,-max(4*l,4);1.5,max(l,0.5)]; A.auto_scale="off";A.isoview="on";A.axes_visible=["off" "off" "off"]; drawnow() // afficher le buffer graphique sleep(10); // delai d'affichage end //*********************************************************** // choix d'une nouvelle animation ou d'une sortie du script //*********************************************************** xtitle("(un clic pour continuer )") // titre de la fenêtre plot(x,y,'-r') // affichage trajectoire A=gca();A.isoview="on";xgrid(3); // afficher une grille (verte) [c_i,x,y,c_w]=xclick(); // attente d'un clic de souris dans la fenêtre graphique clf(); // choix d'une nouvelle action xtitle("(clic gauche pour démarrer l''animation, clic droit pour arrêter)") plot(0,0,'.k');A=gca();A.x_location="origin";A.y_location="origin"; [c_i,x,y,c_w]=xclick(); //attente d'un clic de souris dans la fenêtre end
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//Velocity of light in diamond clear; clc; printf("\tExample 21.2\n"); er=5.5; //Relative permitivity xm=-2.17D-5; //Magnetic Suseptibility eo=8.85D-12; //Permitivity in free space uo=4*%pi*10^-7; //Permeability e=er*eo; u=uo*(1+xm); v=1/sqrt(u*e); printf("\nVelocity in diamond is %.2e m/s\n",v); //End
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// Copyright (C) 2015 - IIT Bombay - FOSSEE // // This file must be used under the terms of the CeCILL. // This source file is licensed as described in the file COPYING, which // you should have received as part of this distribution. The terms // are also available at // http://www.cecill.info/licences/Licence_CeCILL_V2-en.txt // Author: Manoj Sree Harsha // Organization: FOSSEE, IIT Bombay // Email: toolbox@scilab.in function x = exposure(algo_type,img_index,varargin) //Compensate exposure in the specified image. // //Calling Sequence //stacksize('max') //image1=imread('path of the image file') //image2=imread('path of the image file') //y = exposure(algo_type,img_index,image1,image2) //image3=imread('path of the image file') //y = exposure(algo_type,img_index,image1,image2,image3) //image4=imread('path of the image file') //y = exposure(algo_type,img_index,image1,image2,image3,image4) //image5=imread('path of the image file') //y = exposure(algo_type,img_index,image1,image2,image3,image4,image5) //image6=imread('path of the image file') //y = exposure(algo_type,img_index,image1,image2,image3,image4,image6) // //Parameters //algo_type : an integer between 1 and 3 (both inclusive) specifying the algorithm to be used for exposure compensation. //img_index : index of the image on which exposure compensator will be applied //image1 : an image //image2 : an image //image3 : an image //image4 : an image //image5 : an image //image6 : an image // //Description //y = exposure(algo_type,img_index,image1,image2) returns an image whose exposure is compensated. //Features are extracted from each image and matching is done on two consecutive images to ensure the continuity in images. //After this camera parameters are estimated which is required to do particular type of warping. //After warping is done exposure is compensated in an image whose index is mentioned. // //Examples //a=imread('images/lenahi.jpg'); //b=imread('images/lenalow.jpg'); //algo_type=1; //img_index=1; //y=exposure(algo_type,img_index,a,b); //imshow(y) //Authors // Manoj Sree Harsha [lhs rhs]=argn(0) if rhs<4 error(msprintf("Function need atleast 4 arguments")) elseif rhs>8 error(msprintf("Too many input arguments,max. no of arguments is 8")) end for i=1:(rhs-2) varargin(i)=mattolist(varargin(i)) end if rhs==4 y=raw_exposure(algo_type,img_index,varargin(1),varargin(2)); elseif rhs==5 y=raw_exposure(algo_type,img_index,varargin(1),varargin(2),varargin(3)); elseif rhs==6 y=raw_exposure(algo_type,img_index,varargin(1),varargin(2),varargin(3),varargin(4)); elseif rhs==7 y=raw_exposure(algo_type,img_index,varargin(1),varargin(2),varargin(3),varargin(4),varargin(5)); elseif rhs==8 y=raw_exposure(algo_type,img_index,varargin(1),varargin(2),varargin(3),varargin(4),varargin(5),varargin(6)); end channels = size(y) for i = 1:channels x(:, :, i) = (y(i)) end x=double(x); endfunction
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clc //initialisation of variables i= 1/1000 d= 4 //ft C= 125 k= 0.95 o= 5.372 //CALCULATIONS h= k*d A= d^2*(o-sind(o*180/%pi))/8 P= (d/2)*o m= A/P V= C*sqrt(m*i) Q= V*A //RESULTS printf ('Discharge= %.2f cuses',Q)
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clc; //page 208 //problem 4.4 //Given modulating signal m(t) = 2*sin(2*pi*(10^3)*t), B for phase modulation Bp = 10 & for fequency modulation Bf = 10 Bp = 10 Bf = 10 //So Amplitude of modulating signal is Am=2 metres Am = 2 //Frequency of modulating signal is fm = 1000 hertz fm=1000 //Bandwidth = 2*(1+B)*fm //Bandwidth for phase modulation with modulating signal m(t) is bw_pm = 2*(1+Bp)*fm bw_pm = 2*(1+10)*1000 //Bandwidth for frequency modulation with modulating signal m(t) is bw_fm = 2*(1+Bf)*fm bw_fm = 2*(1+10)*1000 disp('Bandwidth for phase modulation '+string(bw_pm)+' Hz') disp('Bandwidth for frequency modulation '+string(bw_fm)+' Hz') //Bandwidth for phase & frequency modulation if frequency of modulating signal is doubled i.e fm = 2000 hertz //Bp & Bf after frequency of modulating signal is doubled //Bp = kp*Am, observing the equation as there is no change in amplitude Bp = 10 Bp = 10 //Bf = kf*Am/fm, observing the equation as there is change in frequency Bf = 10/2 = 5 Bf = 5 //Bandwidth for phase modulation if frequency of modulating signal is doubled is bw_double_pm = 2*(1+Bp)*fm bw_double_pm = 2*(1+10)*2000 //Bandwidth for frequency modulation if frequency of modulating signal is doubled is bw_double_fm = 2*(1+Bf)*fm bw_double_fm = 2*(1+5)*2000 disp('Bandwidth for phase modulation for doubled frequency '+string(bw_double_pm)+' Hz') disp('bandwidth for frequency modulation for doubled frequency '+string(bw_double_fm)+' Hz') //Bandwidth for phase & frequency modulation if amplitude of modulating signal is halfed i.e Am = 1 metre //Bp & Bf after amplitude of modulating signal is halfed //Bp = kp*Am, observing the equation as there is change in amplitude Bp = 10/2 = 5 Bp = 5 //Bf = kf*Am/fm, observing the equation as there is change in amplitude Bf = 5/2 = 2.5 Bf = 2.5 //Bandwidth for phase modulation if frequency of modulating signal is doubled is bw_halfed_pm = 2*(1+Bp)*fm bw_halfed_pm = 2*(1+5)*2000 //Bandwidth for frequency modulation if frequency of modulating signal is doubled is bw_halfed_fm = 2*(1+Bf)*fm bw_halfed_fm = 2*(1+2.5)*2000 disp('Bandwidth for phase modulation for halfed amplitude '+string(bw_halfed_pm)+' Hz') disp('Bandwidth for frequency modulation for halfed amplitude '+string(bw_halfed_fm)+' Hz')
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//Example 12_16 clc;clear; // Given values D=3/100;// Diameter in m P_1=150;// kPa T_1=300;// K Ma_1=0.4;// Mach number // Properties k=1.4;// Specific heat ratio C_p=1.005;// kJ/kg.K R=0.287;// kJ/kg.K nu=1.58*10^-5;//Kinematic viscosity in m^2/s // Calculation c_1=sqrt(k*R*T_1*1000);// m/s V_1=Ma_1*c_1;// Mach number Re_1=(V_1*D)/nu;// The inlet Reynolds number // The friction factor is determined from the Colebrook equation, function[X]=frictionfactor(y) X(1)=real(-(2.0*log10((0/3.7)+(2.51/((Re_1)*sqrt(y(1)))))))-(1/sqrt(y(1))); endfunction y=[0.01]; z=fsolve(y,frictionfactor); f=z(1); // The Fanno flow functions corresponding to the inlet Mach number of 0.4,From Table A-16 P_0r=1.5901;// (P_0r=P_01/P_0*) T_r=1.1628;// (T_1r=T_1/T*) P_r=2.6958;// (P_1r=P_1/P*) V_r=0.4313;// (V_1r=V_1/V*) fL_D=2.3085; L_1=((fL_D*D)/f);// m T_c=T_1/T_r;// K P_c=P_1/P_r;// kPa V_c=V_1/V_r;// m/s P_01L=(1-(1/P_0r))*100; printf('\nThe duct length=%0.2f m \nThe temperature at exit=%0.0f K \nThe pressure at exit=%0.1f kPa \nThe velocity at exit=%0.0f m/s \nThe percentage of stagnation pressure lost in the duct=%0.1f percentage',L_1,T_c,P_c,V_c,P_01L);
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//Example 16.12. clc format(5) t=1/(100*10^3) // in seconds x1=t*10^6 // in us disp(x1,"The period of oscillation is, T(us) = 1/f =") disp(" T1 = 2us (given)") t2=10-2 // in us disp(t2,"Hence, T2(us) = T - T1 =") disp(" T1 = 0.693*R1C1") c1=(2*10^-6)/(0.693*(20*10^3)) // in faraday x1=c1*10^12 // in pF disp(x1,"Therefore, C1(pF) = T1 / 0.693R1 =") //answer in textbook is wrong c2=(8*10^-6)/(0.693*(20*10^3)) // in faraday x1=c2*10^12 // in pF disp(" T2 = 0.693*R2*C2") //answer in textbook is wrong disp(x1,"Therefore, C2(pF) = T2 / 0.693R2 =")
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//page no. 31 //Example no 1-17 clc; clear all; disp('Solution (i) is '); l=0.045;//wavelength in nm h=6.63*10^-34; //planks constant in J/s c=3*10^8; //speed of light in m/s E=h*c/l/10^-9; //energy of photon in eV mprintf("\n E = %e J",E); E1=E/(1.6*10^-19); // energy in joule mprintf("\n E = %e eV",E1); e=1.6*10^-19; // charge of electron disp('Solution (ii) is '); V=E/e; printf("\n Required voltage is = %0.2f KV",V/1000);// result // Value of wavelenght in problem is .45 but in the solution is .045 //the value considered above is .045
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//METODO DE NEWTON //X vector fila con los puntos a interpolar //Y vector fila con f(X)=Y function N = newton(X, Y) n = length(X); d = zeros(n, n); d(:, 1) = Y'; for j=2:n for k=j:n d(k, j) = (d(k, j-1) - d(k-1, j-1))/(X(k) - X(k-j+1)); end end N = d(1, 1); for i=2:n N = N + d(i, i) * poly(X(1:i-1), "x"); end endfunction //function y = f(x) // y = horner(N, x); //endfunction //x = min(X):(max(X)-min(X))/100:max(X); //plot(X, Y, '*r'); //fplot2d(x, f); //o plot(x, f(x))
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load LShift.hdl, output-file LShift.out, compare-to LShift.cmp, output-list in%D1.16.1 out%D1.16.1; set in 1, eval, output; set in -1, eval, output; set in 2, eval, output; set in -2, eval, output; set in %X8000, eval, output; set in 256, eval, output; set in -256, eval, output; set in %XFFF0, eval, output;
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clear; clc; printf("\t\t\tExample Number 1.2\n\n\n"); // convection calculation // illustration1.2 // solution Twall = 250;//[degree celsius] wall temperature Tair = 20;//[degree celsius] air temperature h = 25;//[W/square meter] heat transfer coefficient l = 75*10^(-2);//[m] length of plate b = 50*10^(-2);//[m] width of plate area = l*b;//[square meter] area of plate dt = 250-20;//[degree celsius] // from newton's law of cooling q = h*area*dt;// [W] printf("rate of heat transfer is %f kW",q/1000);
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// Grob's Basic Electronics 11e // Chapter No. 19 // Example No. 19_20 clc; clear; // Two series coils, each with an L of 250 uH, have a total inductance of 550 uH connected series-aiding and 450 uH series-opposing. (a) How much is the mutual inductance Lm between the two coils? (b) How much is the coupling coefficient k? // Given data l1 = 250*10^-6; // Coil Inductance 1=250 uH l2 = 250*10^-6; // Coil Inductance 2=250 uH Lts = 550*10^-6; // Inductance series-aiding=550 uH Lto = 450*10^-6; // Inductance series-opposing=450 uH Lm = (Lts-Lto)/4 disp (Lm,'The Mutual Inductance in Henry') disp ('i.e 25 uH') lt = sqrt(l1*l2); k = Lm/lt; disp (k,'The Coupling coefficient k is')
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<scriptConfig name="VV_Test_3" script="SA13_volt_var"> <params> <param name="ratings.v_nom" type="float">0.0</param> <param name="ratings.var_ramp_max" type="float">0.0</param> <param name="ratings.k_var_max" type="float">0.0</param> <param name="ratings.v_msa" type="float">0.0</param> <param name="ratings.deadband_max" type="float">0.0</param> <param name="ratings.v_min" type="float">0.0</param> <param name="ratings.t_settling" type="float">0.0</param> <param name="ratings.s_rated" type="float">0.0</param> <param name="ratings.p_rated" type="float">0.0</param> <param name="ratings.v_max" type="float">0.0</param> <param name="ratings.deadband_min" type="float">0.0</param> <param name="ratings.var_msa" type="float">0.0</param> <param name="ratings.q_max_cap" type="float">0.0</param> <param name="ratings.q_max_ind" type="float">0.0</param> <param name="srd.segment_point_count" type="int">3</param> <param name="srd.p_min_pct" type="float">20.0</param> <param name="srd.p_max_pct" type="float">100.0</param> <param name="ratings.power_priority" type="string">Active</param> <param name="general.tests" type="string">All</param> <param name="gridsim.auto_config" type="string">Disabled</param> <param name="pvsim.mode" type="string">Manual</param> <param name="gridsim.mode" type="string">Manual</param> <param name="der.mode" type="string">Manual</param> <param name="das.mode" type="string">Manual</param> <param name="srd.k_var_min" type="string">None</param> </params> </scriptConfig>
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//find.. clc //solution //given de=650//mm re=0.325//m d=1//m r=0.500//mm n=4 q=(%pi/180)*22.5 m=2000//kg v=2.5//m/s h=2.75//m u=0.2 g=9.81//m/s^2 pb=0.3//N/mm^2 acc=v^2/(2*h)//m/s^2 fc=m*acc//N W=(2000*9.81)+fc//N T=W*re//N-m Ftt=T/r//N Ft=Ftt/4//N Rn=Ft/0.2//N //Ab=w*(2*r*sin(q))=382.7*w//mm^2 //pb=W/Ab w=Rn/(0.3*382.7)//mm printf("width of side is ,%f mm\n",w) TE=(0.5*m*v^2)+(m*g*h) printf("heat generated is,%f N-m\n",TE)
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K=4 N=9//no.of cells in 1 cluster tbw=60*10^6//total bandwidth cbwpc=25*10^3//channel bandwidth/simplex channel n=2//in a duplex link no of channels dcbw=n*cbwpc//duplex channel bandwidth N=tbw/dcbw sbw=10^6//bandwidth for setup channels N1=sbw/dcbw//total no.of available setup channels disp(N1,'total no.of available setup channels') vbw=tbw-sbw N2=vbw/dcbw//total no. of available voice channels disp(N2,'total no.of available voice channels')
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//chapter 5 //example 5.26 //Calculate minimum energy of electron //page 113-114 clear; clc; //given a=4E-10; // in m (length of the box) m=9.1E-31; // in Kg (mass of electron) h=6.626E-34; // in J-s (Planck'c constant) n1=1; // ground state e=1.6*1E-19; // in C (charge of electron) //calculate // Since E_n=n^2*h^2/(8*m*a^2) (Energy corresponding to nth quantum state) E1=n1^2*h^2/(8*m*a^2); // calculation of energy corresponding to the ground state printf('\nThe minimum energy of electron is \tE1=%1.3E J',E1); E1=E1/e; //changing unit from J to eV printf('\n\t\t\t\t\t =%.3f eV',E1); // Note: The answer in the book corresponding to J is wrong due to printing error.
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T=[10 20 40 80] M=[14.76 20.14 27.73 38.47] sqrtT=sqrt(T);
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clc cp=1.005; //kJ/kg K cv=0.718; //kJ/kg K R=0.287; //kJ/kg K m=1; //kg T1=290; //K T0=290; //K T2=400; //K p1=1; //bar p0=1; //bar p2=6; //bar //Wrev=change in internal energy - T0*change in entropy disp("(i) The irreversibility") Wrev=-[cv*(T2-T1) - T0*[cp*log(T2/T1) - R*log(p2/p1)]]; n=[1/(1-log(T2/T1)/log(p2/p1))]; Wact=m*R*(T1-T2)/(n-1); I=Wrev-Wact; disp("Irreversibility=") disp(I) disp("kJ") disp("(ii)The effectiveness = ") effectiveness=Wrev/Wact*100; disp(effectiveness) disp("%")
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clc; clear; printf("\t\t\tChapter4_example6\n\n\n"); // properties of aluminium from appendix table B1 k_al=236; p_al=2.7*1000; c_al=896; // properties of oak from appendix table B3 k_oak=0.19; p_oak=0.705*1000; c_oak=2390; sqrt_kpc_al=sqrt(k_al*p_al*c_al); printf("\nThe square root of kpc product of aluminium is %.2e sq.W.s/(m^4.sq.K)",sqrt_kpc_al); kpc_R=4; T_Li=20; T_Ri=37.3; T_al=(T_Li*(sqrt_kpc_al)+T_Ri*sqrt(kpc_R))/(sqrt_kpc_al+sqrt(kpc_R)); printf("\nThe temperature of aluminium is felt as %.1f degree celsius",T_al); sqrt_kpc_oak=sqrt(k_oak*p_oak*c_oak); printf("\nThe square root of kpc product of oak is %.2e sq.W.s/(m^4.sq.K)",sqrt_kpc_oak); T_oak=(T_Li*(sqrt_kpc_oak)+T_Ri*sqrt(kpc_R))/(sqrt_kpc_oak+sqrt(kpc_R)); printf("\nThe temperature of oak is felt as %.1f degree celsius",T_oak); if (T_al>T_oak) then printf("\nThe aluminium will feel warmer."); elseif (T_al<T_oak) then printf("\nThe oak will feel warmer."); else printf("\nBoth will be felt equally warm.") end
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clc //Intitalisation of variables clear Kx= 4 y1= 7.8 //per cent //CALCULATIONS y= ((2*(Kx+1)-sqrt(4*(Kx+1)^2-4*(Kx-1)*Kx))*100/(2*(Kx-1)))+y1 //RESULTS printf ('per cent of acid that is esterified = %.1f per cent ',y)
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clear //Given E = 30*(10**3) //ksi - The youngs modulus of the material stress_y = 40 //ksi - yield stress stress_max = 24.4 //ksi - the maximum stress l = 2 //in - The length of the crossection b = 3 //in - the width of the crossection h = 2 //in - the depth of the crossection //lets check ultimate capacity for a 2 in deep section M_ul = stress_max*b*(l**2)/4 //K-in the ultimate capacity curvature = 2*stress_y/(E*(h/2) ) //per inch the curvature of the beam curvature_max = stress_max/(E*(b/2)) //per inch The maximum curvature printf("\n the curvature in 11-in is %e per inch",curvature) printf("\n the ultimate curvature %e per inch",curvature_max)
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//Exa 2.20 clc; clear; close; //given data e=1.6*10^-19;//in coulamb rho=0.00912;//in ohm-m B=0.48;//in Wb/m^2 RH=3.55*10^-4;//in m^3-coulamb^-1 SIGMA=1/rho;//in (ohm=m)^-1 THETAh=atand(SIGMA*B*RH);//in Degree disp(THETAh,"Hall angle in degree : ");
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// Example 2.7.13 page 2.31 clc; clear; n1=1.447; //refractive index of core n2=1.442; //refractive index of cladding lamda=1.3d-6; //Wavelength a=3.6d-6; //core radius NA=sqrt(n1^2 - n2^2); //computing Numerical aperture v= 2*%pi*a*NA/lamda; //computing normalized frequency printf("As normalized frequency is %.2f which is less than 2.405, this fiber will permit single mode transmission",v); lamda_cut_off=v*lamda/2.405 lamda_cut_off=lamda_cut_off*10^9 printf("\n\nSingle mode operation will occur above this cut off wavelength of %.2f nm",lamda_cut_off); printf("\n\n NOTE - Calculation error in the book.\n(1.447^2 - 1.442^2)^0.5=0.121; they have taken 0.141\nHence calculations after that are incorrect in the book"); //Calculation error in the book.(1.447^2 - 1.442^2)^0.5=0.121; they have taken 0.141.Hence calculations after that are incorrect in the book. //They have taken radius as 2.6d-6, whereas in question it is given 3.6d-6. //answers in the book //Normalized frequency is 1.77.(incorrect) //cut off wavelength 956nm.(incorrect)
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function [P,Q,THETA,RMAT,SUCCESS] = RLG(STANCE,NORMALS,PARAMS) //Author : Maxens ACHIEPI //Space Robotics Laboratory - Tohoku University //Description: // Cxy,WS_proj_R0,footPlane_Rmat,zFinalInterval,psiInter,thetInter,phiInter //[] //INPUT //STANCE: Row array of the current footholds. Contains struct describing // footholds: // *foothold: struct. // *foothold.leg: string identifying the leg (FR,FL,HR,HL); // *foothold.pos: row vector. Position of the foot in R0 //PARAMS: a struct containing all the parameters relating to the robot // geometry, as well as problem-specific parameters: // *PARAMS.extRad; // *PARAMS.distApiOb: distances between the leg attachment and the EoF CoM // *PARAMS.intRad; // *PARAMS.halfAngle; // *PARAMS.shellPtsNb; // *PARAMS.shrink // *PARAMS.kpxy; // *PARAMS.kpz; // *PARAMS.kRot // *PARAMS.tInc; // *PARAMS.aInc; // *PARAMS.baseDimensions: (1) on x, (2) on y; // *PARAMS.legLength: [l1,l2,l3] // *PARAMS.verbose: %T or %F //OUTPUT //P: the base position //Q: the quaternion defining the rotation //THETA: the leg's joint angles //RMAT: the rotation matrix //SUCCESS: boolean for benchmarking purposes (atm) //TODO : put psi/theta/phi range finding in function // could you put bounds on phi so that it doesn't flip over? NAH(?) // put IK in function // Remove RMAT output // Change rotation parametrization to full quaternion //----------------------------------------------------------------------------// P = 0;Q = 0;THETA = 0;SUCCESS = %F;RMAT = 0; //Compute LS-fit plane by ACP stance_pos_list = STANCE(:).pos; stance_pos_array = []; for i=1:size(STANCE,2) stance_pos_array(i,:) = stance_pos_list(i); end foot_nb = size(stance_pos_array,1); [footPlane_z,footPlane_d,footPlane_or] = plane_ACP(stance_pos_array); footPlane_z = footPlane_z/norm(footPlane_z); FL_present = %f;HL_present = %f;FR_present = %f;HR_present = %f; for i=1:foot_nb select STANCE(i).leg case 'FL' then FL = i; FL_present = %t; case 'HL' then HL = i; HL_present = %t; case 'FR' then FR = i; FR_present = %t; case 'HR' then HR = i; HR_present = %t; end end if HR_present&FR_present then // footPlane_x = (STANCE(HR).pos-footPlane_or) + 0.5*(STANCE(FR).pos-STANCE(HR).pos); footPlane_x = projectionDroite(footPlane_or,STANCE(HR).pos,STANCE(FR).pos-STANCE(HR).pos); //vector from HR to orth proj of stance centroid on line HR-FR footPlane_x = footPlane_x - footPlane_or; footPlane_x = footPlane_x; // footPlane_x = projectionPlan(footPlane_x,footPlane_or,footPlane_z); // footPlane_x = footPlane_x - (footPlane_z*footPlane_or')*footPlane_z footPlane_x = footPlane_x/norm(footPlane_x); footPlane_y = cross(footPlane_z,footPlane_x); elseif HL_present&FL_present then // footPlane_x = (STANCE(HL).pos-footPlane_or) + 0.5*(STANCE(FL).pos-STANCE(HL).pos); footPlane_x = projectionDroite(footPlane_or,STANCE(HL).pos,STANCE(FL).pos-STANCE(HL).pos); //vector from HL to orth proj of stance centroid on line HL-FL footPlane_x = footPlane_x - footPlane_or; footPlane_x = -footPlane_x; // disp(footPlane_x) // footPlane_x = projectionPlan(footPlane_x,footPlane_or,footPlane_z); // footPlane_x = footPlane_x - (footPlane_z*footPlane_or')*footPlane_z // disp(footPlane_x) footPlane_x = footPlane_x/norm(footPlane_x); footPlane_y = cross(footPlane_z,footPlane_x); end footPlane_Rmat = [footPlane_x;footPlane_y;footPlane_z]; //R_P_0 [footPlane_angle,footPlane_vector] = angle_vector_FromMat(footPlane_Rmat); footPlane_Q = createQuaternion(footPlane_angle,footPlane_vector); //Compute leg approximate workspaces. Project them on footPlane. for i = 1:foot_nb //leg workspace, all points in R0 WSmi_R0 = []; WSmi_proj_RP = []; //shell descriptions shellDesc_i = struct('origin',stance_pos_array(i,:),'extRad',PARAMS.extRad(i),'intRad',PARAMS.intRad(i),'axis',NORMALS(i,:),'halfAngle',PARAMS.halfAngle); shellDesc(i) = shellDesc_i; shellDesc_AUG_i = struct('origin',stance_pos_array(i,:),'extRad',PARAMS.extRad(i)+PARAMS.distApiOb(i),'intRad',PARAMS.intRad(i),'axis',NORMALS(i,:),'halfAngle',PARAMS.halfAngle); shellDesc_AUG(i) = shellDesc_AUG_i; WSmi_alpha = linspace(0,2*%pi,PARAMS.shellPtsNb); WSmi_theta = linspace(%pi/2-shellDesc_AUG_i.halfAngle,%pi/2,PARAMS.shellPtsNb); [x1,y1,z1] = halfSph(shellDesc_AUG_i.origin,shellDesc_AUG_i.extRad,2*WSmi_alpha,WSmi_theta,shellDesc_AUG_i.axis); WSmi_R0 = [x1',y1',z1']; if shellDesc_i.intRad then [x2,y2,z2] = halfSph(shellDesc_AUG_i.origin,shellDesc_AUG_i.intRad,2*WSmi_alpha,WSmi_theta,shellDesc_AUG_i.axis); WSmi_R0 = [WSmi_R0;x2' y2' z2']; end WS_R0(:,:,i) = WSmi_R0; //projection, all points in RP for j=1:size(WSmi_R0,1) v = projectionPlan(WSmi_R0(j,:),footPlane_or,footPlane_z); WSmi_proj_R0(j,1) = v(1);WSmi_proj_R0(j,2) = v(2);WSmi_proj_R0(j,3) = v(3); v = footPlane_Rmat*(v'-footPlane_or'); WSmi_proj_RP(j,1) = v(1);WSmi_proj_RP(j,2) = v(2); end WS_proj_RP(:,:,i) = WSmi_proj_RP; WS_proj_R0(:,:,i) = WSmi_proj_R0; end //Compute Cxy Cxy = computeCxy(WS_proj_RP,[1 0;0 1]); if isnan(Cxy.origin) then if PARAMS.verbose then mprintf('Could not compute intersection of workspaces! Stance is probably unreachable...\n'); end return; end //Sample pxy_RP, transform into pxy_R0 kpxy = 0; while kpxy<PARAMS.kpxy kpxy = kpxy+1; kpz = 0; pxy_RP = sampleInBBox(Cxy,PARAMS.shrink); pxy_R0 = footPlane_Rmat'*[pxy_RP 0]'+footPlane_or'; if PARAMS.verbose then mprintf("XY - At iteration %d of %d:\nBase xy_R0 position: [%.4f, %.4f]\n",kpxy,PARAMS.kpxy,pxy_R0(1),pxy_R0(2)); end zInterval = cell(1,foot_nb); //Compute intersections of the line perpendicular to footPlane, going through pxy_R0, with the WSmi line_z = struct('origin',pxy_R0','direction',footPlane_z); for i=1:foot_nb [boolInterT_i,tMultiple_i,tInterval_i,d_i]=intersectLineWS(WS_R0(:,:,i),shellDesc_AUG(i),line_z,PARAMS.tInc); if boolInterT_i then tInterval(i).entries = createZInterval(tInterval_i,d_i); if PARAMS.verbose & tMultiple_i then mprintf(" T - For leg %d, t lies in %d different intervals", i, size(tInterval(i).entries,1)); elseif PARAMS.verbose then mprintf(" T - For leg %d, t range is: %.4f to %.4f\n",i,tInterval(i).entries(1),tInterval(i).entries(2)); end else if PARAMS.verbose then mprintf(" T - No intersection with leg %d workspace! Resampling pxy_RP...\n",i); end break; end end if ~boolInterT_i then continue; end //Sample pz_R0 [tFinalBool,tFinalInterval] = intersectSetIntervals(tInterval); if ~tFinalBool then if PARAMS.verbose then mprintf(" T - t valid intervals do not intersect! Resammpling pxy_RP...\n"); end continue; end while kpz<PARAMS.kpz kpz = kpz+1; kRot = 0; t_R0 = sampleFromMultInterval(tFinalInterval); if PARAMS.verbose then mprintf('T - At iteration %d of %d:\n Base t_R0 : %.4f\n",kpz,PARAMS.kpz,t_R0); end //Compute intersections of Api arcs and WSmi for the rotation parameter(s) base_R0 = pxy_R0'+t_R0*line_z.direction; P = base_R0; offset_i = []; xOff = [1 0 0]*PARAMS.baseDimensions(1)/2; yOff = [0 1 0]*PARAMS.baseDimensions(2)/2; //Rotation is represented by angle-vector //Sample random axis - Watch out because uniform distrib on the three coordinates is not spherically symmetric Mean = zeros(3,1);Cov = eye(3,3); while kRot<PARAMS.kRot kRot = kRot+1; rot_axis = grand(1,"mn",Mean,Cov); rot_axis = rot_axis/norm(rot_axis); rot_axis = rot_axis'; //guarantee to be uniformly distributed on the unit sphere if PARAMS.verbose then mprintf('AXIS - At iteration %d of %d:\n Axis : %.4f %.4f %.4f\n",kRot,PARAMS.kRot,rot_axis(1),rot_axis(2),rot_axis(3)); end R_0_EF = footPlane_Rmat; //initial rotation of base // R_0_EF = eye(3,3); //no base rotation angleInter=cell(1,foot_nb); arcDesc = struct('origin',base_R0,'normal',rot_axis); for i=1:foot_nb select STANCE(i).leg case 'FR' then offset_i = xOff + yOff; case 'FL' then offset_i = - xOff + yOff; case 'HR' then offset_i= + xOff - yOff; case 'HL' then offset_i = - xOff - yOff; else if PARAMS.verbose then mprintf("Error in the definition of foothold %d : leg name does not exist!\n",i); end return; end [boolInterAngle_i,angleMultiple_i,angleInter_i] = intersectArcWS(WS_R0(:,:,i),offset_i,R_0_EF,shellDesc(i),arcDesc,PARAMS.aInc); if boolInterAngle_i then angleInter(i).entries = createAngleInterval(angleInter_i); if PARAMS.verbose & angleMultiple_i then mprintf(" ANGLE - For leg %d, angle lies in %d different intervals\n", i, size(angleInter(i).entries,1)); elseif PARAMS.verbose then mprintf(" ANGLE - For leg %d, angle range is: %.4f to %.4f\n",i,angleInter(i).entries(1),angleInter(i).entries(2)); end else if PARAMS.verbose then mprintf(" ANGLE - No intersection with leg %d workspace! Resampling axis...\n",i); end break; end end if ~boolInterAngle_i then continue; end //Sample angle [angleFinalBool,angleFinalInterval] = intersectSetIntervals(angleInter); if ~angleFinalBool then if PARAMS.verbose then mprintf(" ANGLE - angle valid intervals do not intersect! Resampling axis...\n"); end continue; end angle = sampleFromMultInterval(angleFinalInterval); if PARAMS.verbose then mprintf('Rotation angle: %.4f",angle*180/%pi); end Q = quatMult(footPlane_Q,createQuaternion(angle,rot_axis)); RMAT = matrix_fromQuaternion(Q); if PARAMS.verbose then mprintf("\nBase state sampled! Now using closed form IK for the legs...\n"); end for i=1:foot_nb select STANCE(i).leg case 'FR' then offset_i = xOff + yOff; R_Leg_EF = [0 1 0;1 0 0;0 0 -1]; factor_t2 = -1; factor_t3 = -1; factor_elbow = +1; case 'FL' then offset_i = - xOff + yOff; R_Leg_EF = [0 1 0;-1 0 0;0 0 1]; factor_t2 = +1; factor_t3 = +1; factor_elbow = -1; case 'HR' then offset_i= + xOff - yOff; R_Leg_EF = [0 -1 0;1 0 0;0 0 1]; factor_t2 = +1; factor_t3 = +1; factor_elbow = -1; case 'HL' then offset_i = - xOff - yOff; R_Leg_EF = [0 -1 0;-1 0 0;0 0 -1]; factor_t2 = -1; factor_t3 = -1; factor_elbow = +1; end IK_target_RLeg = -R_Leg_EF*offset_i' + R_Leg_EF*RMAT'*(STANCE(i).pos'-base_R0'); //the foothold for the ith leg, in the leg base frame IK_target_array(:,i) = IK_target_RLeg; THETA(i,1) = atan(IK_target_RLeg(2),IK_target_RLeg(1)); rem = sqrt(IK_target_RLeg(1)**2+IK_target_RLeg(2)**2)-PARAMS.legLength(1); nc3 = IK_target_RLeg(3)**2+rem**2-PARAMS.legLength(2)**2-PARAMS.legLength(3)**2; dc3 = 2*PARAMS.legLength(2)*PARAMS.legLength(3); c3 = nc3/dc3; bool_ik = abs(c3)>1; if bool_ik then if PARAMS.verbose then mprintf("\nIK - NO SOLUTION FOR LEG %s INVERSE KINEMATICS\nResampling axis...\n",STANCE(i).leg); end // return; break; end s3 = factor_elbow*sqrt(1-c3**2); //ELBOw UP THETA(i,3) = factor_t3*atan(s3,c3); THETA(i,2) = factor_t2*(atan(IK_target_RLeg(3),rem)-atan(PARAMS.legLength(3)*s3,PARAMS.legLength(2)+PARAMS.legLength(3)*c3)) end if bool_ik then continue; end SUCCESS=%T; if PARAMS.verbose then mprintf("\nSUCCESS!\n"); end return; end if PARAMS.verbose then mprintf("AXIS - Reached maximum number of trials, resampling T...\n"); end end if PARAMS.verbose then mprintf("Z - Reached maximum number of trials, resampling XY...\n"); end end if PARAMS.verbose then mprintf("XY - Reached maximum number of trials, aborting...\n"); end endfunction
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Add16.tst
load Add16.hdl, output-file Add16.out, output-list in0%D1.6.1 in1%D1.6.1 sum%D1.6.1; set in0 %X0000, set in1 %X0000, eval, output; set in0 %X0001, set in1 %X0000, eval, output; set in0 %X0000, set in1 %X0001, eval, output; set in0 %X0001, set in1 %X0001, eval, output; set in0 %X0001, set in1 %X0003, eval, output; set in0 %X0003, set in1 %X0003, eval, output; set in0 %X0FF0, set in1 %X1000, eval, output; set in0 %X8000, set in1 %X8000, eval, output;
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FREA-ENT/svp_UL1741SA
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LVRT_VT.tst
<scriptConfig name="LVRT_LV1" script="SA9_volt_trip_time"> <params> <param name="gridsim.frea.phases" type="int">1</param> <param name="vrt.n_r" type="int">1</param> <param name="vrt.t_hold" type="float">1.0</param> <param name="eut.t_msa" type="float">1.0</param> <param name="eut.v_msa" type="float">2.0</param> <param name="eut.t_trip" type="int">5</param> <param name="vrt.v_test" type="float">100.0</param> <param name="eut.v_nom" type="float">190.0</param> <param name="gridsim.frea.ip_port" type="int">2001</param> <param name="eut.p_rated" type="int">4000</param> <param name="gridsim.frea.ip_addr" type="string">127.0.0.1</param> <param name="aist.library_version" type="string">3.0.0</param> <param name="aist.script_version" type="string">3.0.0</param> <param name="hil.mode" type="string">Disabled</param> <param name="der.mode" type="string">Disabled</param> <param name="gridsim.auto_config" type="string">Enabled</param> <param name="gridsim.mode" type="string">FREA_Simulator</param> <param name="das.mode" type="string">Manual</param> <param name="eut.phases" type="string">Single Phase</param> <param name="gridsim.frea.comm" type="string">TCP/IP</param> </params> </scriptConfig>
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example_2_6.sce
//Scilab Code for Example 2.6 of Signals and systems by //P.Ramakrishna Raoclear; clc; clear; syms s X x t R C V Vo; //After solving for I(s) //I(s)=(V-Vo)/R . 1/(s+1/RC) X=(V-Vo)/((s+1/(R*C))*R); disp(X,"I(s)="); x=ilaplace(X); disp(x,"i(t)=");
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Ch06Ex4.sce
// Scilab Code Ex6.4: Page-371 (2011) clc;clear; lambda = 3e-011;....// Wavelength of the X-ray, m d = 5e-011;....// Lattice spacing, m n = [2 3];....// Orders of diffraction // Bragg's equation for X-rays of wavelength lambda is n*lambda = 2*d*sin(theta), solving for thetas for i = 1:1:2 theta = asind(n(i)*lambda/(2*d)); printf("\nFor n = %d, theta = %4.1f degrees", n(i), theta); end // Result // For n = 2, theta = 36.9 degrees // For n = 3, theta = 64.2 degrees
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solution8_20.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('solution8_20.sce') //Obtain path of data file datapath = path + filesep() + 'data8_20.sci' //Clear all clc //Execute the data file exec(datapath) //Calculate the diameter of the rivets d (mm) d = 6 * sqrt(t) dround = ceil(d) //Calculate the shear resistance of one rivet in double shear Ps (N) Ps = 1.875 * ((%pi/4) * (dround^2) * tau) //Calculate the crushing resistance of one rivet Pc (N) Pc = dround * t * sigmac //Choose appropriate criterion P (N) if (Ps < Pc) then P = Ps else P = Pc end //Calculate the tensile strength of the plate in the outer row Pt (N) Pt = (w - dround)* t* sigmat //Calculate the number of rivets required n n = Pt/P n = ceil(n) //Calculate the margin m (mm) m = 1.5 * dround mround = round_five(m) //Calculate the transverse pitch pt (mm) pt = 2 * dround ptround = round_five(pt) //Calculate the strap thickness t1 (mm) t1 = 0.625 * t //Calculate the pitch p (mm) p = (w - (2 * mround))/2 //Calculate the strength of the joint along: //Section A-A SA = (w - dround) * t * sigmat //Section B-B SB = ((w - (2 * dround)) * t * sigmat) + Ps //Section C-C SC = ((w - (3 * dround)) * t * sigmat) + (3 * Ps) //Calculate the shear resistance of all the rivets SS (N) SS = n * Ps //Choose lowest of all the calculated strengths PLow (N) if ((SA < SB) & (SA < SC) & (SA < SS)) then PLow = SA elseif ((SB < SA) & (SB < SC) & (SB < SS)) PLow = SB elseif ((SC < SA) & (SC < SB) & (SC < SS)) Plow = SC else PLow = SS end //Calculate the strength of the plate PSolid (N) PSolid = w * t * sigmat //Calculate the efficiency of the joint eta (%) eta = (PLow/PSolid) * 100 //Print results printf('\nDiameter of the rivet(d) = %f or %f mm\n',d,dround) printf('\nNumber of rivets required(n) = %f\n',n) printf('\nMargin(m) = %f or %f mm\n',m,mround) printf('\nTransverse pitch(pt) = %f or %f mm\n',pt,ptround) printf('\nThickness of strap(t1) = %f mm\n',t1) printf('\nPitch(p) = %f mm\n',p) printf('\nEfficiency of the joints(eta) = %f percent\n',eta)
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/tests/transpose-006.tst
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../inputs/mini-06.ssv
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Ex3_4.sce
clear // // // //Variable declaration n=4 A=107.87 //atomic weight rho=10500 //density(kg/m**3) N=6.02*10**26 //number of molecules theta=19+(12/60) //angle(degrees) h=1 k=1 l=1 h0=6.625*10**-34 //planck constant c=3*10**8 //velocity of light(m/s) e=1.6*10**-19 //charge(coulomb) //Calculation theta=theta*%pi/180 //angle(radian) a=(n*A/(N*rho))**(1/3) d=a*10**10/sqrt(h**2+k**2+l**2) lamda=2*d*sin(theta) //wavelength of x rays(angstrom) E=h0*c/(lamda*10**-10*e) //energy of x rays(eV) //Result printf("\n wavelength of x rays is %0.3f angstrom",lamda) printf("\n answer varies due to rounding off errors") printf("\n energy of x rays is %0.0f *10**3 eV",E/10**3)
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/PresentationFiles_Subjects - Kopie/CONT/JH56CNU/ATWM1_Working_Memory_MRI_Nonsalient_Cued_Run1.sce
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atwm1/Presentation
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9732a004ca091b184b670c56c55f538ff6600c08
refs/heads/master
2020-04-15T14:04:41.900640
2020-02-14T16:10:11
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sce
ATWM1_Working_Memory_MRI_Nonsalient_Cued_Run1.sce
# ATWM1 MRI Experiment scenario = "ATWM1_Working_Memory_MRI_nonsalient_cued_run1"; scenario_type = fMRI; # Fuer Scanner #scenario_type = fMRI_emulation; # Zum Testen #scenario_type = trials; scan_period = 2000; # TR pulses_per_scan = 1; pulse_code = 1; #pulse_width=6; default_monitor_sounds = false; active_buttons = 2; response_matching = simple_matching; button_codes = 10, 20; default_font_size = 28; default_font = "Arial"; default_background_color = 0 ,0 ,0 ; #write_codes=true; # for MEG only begin; #Picture definitions box { height = 300; width = 300; color = 0, 0, 0;} frame1; box { height = 290; width = 290; color = 255, 255, 255;} frame2; box { height = 30; width = 4; color = 0, 0, 0;} fix1; box { height = 4; width = 30; color = 0, 0, 0;} fix2; box { height = 30; width = 4; color = 255, 0, 0;} fix3; box { height = 4; width = 30; color = 255, 0, 0;} fix4; box { height = 290; width = 290; color = 128, 128, 128;} background; TEMPLATE "StimuliDeclaration.tem" {}; trial { sound sound_incorrect; time = 0; duration = 1; } wrong; trial { sound sound_correct; time = 0; duration = 1; } right; trial { sound sound_no_response; time = 0; duration = 1; } miss; # baselinePre (at the beginning of the session) trial { picture { box frame1; x=0; y=0; box frame2; x=0; y=0; box background; x=0; y=0; bitmap fixation_cross_black; x=0; y=0; }default; time = 0; duration = 9400; mri_pulse = 1; code = "BaselinePre"; #port_code = 1; }; TEMPLATE "ATWM1_Working_Memory_MRI.tem" { trigger_volume_encoding trigger_volume_retrieval cue_time preparation_time encoding_time single_stimulus_presentation_time delay_time retrieval_time intertrial_interval alerting_cross stim_enc1 stim_enc2 stim_enc3 stim_enc4 stim_enc_alt1 stim_enc_alt2 stim_enc_alt3 stim_enc_alt4 trial_code stim_retr1 stim_retr2 stim_retr3 stim_retr4 stim_cue1 stim_cue2 stim_cue3 stim_cue4 fixationcross_cued retr_code the_target_button posX1 posY1 posX2 posY2 posX3 posY3 posX4 posY4; 6 11 292 292 399 125 9543 2992 14342 fixation_cross gabor_127 gabor_046 gabor_076 gabor_154 gabor_127_alt gabor_046 gabor_076_alt gabor_154 "1_1_Encoding_Working_Memory_MRI_P6_LR_Nonsalient_DoChange_CuedRetrieval_300_300_399_9601_3000_14400_gabor_patch_orientation_127_046_076_154_target_position_2_4_retrieval_position_2" gabor_circ gabor_093_framed gabor_circ gabor_circ blank blank blank blank fixation_cross_target_position_2_4 "1_1_Retrieval_Working_Memory_MRI_P6_LR_Nonsalient_DoChange_CuedRetrieval_retrieval_patch_orientation_093_retrieval_position_2" 2 45.96 45.96 -45.96 45.96 -45.96 -45.96 45.96 -45.96; 20 25 292 292 399 125 9543 2992 12342 fixation_cross gabor_046 gabor_063 gabor_097 gabor_169 gabor_046 gabor_063 gabor_097_alt gabor_169_alt "1_2_Encoding_Working_Memory_MRI_P6_LR_Nonsalient_DoChange_CuedRetrieval_300_300_399_9601_3000_12400_gabor_patch_orientation_046_063_097_169_target_position_1_2_retrieval_position_2" gabor_circ gabor_018_framed gabor_circ gabor_circ blank blank blank blank fixation_cross_target_position_1_2 "1_2_Retrieval_Working_Memory_MRI_P6_LR_Nonsalient_DoChange_CuedRetrieval_retrieval_patch_orientation_018_retrieval_position_2" 2 45.96 45.96 -45.96 45.96 -45.96 -45.96 45.96 -45.96; 33 38 292 292 399 125 9543 2992 14342 fixation_cross gabor_009 gabor_118 gabor_039 gabor_145 gabor_009 gabor_118 gabor_039_alt gabor_145_alt "1_3_Encoding_Working_Memory_MRI_P6_LR_Nonsalient_NoChange_CuedRetrieval_300_300_399_9601_3000_14400_gabor_patch_orientation_009_118_039_145_target_position_1_2_retrieval_position_2" gabor_circ gabor_118_framed gabor_circ gabor_circ blank blank blank blank fixation_cross_target_position_1_2 "1_3_Retrieval_Working_Memory_MRI_P6_LR_Nonsalient_NoChange_CuedRetrieval_retrieval_patch_orientation_118_retrieval_position_2" 1 45.96 45.96 -45.96 45.96 -45.96 -45.96 45.96 -45.96; 47 52 292 292 399 125 9543 2992 12342 fixation_cross gabor_027 gabor_058 gabor_073 gabor_101 gabor_027 gabor_058 gabor_073_alt gabor_101_alt "1_4_Encoding_Working_Memory_MRI_P6_LR_Nonsalient_NoChange_UncuedRetriev_300_300_399_9601_3000_12400_gabor_patch_orientation_027_058_073_101_target_position_1_2_retrieval_position_4" gabor_circ gabor_circ gabor_circ gabor_101_framed blank blank blank blank fixation_cross_target_position_1_2 "1_4_Retrieval_Working_Memory_MRI_P6_LR_Nonsalient_NoChange_UncuedRetriev_retrieval_patch_orientation_101_retrieval_position_4" 1 45.96 45.96 -45.96 45.96 -45.96 -45.96 45.96 -45.96; 60 66 292 292 399 125 11543 2992 14342 fixation_cross gabor_121 gabor_067 gabor_175 gabor_098 gabor_121_alt gabor_067_alt gabor_175 gabor_098 "1_5_Encoding_Working_Memory_MRI_P6_LR_Nonsalient_NoChange_CuedRetrieval_300_300_399_11601_3000_14400_gabor_patch_orientation_121_067_175_098_target_position_3_4_retrieval_position_4" gabor_circ gabor_circ gabor_circ gabor_098_framed blank blank blank blank fixation_cross_target_position_3_4 "1_5_Retrieval_Working_Memory_MRI_P6_LR_Nonsalient_NoChange_CuedRetrieval_retrieval_patch_orientation_098_retrieval_position_4" 1 45.96 45.96 -45.96 45.96 -45.96 -45.96 45.96 -45.96; 75 80 292 292 399 125 9543 2992 12342 fixation_cross gabor_105 gabor_029 gabor_157 gabor_138 gabor_105_alt gabor_029 gabor_157_alt gabor_138 "1_6_Encoding_Working_Memory_MRI_P6_LR_Nonsalient_NoChange_CuedRetrieval_300_300_399_9601_3000_12400_gabor_patch_orientation_105_029_157_138_target_position_2_4_retrieval_position_2" gabor_circ gabor_029_framed gabor_circ gabor_circ blank blank blank blank fixation_cross_target_position_2_4 "1_6_Retrieval_Working_Memory_MRI_P6_LR_Nonsalient_NoChange_CuedRetrieval_retrieval_patch_orientation_029_retrieval_position_2" 1 45.96 45.96 -45.96 45.96 -45.96 -45.96 45.96 -45.96; 88 93 292 292 399 125 9543 2992 12342 fixation_cross gabor_011 gabor_122 gabor_082 gabor_151 gabor_011_alt gabor_122 gabor_082_alt gabor_151 "1_7_Encoding_Working_Memory_MRI_P6_LR_Nonsalient_NoChange_CuedRetrieval_300_300_399_9601_3000_12400_gabor_patch_orientation_011_122_082_151_target_position_2_4_retrieval_position_2" gabor_circ gabor_122_framed gabor_circ gabor_circ blank blank blank blank fixation_cross_target_position_2_4 "1_7_Retrieval_Working_Memory_MRI_P6_LR_Nonsalient_NoChange_CuedRetrieval_retrieval_patch_orientation_122_retrieval_position_2" 1 45.96 45.96 -45.96 45.96 -45.96 -45.96 45.96 -45.96; 101 107 292 292 399 125 11543 2992 14342 fixation_cross gabor_002 gabor_142 gabor_109 gabor_167 gabor_002 gabor_142_alt gabor_109_alt gabor_167 "1_8_Encoding_Working_Memory_MRI_P6_LR_Nonsalient_DoChange_UncuedRetriev_300_300_399_11601_3000_14400_gabor_patch_orientation_002_142_109_167_target_position_1_4_retrieval_position_2" gabor_circ gabor_092_framed gabor_circ gabor_circ blank blank blank blank fixation_cross_target_position_1_4 "1_8_Retrieval_Working_Memory_MRI_P6_LR_Nonsalient_DoChange_UncuedRetriev_retrieval_patch_orientation_092_retrieval_position_2" 2 45.96 45.96 -45.96 45.96 -45.96 -45.96 45.96 -45.96; 116 122 292 292 399 125 11543 2992 14342 fixation_cross gabor_133 gabor_025 gabor_062 gabor_103 gabor_133 gabor_025_alt gabor_062 gabor_103_alt "1_9_Encoding_Working_Memory_MRI_P6_LR_Nonsalient_DoChange_CuedRetrieval_300_300_399_11601_3000_14400_gabor_patch_orientation_133_025_062_103_target_position_1_3_retrieval_position_1" gabor_179_framed gabor_circ gabor_circ gabor_circ blank blank blank blank fixation_cross_target_position_1_3 "1_9_Retrieval_Working_Memory_MRI_P6_LR_Nonsalient_DoChange_CuedRetrieval_retrieval_patch_orientation_179_retrieval_position_1" 2 45.96 45.96 -45.96 45.96 -45.96 -45.96 45.96 -45.96; 131 137 292 292 399 125 11543 2992 14342 fixation_cross gabor_045 gabor_174 gabor_008 gabor_064 gabor_045_alt gabor_174 gabor_008_alt gabor_064 "1_10_Encoding_Working_Memory_MRI_P6_LR_Nonsalient_DoChange_CuedRetrieval_300_300_399_11601_3000_14400_gabor_patch_orientation_045_174_008_064_target_position_2_4_retrieval_position_4" gabor_circ gabor_circ gabor_circ gabor_114_framed blank blank blank blank fixation_cross_target_position_2_4 "1_10_Retrieval_Working_Memory_MRI_P6_LR_Nonsalient_DoChange_CuedRetrieval_retrieval_patch_orientation_114_retrieval_position_4" 2 45.96 45.96 -45.96 45.96 -45.96 -45.96 45.96 -45.96; 146 152 292 292 399 125 11543 2992 14342 fixation_cross gabor_083 gabor_045 gabor_163 gabor_017 gabor_083 gabor_045 gabor_163_alt gabor_017_alt "1_11_Encoding_Working_Memory_MRI_P6_LR_Nonsalient_NoChange_CuedRetrieval_300_300_399_11601_3000_14400_gabor_patch_orientation_083_045_163_017_target_position_1_2_retrieval_position_1" gabor_083_framed gabor_circ gabor_circ gabor_circ blank blank blank blank fixation_cross_target_position_1_2 "1_11_Retrieval_Working_Memory_MRI_P6_LR_Nonsalient_NoChange_CuedRetrieval_retrieval_patch_orientation_083_retrieval_position_1" 1 45.96 45.96 -45.96 45.96 -45.96 -45.96 45.96 -45.96; 161 167 292 292 399 125 11543 2992 12342 fixation_cross gabor_013 gabor_044 gabor_124 gabor_178 gabor_013 gabor_044_alt gabor_124_alt gabor_178 "1_12_Encoding_Working_Memory_MRI_P6_LR_Nonsalient_NoChange_UncuedRetriev_300_300_399_11601_3000_12400_gabor_patch_orientation_013_044_124_178_target_position_1_4_retrieval_position_2" gabor_circ gabor_044_framed gabor_circ gabor_circ blank blank blank blank fixation_cross_target_position_1_4 "1_12_Retrieval_Working_Memory_MRI_P6_LR_Nonsalient_NoChange_UncuedRetriev_retrieval_patch_orientation_044_retrieval_position_2" 1 45.96 45.96 -45.96 45.96 -45.96 -45.96 45.96 -45.96; 175 180 292 292 399 125 9543 2992 12342 fixation_cross gabor_040 gabor_150 gabor_069 gabor_084 gabor_040_alt gabor_150 gabor_069_alt gabor_084 "1_13_Encoding_Working_Memory_MRI_P6_LR_Nonsalient_NoChange_CuedRetrieval_300_300_399_9601_3000_12400_gabor_patch_orientation_040_150_069_084_target_position_2_4_retrieval_position_4" gabor_circ gabor_circ gabor_circ gabor_084_framed blank blank blank blank fixation_cross_target_position_2_4 "1_13_Retrieval_Working_Memory_MRI_P6_LR_Nonsalient_NoChange_CuedRetrieval_retrieval_patch_orientation_084_retrieval_position_4" 1 45.96 45.96 -45.96 45.96 -45.96 -45.96 45.96 -45.96; 188 193 292 292 399 125 9543 2992 14342 fixation_cross gabor_091 gabor_157 gabor_177 gabor_046 gabor_091 gabor_157_alt gabor_177 gabor_046_alt "1_14_Encoding_Working_Memory_MRI_P6_LR_Nonsalient_DoChange_CuedRetrieval_300_300_399_9601_3000_14400_gabor_patch_orientation_091_157_177_046_target_position_1_3_retrieval_position_3" gabor_circ gabor_circ gabor_130_framed gabor_circ blank blank blank blank fixation_cross_target_position_1_3 "1_14_Retrieval_Working_Memory_MRI_P6_LR_Nonsalient_DoChange_CuedRetrieval_retrieval_patch_orientation_130_retrieval_position_3" 2 45.96 45.96 -45.96 45.96 -45.96 -45.96 45.96 -45.96; 202 208 292 292 399 125 11543 2992 12342 fixation_cross gabor_042 gabor_061 gabor_129 gabor_019 gabor_042_alt gabor_061 gabor_129 gabor_019_alt "1_15_Encoding_Working_Memory_MRI_P6_LR_Nonsalient_DoChange_CuedRetrieval_300_300_399_11601_3000_12400_gabor_patch_orientation_042_061_129_019_target_position_2_3_retrieval_position_3" gabor_circ gabor_circ gabor_179_framed gabor_circ blank blank blank blank fixation_cross_target_position_2_3 "1_15_Retrieval_Working_Memory_MRI_P6_LR_Nonsalient_DoChange_CuedRetrieval_retrieval_patch_orientation_179_retrieval_position_3" 2 45.96 45.96 -45.96 45.96 -45.96 -45.96 45.96 -45.96; }; # baselinePost (at the end of the session) trial { picture { box frame1; x=0; y=0; box frame2; x=0; y=0; box background; x=0; y=0; bitmap fixation_cross_black; x=0; y=0; }; time = 0; duration = 20600; code = "BaselinePost"; #port_code = 2; };
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EX2_1.sce
//Clearing Console clc clear //Node 1 Displacement U1=0 //Stiffness of Springs K1=50 K2=75 //Nodal Forces F2=75 F3=75 //varible decleration K=[] F=[] U=[] //Constructing Stiffness and Force matrices K(1,1)=K1+K2 K(1,2)=-K2 K(2,1)=-K2 K(2,2)=K2 F(1,1)=F2 F(2,1)=F3 //Solving for Nodal Displacements U2 and U3 U=linsolve(K,-F) //K*U=F (equlibrium equation) //Solving for Nodal force F1 F1=-50*U(1,1) //Printing Results printf('\nResults\n') printf('\nNodal displacements \nU1=%fin \nU2=%fin \nU3=%fin\n',U1,U(1,1),U(2,1)) printf('\nNodal Force F1=%flb\n',F1)
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Example_7_2.sce
//Example 7.2 clear; clc; //Given R=0.08205;//gas constant in dm^3 atm K^-1 mol^-1 b=0.0391;//Van der Waals constant in dm^3 mol^-1 T=1273;//Temperature in K P=1000;//pressure in atm //To calculate the fugacity coefficient k=(b*P)/(R*T);//k=log(f/P) f=P*exp(k);//fugacity coefficient in atm mprintf('Fugacity coefficient = %f atm',f); //end
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/Graph/plot using plot2d keyword and using numbers for changing marker.sce
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plot using plot2d keyword and using numbers for changing marker.sce
x = [0 : 0.1: 2*%pi]; y = sin(x); plot2d(x, y, -3); // markers are represented by negative no. plot2d(x, y, -2);
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load MAdd16.hdl, output-file MAdd16.out, output-list a%B1.16.1 b%B1.16.1 out%B1.16.1; set a %B0101000101110111, set b %B0011101101101000, eval, output; set a %B1100110100100100, set b %B0001100101100011, eval, output; set a %B0001011101101101, set b %B0110010000110101, eval, output; set a %B1100000011100110, set b %B0010110101000100, eval, output; set a %B1000000111100000, set b %B1000111011100100, eval, output; set a %B1010000111010100, set b %B0001101101001001, eval, output; set a %B0100110110010110, set b %B1110011010101010, eval, output; set a %B1011110111001100, set b %B1101010000001011, eval, output; set a %B1010011101010100, set b %B0110101011100000, eval, output; set a %B1111100011010100, set b %B1011110010000001, eval, output; set a %B1000000001101111, set b %B1001001011110000, eval, output; set a %B0011111001101111, set b %B1110001010100101, eval, output; set a %B0001111101000100, set b %B1100110010110100, eval, output; set a %B0111000110111011, set b %B0001101000111101, eval, output; set a %B0011001001001011, set b %B1111001111000110, eval, output; set a %B1001110101100001, set b %B0011110101111101, eval, output;
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Ex7_2.sce
clear // // // //Variable declaration lamda=0.58 //wavelength(angstrom) theta1=6.45*%pi/180 //glancing angle(radian) theta2=9.15*%pi/180 //glancing angle(radian) theta3=13*%pi/180 //glancing angle(radian) n=1 //order //Calculation d1=lamda/(2*sin(theta1)) //interplanar spacing at 1st angle(angstrom) d2=lamda/(2*sin(theta2)) //interplanar spacing at 2nd angle(angstrom) d3=lamda/(2*sin(theta3)) //interplanar spacing at 3rd angle(angstrom) //Result printf("\n interplanar spacing at 1st angle is %0.3f angstrom",d1) printf("\n interplanar spacing at 2nd angle is %0.3f angstrom",d2) printf("\n interplanar spacing at 3rd angle is %0.3f angstrom",d3) printf("\n answers given in the book are wrong")
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Ex14_23_12.sce
//Section-14,Example-6,Page no.-PC.84 //To calculate the free energy change and justify the given reactions. clc; //Cu_2S + O_2 = 2Cu + SO_2 dl_G1=88.2 dl_G2=300.1 dl_G=dl_G1-dl_G2 disp(dl_G,'Free energy change(kJ)')
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Ex13_11.sce
//Introduction to Fiber Optics by A. Ghatak and K. Thyagarajan, Cambridge, New Delhi, 1999 //Example 13.11 //OS=Windows XP sp3 //Scilab version 5.5.2 clc; clear; //given R=0.5;//Responsivity in A/W T=300;//Missing data- Temperature in K C=1e-12;//Photodiode capacitance in F BER=1e-9;//Bit error rate SNR=144;//Signal-to-noise ratio corresponding to BER of (10)^(-9) kB=1.38e-23;//Boltzmann constant in SI Units //Case(i): B=100e6;//Bit rate in b/s Pmin=B/R*sqrt(2*%pi*kB*T*C*SNR); mprintf("\n For 100 Mb/s, Pmin=%.2f uW",Pmin/1e-6);//Dividing by 10^(-6) to convert into uW //Case(ii): B=1e9;//Bit rate in b/s Pmin=B/R*sqrt(2*%pi*kB*T*C*SNR); mprintf("\n For 1 Gb/s, Pmin=%.2f uW",Pmin/1e-6);//Dividing by 10^(-6) to convert into uW
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//chapter 5 //example 5.7 //Calculate velocity and kinetic energy //page 105 clear; clc; //given lambda=1.66E-10; // in m (wavelength) m=9.1E-31; // in Kg (mass of electron) h=6.626E-34; // in J-s (Planck's constant) e=1.6E-19; // in C (charge on electron) //calculate // Since lambda=h/(m*v) // Therefore we have v=h/(m*lambda); // calculation of velocity printf('\nThe velocity of electron is \tv=%1.3E m/s',v); K=m*v^2/2;//calculation of kinetic energy printf('\nThe kinetic energy is \tK=%1.4E J',K); K=K/e; // changing unit from J to eV printf('\n\t\t\t=%.3f eV',K); // Note: The answer in the book for kinetic energy is wrong due to calculation mistake
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//5.8 clc; f=50; Vin=230; w=2*%pi*f; L=20*10^-3;R=5; th=atand(R/(w*L)); printf("Firing angle=%.2f degree",th) disp('Therefore, Range of firing angle is 38.51 degree to 180 degree') Beta=180; printf("Conduction angle of thyristor=%.0f degree",Beta) IL=Vin/((R^2+w^2*L^2))^0.5; printf(" \nRMS load current =%.2f A", IL) Po=IL^2*R; printf(" \nPower Output =%.2f W", Po) pf_input=Po/(Vin*IL); printf(" \nInput Power factor =%.3f lagging", pf_input)
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//Solutions to Problems In applied mechanics //A N Gobby clear all; clc //initialisation of variables a=10//ft/s x=1/12//ft/s g=32.2//ft //CALCULATIONS P=2*%pi*sqrt(x/a)//sec L=(P)/(2*%pi/sqrt(g))/2//ft //RESULTS printf('the simple pendulum =% f ft',L)
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//Change plus/minus interaction depending on the scalar product of the vectors //main clear; number_of_steps = 50;//number of inetrations n = 3; //number of agents a = [1,0]; agents(:,1) = zeros(n,1); agents(:,2) = ones(n,1); for i = 1:n val(i,1) = abs(rand()); val(i,2) = abs(rand()); s = val(i,1)+val(i,2); val(i,1) = val(i,1) / s; val(i,2) = val(i,2) / s; end p = [0,0]; for i=1:n for j =1:2 X(i,1,j) = agents(i,j) end end for k = 1:number_of_steps // Value(k,:) = v for i = 1:n p = [X(i,k,1) X(i,k,2)] v = val(i,:) tau = max(v.*p, v.*a) p_temp = p + tau s = sum(p_temp) p = p_temp ./ s X(i,k+1,1) = p(1) X(i,k+1,2) = p(2) end end t = [1:1:number_of_steps] mean_val = mean(val,'c'); for k = 1:number_of_steps for i =1:n for j = 1:2 temp(j,i) = X(i,k,j) end end mean_agents(k,1) = mean(temp(1,:),'c'); mean_agents(k,2) = mean(temp(2,:),'c'); end //t=[1:1:number_of_steps+1] //V1 = mean_val(1).*ones(1,number_of_steps+1) //V2 = mean_val(2).*ones(1,number_of_steps+1) //plot(t,V1,'r',t,V2,'r') //plot(mean_agents) //legend('innovation', 'old product') for i=1:n for k=1:number_of_steps y1(i,k) = X(i,k,1) y2(i,k) = X(i,k,2) end end plot(t',y1,'--') plot(t',y2)
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clc // initialization of variables clear sig_xx=20 // MPa sig_yy=10 // MPa sig_xy=30 // MPa sig_xz=-10 // MPa sig_yz=80 // MPa I2=-7800 // (MPa)^2 // part (a) // Assume sig_zz=k and evaluate determinants to solve for k det1=sig_xx*sig_yy-sig_xy^2 //det2=k*sig_xx-sig_xz^2 //det3=k*sig_yy-sig_yz^2 k=(I2-det1+sig_xz^2+sig_yz^2)/(sig_xx+sig_yy) sig_zz=k I1=sig_xx+sig_yy+sig_zz M=[sig_xx sig_xy sig_xz sig_xy sig_yy sig_yz sig_xz sig_yz sig_zz] I3=det(M) // p=poly([1 -I1 I2 -I3], "x") p=[1 -I1 I2 -I3] sigma=roots(p) // results printf('\n part (a) \n') printf(' The unknown stress component is = %.d M Pa and the stress invariants I1, I2, I3 are respectively %.d , %.d , %.d ',sig_zz,I1,I2,I3) printf('\n The principal stresses are sigma1= %.3f , sigma2=%.3f , sigma3=%.3f M Pa',sigma(2),sigma(3),sigma(1))
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// Exa 4.22 clc; clear; close; format('v',6) // Given data P = 100;// in W V = 120;// in V f= 50;// in Hz I = P/V;// in A V = 200;// in V V_R = 120;// in V V_L = sqrt( (V^2) - (V_R^2) );// in V // V_L = I*X_L; X_L = V_L/I;// in ohm // X_L = 2*%pi*f*L; L = X_L/(2*%pi*f);// in H disp(L,"The value of pure inductance in H is"); // Note: There is calculation error to find the value of V_L, So the answer in the book is wrong and coding is correct.
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clc // Given that alpha = %pi / 3 // angle between polarizer and analyzer // Sample Problem 7 on page no. 3.25 printf("\n # PROBLEM 7 # \n") r = (cos(alpha))^2 // where r = transmitted intensity / incident intensity printf("\n Standard formula used \n r = (cos(alpha))^2. \n") printf("\n Ratio between transmitted intensity to incident intensity = %f ",r)
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Bode Plot.sce
steps_per_dec = 6; decades = 6; start_freq = 0.1; // the transfer function function foo=G(w) D = %i*w; foo = ((D+1000)/(D^2+5*D+100)); endfunction // this section writes the values to a datafile that may be graphed in a spreadsheet fd = mopen("data.txt", "w"); for step = 0:(steps_per_dec*decades), f = start_freq*10^(step/steps_per_dec); //calculate the next frequency w = f*2*%pi; //convert the frequency to radians [gain,phase] = polar(G(w)); //find the gain and convert it to mag and angle gaindb = 20*log10(gain); //convert magnitude to dB phasedeg = 180*phase/%pi; //convert to degrees //mfprint(fd, "%f, %f, %f \n", f, gaindb, phasedeg); end mclose(fd); //to graph it directly the following is used D = poly(0, 'D'); h = syslin('c', ((D+1000)/(D^2+5*D+100))); bode(h, 0.1, 1000, 'Sample Transfer Function');
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k = [0.3090 0.9800 0.0031 0.0082 0.0082]; l = [10 0.9800 0.0031 0.0082 0.0082]; [a, efinal] = rc2poly(k,l) disp(a); disp(efinal); //output //!--error 15 //Submatrix incorrectly defined. //at line 44 of function rc2poly called by : //[a, efinal] = rc2poly(X,l) //at line 3 of exec file called by : //2poly\rc2poly4.sce', -1 //MATLAB o/p //Subscripted assignment dimension mismatch. //Error in rc2poly (line 54) //e(1) = e0.*(1-kr(1)'.*kr(1));
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example5_5_TACC.sce
//example 5.5 clear; clc; //Given: T=298;//Temperature [K] n=1;//no. of moles V1=500;//initial volume [cm3] V2=1000;//final volume [cm3] R=8.314;//Universal gas constant [J/mol/K] //to find the molar entropy change S=R*log(V2/V1)//molar entropy change at constant temperature[J/K] printf("Molar entropy change of argon = %f J/K", S);
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//Example 17.3 ratio=2;//Ratio of the two sound wave intensities, I2/I1 delta_beta=10*log10(ratio);//Difference in sound intensity levels, beta2-beta1, (dB) printf('Difference in sound level = %0.2fdB (when one sound wave is twice as intense as the other)',delta_beta) //Openstax - College Physics //Download for free at http://cnx.org/content/col11406/latest
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Ex2_9.sce
// Example 2.9 clc; clear; close; // Given data format('v',9); V1= 745;// in µV V2= 740;// in µV Ad= 5*10^5;// differential voltage gain CMRR= 80;// in dB CMRR= 10^(CMRR/20); Vd= V1-V2;// difference signal in µV Vcm= (V1+V2)/2;// common-mode signal in µV // Output voltage, Vout= Ad*Vd*(1+1/CMRR*Vcm/Vd);// in µV AdVd= Ad*Vd;// in µV // Error voltage Verror= Vout-AdVd;// in µV Vout= Vout*10^-6;// in V Verror= Verror*10^-6;// in V Per_error= Verror/Vout*100;// percentage error disp(Vout,"The output voltage in volts is : ") disp(Per_error,"The percentage error in the output voltage is : ")
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clear; clc; ia=20; ib=20*(%e^(%i*%pi)); ic=0; a=1*%e^(%i*(120*%pi/180)); b=a^2; ia0=1/3*(ia+ib+ic); ia1=1/3*(ia+(a*ib)+(b*ic)); ia2=1/3*(ia+(b*ib)+(a*ic)); ia0r=real(ia0); ia0i=imag(ia0); ia0m=sqrt((ia0r^2)+(ia0i^2)); ia0a=0-atand(ia0r/ia0i); ia1r=real(ia1); ia1i=imag(ia1); ia1m=sqrt((ia1r^2)+(ia1i^2)); ia1a=atand(ia1i/ia1r); ia2r=real(ia2); ia2i=imag(ia2); ia2m=sqrt((ia2r^2)+(ia2i^2)); ia2a=atand(ia2i/ia2r); mprintf("the symmetric components are \n ia0=%f+j%f A \tor\t %f/_%d A",ia0r,ia0i,ia0m,ia0a); mprintf("\n ia1=%f+j%f A \tor\t %f/_%d A",ia1r,ia1i,ia1m,ia1a); mprintf("\n ia2=%f+j(%f) A \tor\t %f/_%d A",ia2r,ia2i,ia2m,ia2a); ib1=b*ia1; ib2=a*ia2; ic1=a*ia1; ic2=b*ia2; ib0=ia0; ic0=ia0; ib1r=real(ib1); ib1i=imag(ib1); ib1m=sqrt((ib1r^2)+(ib1i^2)); ib1a=atand(ib1i/ib1r); ib2r=real(ib2); ib2i=imag(ib2); ib2m=sqrt((ib2r^2)+(ib2i^2)); ib2a=atand(ib2i/ib2r); ic1r=real(ic1); ic1i=imag(ic1); ic1m=sqrt((ic1r^2)+(ic1i^2)); ic1a=atand(ic1i/ic1r); ic2r=real(ic2); ic2i=imag(ic2); ic2m=sqrt((ic2r^2)+(ic2i^2)); ic2a=atand(ic2i/ic2r); mprintf("\n \n ib0=%fA ",ib0); mprintf("\n ib1=%f+j%f A \tor\t %f/_%d A",ib1r,ib1i,ib1m,ib1a); mprintf("\n ib2=%f+j(%f) A \tor\t %f/_%d A",ib2r,ib2i,ib2m,ib2a); mprintf("\n \n ic0=%f A",ic0); mprintf("\n ic1=%f+j%f A \tor\t %f/_%d A",ic1r,ic1i,ic1m,ic1a); mprintf("\n ic2=%f+j(%f) A \tor\t %f/_%d A",ic2r,ic2i,ic2m,ic2a);
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EX1_20.sce
clear; clc; printf("\nEx1.20\n"); //page no.-33 //given a=2.9*10^-10;......//lattice constant in m M=55.85;........//atomic wt. of Ge N=6.02*10^26;....//avagadro no. rho=7870;........//density in Kg/m^3 n=(a^3*rho*N)/M........//no. of atoms per unit cell printf("\nNo. of atoms per unit cell is 2 \n");
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Ex2_14.sce
clc //Chapter2 //Ex_2.14 //Given Xd=0.15 p_c=4*10^-8 //ohm*m p_eff=p_c((1+0.5*Xd)/(1-Xd)) disp(p_eff,"Effective resistivity in ohm m is") // change in the answer due to coding
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@relation led7digit @attribute Led1 real[0.0,1.0] @attribute Led2 real[0.0,1.0] @attribute Led3 real[0.0,1.0] @attribute Led4 real[0.0,1.0] @attribute Led5 real[0.0,1.0] @attribute Led6 real[0.0,1.0] @attribute Led7 real[0.0,1.0] @attribute number{0,1,2,3,4,5,6,7,8,9} @inputs Led1,Led2,Led3,Led4,Led5,Led6,Led7 @outputs number @data 1 1 2 2 2 2 5 6 9 9 5 6 7 1 8 6 8 8 0 0 1 1 4 4 1 1 2 2 9 9 3 4 3 9 6 5 0 8 1 1 2 2 2 2 3 9 7 2 8 0 9 4 0 0 4 4 5 6 6 6 7 1 7 1 3 3 4 4 5 9 5 6 6 6 7 1 8 6 0 6 0 0 3 9 4 4 4 4 5 6 6 6 7 1 8 6 9 9 9 6
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idst1.sci
function y = idst1(x,varargin) //This function computes the inverse type I discrete sine transform. //Calling Sequence //Y = idst(X) //Y = idst(X, N) //Parameters //X: Matrix or integer //N: If N is given, then X is padded or trimmed to length N before computing the transform. //Description //This function computes the inverse type I discrete sine transform of Y. If N is given, then Y is padded or trimmed to length N before computing the transform. If Y is a matrix, compute the transform along the columns of the the matrix. //Examples //idst([1,3,6]) //ans = // 3.97487 -2.50000 0.97487 funcprot(0); rhs=argn(2); if(rhs<1 | rhs>2) then error("Wrong number of input arguments."); end select(rhs) case 1 then y=callOctave("idst",x); case 2 then y=callOctave("idst",x,varargin(1)); end endfunction
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//Ex:10.9 clc; clear; close; Br=20*10^6;// data rate in b/s c=3*10^8;// speed of light in m/s y=86*10^-9;// wavelength in m dy=30*10^-9;// spectral width in m X=0.024; Tb=1/Br; Lmax=(0.35*Tb*c*y)/(dy*X);// material dispersion limited transmission distance for RZ coding in m printf("The material dispersion limited transmission distance =%d m", Lmax);
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pathname=get_absolute_file_path('14_2.sce') filename=pathname+filesep()+'14_2data.sci' exec(filename) clear ax=Rh/(W/g);//horizontal deceleration ay=(Rv-W)/(W/g);//vertical deceleration Ialpha=Rv*Sh +Rh*Sv; alpha=(Ialpha*10^6)/Icg; t=v0/ay; omega=alpha*t; printf("\nhorizontal reaction force: %f kN",W*ax/g); printf("\nvertical reaction force: %f kN",W*ay/g); printf("\nα: %f rad/s^2",alpha); printf("\nt: %f s",t); printf("\nω: %f rad/s",omega);
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10_7.sce
//To find diameter of hand wheel clc //Given: d=50,p=12.5,D=60,R=D/2 //mm W=10*1000,P1=100 //N mu=0.15,mu1=0.18 //Solution: //Calculating the helix angle alpha=atan(p/(%pi*d)) //radians //Calculating the tangential force required at the circumference of the screw phi=atan(mu) //Limiting angle of friction, radians P=W*tan(alpha+phi) //N //Calculating the total torque required to turn the hand wheel T=P*d/2+mu1*W*R //N-mm //Calculating the diameter of the hand wheel D1=T/(2*P1*1000)*2 //m //Results: printf("\n\n Diameter of the hand wheel, D1 = %.3f m.\n\n",D1)
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// Example 3_6 clc;funcprot(0); // Given data T=100;// The torque in N.m n=3000;// rpm // Calculation omega=n*(2*%pi)*(1/60);// rad/s W=T*omega;// The power in W Hp=W/746;// The horse power in hp printf("\nThe horse power delivered,Hp=%2.1f hp",Hp);
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clc; mC=1; mO=3; mN=(3*79/21); Tar=mC+mO+mN; p1=1.013*10^5; R=8.3145*10^3; T=338; V=Tar*R*T/p1; Vr=V/[(2*12)+6+16]; disp(Vr,"Volume of reactants per kilogram of fuel:"); //part II mCO2=2; mH2O=3; mN2=(3*79/21); Tap=mCO2+mH2O+mN2; T=393; p=10^5; V=Tap*R*T/p1; Vr=V/[(2*12)+6+16]; disp(Vr,"Volume of products per kg of fuel is:");
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clc,clear printf('Example 3.15\n\n') V=250 R_sh=275,R_a=0.8 //resistance of shunt field and amature I_L0=3.91 //load current I_sh=V/R_sh I_a0= I_L0 - I_sh constant_losses= V*I_L0 -R_a*(I_a0)^2 //as a generator P_out=10*10^3 I_L=P_out/V I_a = I_L + I_sh field_cu_loss=R_sh*(I_sh)^2 //field copper loss arm_cu_loss= R_a*(I_a)^2 //armature copper loss eta_gen = 100 *(P_out/(P_out+constant_losses + field_cu_loss+ arm_cu_loss)) //efficiency as generator printf('Efficiency as a generator = %.2f percent\n',eta_gen) //as a motor P_in=10*10^3 //at V=250 I_L=P_in/V I_a=I_L - I_sh field_cu_loss=R_sh*(I_sh)^2 //field copper loss arm_cu_loss= R_a*(I_a)^2 //armature copper loss eta_m = 100 *((P_in-(constant_losses + field_cu_loss+ arm_cu_loss))/(P_in)) //efficiency as motor printf('Efficiency as a motor = %.2f percent',eta_m)
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clear; clc; par1=['ab','cde','fh','gi']; //initial partitions par1 par2=['abc','de','fg','hi']; //partition 2 //par=par1+par2; //lub-lower upper bound par_lub=['abcde','fghi']; disp(par_lub); //par=par1.par2 //glb-greatest lower bound par_glb=['ab','c','de','f','g','h','i']; disp(par_glb);
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//Part A Chapter 1 Example 1 clc; clear; close; format('v',8); rho=13550;//kg/m^3 g=9.78;//m/s^2 h=30*10^-2;//m //Pressure Difference P_diff=rho*g*h;//Pa disp("Pressure difference = "+string(P_diff)+" pa");
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function mdaqBlockDelete(block_name) if argn(2) < 1 then mprintf("Description:\n"); mprintf("\tDeletes MicroDAQ user block\n"); mprintf("Usage:\n"); mprintf("\tmdaqBlockDelete(block_name);\n") return; end mprintf("WARNING: This function will remove all files related to ''%s'' block (including C source).\n", block_name); opt = input(" Are you sure? [y/n]: ", "string"); if opt <> 'y' & opt <> 'Y' then return; end //Convert name name_converted = convstr(block_name,'l'); name_converted = strsubst(name_converted, ' ', '_'); name_converted = 'mdaq_' + name_converted; // Delete from macros macrosPath = pathconvert(mdaqToolboxPath()+'macros/user_blocks/'); mdelete(macrosPath+name_converted+'.sci'); mdelete(macrosPath+name_converted+'_sim.sci'); mdelete(macrosPath+name_converted+'.bin'); mdelete(macrosPath+name_converted+'_sim.bin'); // Delete images imagesPath = pathconvert(mdaqToolboxPath()+'images/'); mdelete(imagesPath+'gif'+filesep()+name_converted+'.gif'); mdelete(imagesPath+'h5'+filesep()+name_converted+'.sod'); mdelete(imagesPath+'svg'+filesep()+name_converted+'.svg'); // Delete code srcPath = pathconvert(mdaqToolboxPath()+'src/c/userlib/'); backUpPath = mdaqToolboxPath()+pathconvert("src\c\userlib\.removed_code"); try if isdir(backUpPath) == %F then mkdir(backUpPath); end copyfile(srcPath+name_converted+'.c', backUpPath); catch end mdelete(srcPath+name_converted+'.c'); mdelete(srcPath+name_converted+'.o'); mprintf("Block has been deleted. Please restart Scilab software.\n"); endfunction
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Dmux8Way.tst
load DMux8Way.hdl; output-file DMux8Way.out, compare-to DMux8Way.cmp, output-list sel%B1.3.1 in a b c d e f g h; set sel %B000, set in 0, eval, output; set sel %B001, set in 0, eval, output; set sel %B010, set in 0, eval, output; set sel %B011, set in 0, eval, output; set sel %B100, set in 0, eval, output; set sel %B101, set in 0, eval, output; set sel %B110, set in 0, eval, output; set sel %B111, set in 0, eval, output; set sel %B000, set in 1, eval, output; set sel %B001, set in 1, eval, output; set sel %B010, set in 1, eval, output; set sel %B011, set in 1, eval, output; set sel %B100, set in 1, eval, output; set sel %B101, set in 1, eval, output; set sel %B110, set in 1, eval, output; set sel %B111, set in 1, eval, output;
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/2_año/MN/p2.sce
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jfarizano/LCC
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refs/heads/master
2022-11-15T14:46:36.171561
2022-11-10T21:15:13
2022-11-10T21:15:13
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sce
p2.sce
function r = raicesRobustas(p) c = coeff(p, 0); b = coeff(p, 1); a = coeff(p, 2); disc = b^2 - 4*a*c if disc < 0 then return [%nan, %nan] end if b < 0 then r(1) = 2*c / (-b + sqrt(disc)) r(2) = (-b + sqrt(disc))/(2*a) else if b > 0 then r(1) = (-b - sqrt(disc))/(2*a) r(2) = 2*c / (-b - sqrt(disc)) else r(1) = sqrt(c/a) r(2) = -r(1) end end endfunction function [x, d] = horner(p, x0) coeffs = coeff(p) n = length(coeffs) x = 0 d = 0 for i = n:-1:1 x = coeffs(i) + x*x0 if i > 1 then d = coeffs(i) * (i-1) + d*x0 end end endfunction function x = derivar(f,v,n,h) if (n ==0) then x = f(v) else x = (derivar(f,v+h,n-1,h)-derivar(f,v,n-1,h))/h end endfunction function x = derivarExtra(f,v,n,h) deff("y=D0F(x)", "y="+f) for i = 1:1:n-1 deff("y=D"+string(i)+"F(x)", "y=(D"+string(i-1)+"F(x+h)-D"+string(i-1)+"F(x))/h") end deff ("y=DnF(x)", "y=(D"+string(n-1)+"F(x+h)-D"+string(n-1)+"F(x))/h") x = DnF(v) endfunction function x = derivarMultiple(f,v,n,h) deff("y=D0F(x)", "y="+f) for i = 1:1:n deff("y=D"+string(i)+"F(x)", "y=(D"+string(i-1)+"F(x+h)-D"+string(i-1)+"F(x))/h") x(i) = evstr("D" + string(i) +"F(v)") end endfunction function x = taylor(f, n, a, v, h) deff("y=F0(x)", "y="+f) x = F0(a) factorial = 1 derivadas = derivarMultiple(f, a, n, h) for i = 1:1:n factorial = factorial * n x = x + (derivadas(i) * ((v - a) ** i))/factorial end endfunction
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/2489/CH11/EX11.2/11_2.sce
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[]
no_license
FOSSEE/Scilab-TBC-Uploads
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7bc77cb1ed33745c720952c92b3b2747c5cbf2df
refs/heads/master
2020-04-09T02:43:26.499817
2018-02-03T05:31:52
2018-02-03T05:31:52
37,975,407
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11_2.sce
clc //Intitalisation of variables clear T= 500 //C Kp= 1.43*10^-5 //atm R= 1.987 //cal //CALCULATIONS dF= -2.303*R*(273+T)*log10(Kp) //RESULTS printf ('dF = %.f cal ',dF+3)
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/control-system/step_response1.sce
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omrastogi/Digital-Signal-Processing
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refs/heads/main
2023-01-03T13:54:45.554127
2020-11-02T05:40:13
2020-11-02T05:40:13
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sce
step_response1.sce
clc; s = poly(0,'s'); num1 = 2; den1 = s+3; s1 = syslin('c',num1,den1); num2 = 4; den2 = s^2+2*s+4; s2 = syslin('c',num2,den2); num3 = 1; den3 = s; s3 = syslin('c',num3,den3); s4 = s2+s3; s5 = s1*s4; disp(s5); t = 0 : 0.01 : 10; plot(t,s5);
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/1775/CH3/EX3.3/Chapter3_Example3.sce
d3842170637ed1482884691635373e608ec48269
[]
no_license
FOSSEE/Scilab-TBC-Uploads
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2020-04-09T02:43:26.499817
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sce
Chapter3_Example3.sce
//Chapter-3, Illustration 3, Page 141 //Title: Internal Combustion Engines //============================================================================= clc clear //INPUT DATA n=6;//No. of cylinders d=0.61;//Diameter in m L=1.25;//Stroke in m N=2;//No.of revolutions per second m=340;//mass of fuel oil in kg CV=44200;//Calorific value in kJ/kg T=108;//Torque in kN-m imep=775;//Indicated mean efective pressure in kN/(m^2) //CALCULATIONS IP=(imep*L*3.1415*(d^2)*N)/(8);//Indicated power in kW TotalIP=(n*IP);//Total indicated power in kW BP=(2*3.1415*N*T);//Brake power in kW PI=(m*CV)/3600;//Power input in kW nB=(BP/PI)*100;//Brake thermal efficiency bmep=(BP*8)/(n*L*3.1415*(d^2)*2);//Brake mean effective pressure in kN/(m^2) nM=(BP/TotalIP)*100;//Mechanical efficiency bsfc=m/BP;//Brake specific fuel consumption in kg/kWh //OUTPUT mprintf('Total Indicated Power is %3.1f kW \n Brake Power is %3.1f kW \n Brake thermal efficiency is %3.1f percent \n Brake mean effective pressure is %3.1f kN/(m^2) \n Mechanical efficiency is %3.1f percent \n Brake specific fuel consumption is %3.3f kg/kW.h',TotalIP,BP,nB,bmep,nM,bsfc) //==============================END OF PROGRAM=================================