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Now that we have the dataset loaded, let's build a model.We will create training and test sets to evaluate the model's performance. In this case we will use the RandomSplitter(). DeepChem offers a number of other splitters such as the ScaffoldSplitter, which will divide the dataset by chemical scaffold or the ButinaSp...
splitter = dc.splits.RandomSplitter()
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MIT
Chapter11/chapter_11_02_erk2_graph_conv.ipynb
deepchem/DeepLearningLifeSciences
With the dataset split, we can train a model on the training set and test that model on the validation set. At this point we can define some metrics and evaluate the performance of our model. In this case our dataset is unbalanced, we have a small number of active compounds and a large number of inactive compounds. Giv...
metrics = [dc.metrics.Metric(dc.metrics.matthews_corrcoef, np.mean)]
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MIT
Chapter11/chapter_11_02_erk2_graph_conv.ipynb
deepchem/DeepLearningLifeSciences
In order to evaluate the performance of our moldel, we will perform 10 folds of cross valiation, where we train a model on the training set and validate on the validation set.
training_score_list = [] validation_score_list = [] transformers = [] cv_folds = 10 for i in tqdm(range(0,cv_folds)): model = generate_graph_conv_model() train_dataset, valid_dataset, test_dataset = splitter.train_valid_test_split(dataset) model.fit(train_dataset) train_scores = model.evaluate(train_dat...
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MIT
Chapter11/chapter_11_02_erk2_graph_conv.ipynb
deepchem/DeepLearningLifeSciences
To visualize the preformance of our models on the training and test data, we can make boxplots of the models' performance.
sns.boxplot(x=["training"]*cv_folds+["validation"]*cv_folds,y=training_score_list+validation_score_list);
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MIT
Chapter11/chapter_11_02_erk2_graph_conv.ipynb
deepchem/DeepLearningLifeSciences
It is also useful to visualize the result of our model. In order to do this, we will generate a set of predictions for a validation set.
pred = [x.flatten() for x in model.predict(valid_dataset)] pred
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MIT
Chapter11/chapter_11_02_erk2_graph_conv.ipynb
deepchem/DeepLearningLifeSciences
**The results of predict on a GraphConv model are returned as a list of lists. Is this the intent? It doesn't seem consistent across models. RandomForest returns a list. For convenience, we will put our predicted results into a Pandas dataframe.**
pred_df = pd.DataFrame(pred,columns=["neg","pos"])
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MIT
Chapter11/chapter_11_02_erk2_graph_conv.ipynb
deepchem/DeepLearningLifeSciences
We can easily add the activity class (1 = active, 0 = inactive) and the SMILES string for our predicted moleculesto the dataframe. __Is the moleculed id retained as part of the DeepChem dataset? I can't find it__
pred_df["active"] = [int(x) for x in valid_dataset.y] pred_df["SMILES"] = valid_dataset.ids pred_df.head() pred_df.sort_values("pos",ascending=False).head(25) sns.boxplot(x=pred_df.active,y=pred_df.pos)
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MIT
Chapter11/chapter_11_02_erk2_graph_conv.ipynb
deepchem/DeepLearningLifeSciences
The performance of our model is very good, we can see a clear separation between the active and inactive compounds. It appears that only one of our active compounds receieved a low positive score. Let's look more closely.
false_negative_df = pred_df.query("active == 1 & pos < 0.5").copy() PandasTools.AddMoleculeColumnToFrame(false_negative_df,"SMILES","Mol") false_negative_df false_positive_df = pred_df.query("active == 0 & pos > 0.5").copy() PandasTools.AddMoleculeColumnToFrame(false_positive_df,"SMILES","Mol") false_positive_df
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MIT
Chapter11/chapter_11_02_erk2_graph_conv.ipynb
deepchem/DeepLearningLifeSciences
Now that we've evaluated our model's performance we can retrain the model on the entire dataset and save it.
model.fit(dataset)
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MIT
Chapter11/chapter_11_02_erk2_graph_conv.ipynb
deepchem/DeepLearningLifeSciences
Exercise 01 - Syntax, Variables and Numbers Welcome to your first set of Python coding problems! **Notebooks** are composed of blocks (called "cells") of text and code. Each of these is editable, though you'll mainly be editing the code cells to answer some questions.To get started, try running the code cell below (by...
print("You've successfully run some Python code") print("Congratulations!")
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MIT
python-for-data/Ex01 - Syntax, Variables and Numbers.ipynb
Quan030994/atom-assignments
Try adding another line of code in the cell above and re-running it. Now let's get a little fancier: Add a new code cell by clicking on an existing code cell, hitting the `escape` key *(turn to command mode)*, and then hitting the `a` or `b` key. - The `a` key will add a cell above the current cell.- The `b` adds a c...
# Create a variable called color with an appropriate value on the line below # (Remember, strings in Python must be enclosed in 'single' or "double" quotes) color = 'blue'
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MIT
python-for-data/Ex01 - Syntax, Variables and Numbers.ipynb
Quan030994/atom-assignments
1. Simple Arithmetic OperationComplete the code below. In case it's helpful, here is the table of available arithmatic operations:| Operator | Name | Description ||--------------|----------------|--------------------------------------------------------|| ``a + b...
pi = 3.14159 # approximate diameter = 3 # Create a variable called 'radius' equal to half the diameter radius = 3/2 # Create a variable called 'area', using the formula for the area of a circle: pi times the radius squared area = pi * radius**2 area
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MIT
python-for-data/Ex01 - Syntax, Variables and Numbers.ipynb
Quan030994/atom-assignments
**Results**:- Area = 7.0685775 2. Variable ReassignmentAdd code to the following cell to swap variables `a` and `b` (so that `a` refers to the object previously referred to by `b` and vice versa).
# If you're curious, these are examples of lists. We'll talk about # them in depth a few lessons from now. For now, just know that they're # yet another type of Python object, like int or float. a = [1, 2, 3] b = [3, 2, 1] ###################################################################### # Your code goes here. ...
a = [3, 2, 1] b = [1, 2, 3]
MIT
python-for-data/Ex01 - Syntax, Variables and Numbers.ipynb
Quan030994/atom-assignments
3. Order of Operationsa) Add parentheses to the following expression so that it evaluates to 1.*Hint*: Following its default "**PEMDAS**"-like rules for order of operations, Python will first divide 3 by 2, then subtract the result from 5. You need to add parentheses to force it to perform the subtraction first.
(5 - 3) // 2
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MIT
python-for-data/Ex01 - Syntax, Variables and Numbers.ipynb
Quan030994/atom-assignments
Questions, like this one, marked a spicy pepper are a bit harder. Don't feel bad if you can't get these.b) 🌶️ Add parentheses to the following expression so that it evaluates to **0**.
8 - (3 * 2) - (1 + 1)
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MIT
python-for-data/Ex01 - Syntax, Variables and Numbers.ipynb
Quan030994/atom-assignments
4. Your TurnAlice, Bob and Carol have agreed to pool their Halloween candies and split it evenly among themselves.For the sake of their friendship, any candies left over will be smashed. For example, if they collectivelybring home 91 candies, they'll take 30 each and smash 1.Write an arithmetic expression below to cal...
# Variables representing the number of candies collected by Alice, Bob, and Carol alice_candies = 121 bob_candies = 77 carol_candies = 109 # Your code goes here! Replace the right-hand side of this assignment with an expression candies_smash = (alice_candies + bob_candies + carol_candies) % 3 candies_smash # involving...
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MIT
python-for-data/Ex01 - Syntax, Variables and Numbers.ipynb
Quan030994/atom-assignments
『本次練習內容』 運用這幾天所學觀念搭建一個CNN分類器 『本次練習目的』 熟悉CNN分類器搭建步驟與原理 學員們可以嘗試不同搭法,如使用不同的Maxpooling層,用GlobalAveragePooling取代Flatten等等
from keras.models import Sequential from keras.layers import Convolution2D from keras.layers import MaxPooling2D from keras.layers import Flatten from keras.layers import Dense from keras.layers import Dropout from keras.layers import BatchNormalization from keras.layers import Activation import keras.utils from keras...
Model: "sequential_1" _________________________________________________________________ Layer (type) Output Shape Param # ================================================================= conv2d_1 (Conv2D) (None, 30, 30, 16) 448 __________________________________...
MIT
Day015_Cifar_HW.ipynb
semishen/DL-CVMarathon
預測新圖片,輸入影像前處理要與訓練時相同 ((X-mean)/(std+1e-7) ):這裡的mean跟std是訓練集的 維度如下方示範
index = 50 input_example = x_test[index].reshape(1,32,32,3) # input_example.shape input_example=(input_example-mean_train)/(std_train+1e-7) print(classifier.predict(input_example)) print(y_test[index])
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MIT
Day015_Cifar_HW.ipynb
semishen/DL-CVMarathon
Transmission
%matplotlib inline import numpy as np np.seterr(divide='ignore') # Ignore divide by zero in log plots from scipy import signal import scipy.signal from numpy.fft import fft, fftfreq import matplotlib.pyplot as plt #import skrf as rf # pip install scikit-rf if you want to run this one
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
First, let's set up a traditional, full-precision modulator and plot the spectrum of that as a baseline
def prbs(n=0, taps=[]): state = [1]*n shift = lambda s: [sum([s[i] for i in taps]) % 2] + s[0:-1] out = [] for i in range(2**n - 1): out.append(state[-1]) state = shift(state) return out prbs9 = lambda: prbs(n=9, taps=[4,8]) def make_carrier(freq=None, sample_rate=None, samples=None...
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
Now let's look at the FFT of this...
sample_rate = 6e9 modulated = modulate_gmsk(prbs9(), sample_rate=sample_rate) fftm = np.abs(fft(modulated)) fftm = fftm/np.max(fftm) fftbins = fftfreq(len(modulated), 1/sample_rate) plt.figure(figsize=(10,6)) plt.plot(fftbins, 10*np.log10(fftm)) plt.gca().set_ylim(-40, 0)
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
This is clean (as one would expect), now let's see what happens if we reduce things to 1-bit of precision by just rounding The Naive Approach (Rounding)
sample_rate=5e9 modulates_5g = modulated = np.sign(modulate_gmsk(prbs9(), sample_rate=sample_rate)) fftm = np.abs(fft(modulated)) fftm = fftm/np.max(fftm) fftbins = fftfreq(len(modulated), 1/sample_rate) plt.figure(figsize=(10,6)) plt.plot(fftbins, 10*np.log10(fftm)) plt.gca().set_ylim(-40, 0) plt.gca().set_xlim(0,...
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
_Oof_ this is not pretty. What's happening here is that (I think) the aliases are mixing with each other to produce these interference paterns. In this case, it looks like the big subharmonics are spaced about 200Mhz which makes sense given the alias of 2.402ghz at 2.698ghz when sampling at 2.5ghz.
sample_rate = 6e9 modulated_6g = modulated = np.sign(modulate_gmsk(prbs9(), sample_rate=sample_rate)) fftm = np.abs(fft(modulated)) fftm = fftm/np.max(fftm) fftbins = fftfreq(len(modulated), 1/sample_rate) plt.figure(figsize=(10,6)) plt.plot(fftbins, 10*np.log10(fftm)) plt.gca().set_ylim(-40, 0) plt.gca().set_xlim(...
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
Ok, in this case, the alias is at `3 + (3 - 2.402) = 3.6ghz`. The difference between this and 2.402ghz is about 1.2ghz, which looking at the next big peak, looks to be about 1.2ghz, so this makes sense. From this math, we can intuit that it's a good idea for the sample rate to be a whole number multiple of the carrier ...
sample_rate = 2.402e9*4 modulated_4x = modulated = np.sign(modulate_gmsk(prbs9(), sample_rate=sample_rate)) fftm = np.abs(fft(modulated)) fftm = fftm/np.max(fftm) fftbins = fftfreq(len(modulated), 1/sample_rate) plt.figure(figsize=(10,6)) plt.plot(fftbins, 10*np.log10(fftm)) plt.gca().set_ylim(-40, 0) plt.gca().set...
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
There a couple of challenges here, however:1. In order to get the clean(ish) spectrum, we have to clock the output frequency at a rate relative to the carrier frequency. If we only intended to use one frequency, this would be fine but Bluetooth (as an example) hops around frequency constantly by design. This might be d...
# pip install scikit-rf if you want to run this one # Note: running this before we've plotted anything, borks matplotlib import skrf as rf filter2_4 = rf.Network('2_4ghzfilter.s2p') filter2_4.s21.plot_s_db()
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
Hey that's not too far off from data sheet (at least up to 4.4Ghz). To turn this into a filter, we can use the scipy-rf to compute an impulse response which we can then convolve with our input data to see what the filtered output would be:
ts, ms = filter2_4.s21.impulse_response() impulse_response = ms[list(ts).index(0):] impulse_response = impulse_response/np.max(impulse_response) tstep = ts[1] - ts[0] print("Timestep {} seconds, frequency {:e} hz".format(tstep, 1/tstep)) plt.plot(impulse_response) plt.gca().set_xlim(0, 300)
Timestep 3.2641464908425124e-11 seconds, frequency 3.063588e+10 hz
Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
This is great and all but the impulse response is sampled at north of 30ghz (!). Our output serdes runs at around 6ghz so let's resample this to that rate
# Truncate the impulse response so we can get relatively close to 6ghz trunc = impulse_response[:-4] size = int((tstep*(len(trunc) - 1))/(1/6e9) + 1) print(size) impulse_response_6g = scipy.signal.resample(impulse_response, size) plt.plot(impulse_response_6g) plt.gca().set_xlim(0, 50)
274
Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
Not quite as pretty, but it's what we need. Let's verify that this does "the thing" by filtering our 6ghz signal:
sample_rate=6e9 fftm = np.abs(fft(np.convolve(modulated_6g, impulse_response_6g, mode="same"))) fftm = fftm/np.max(fftm) fftbins = fftfreq(len(fftm), 1/sample_rate) plt.figure(figsize=(10,6)) plt.plot(fftbins, 10*np.log10(fftm)) plt.grid(b=True) plt.gca().set_ylim(-40, 0) plt.gca().set_xlim(0, 3e9)
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
This looks better, but the passband for my filter is still super wide (hundreds of MHz, not surprising for a 50c filter, I should look at B39242B9413K610 which is a $1 surface acoustic wave filter). We see some nontrivial imaging up to -12db, which is... not great.What to do? Delta Sigma ModulationA way around this is...
def pwm2(sig, k=1.0): z1 = 0.0 z2 = 0.0 out = np.zeros((len(sig,))) for i in range(len(sig)): v = sig[i] - (k*z1 + z2) out[i] = np.sign(v) z2 = z1 z1 = v - out[i] return out
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
To be clear, `pwm2` is replacing `np.sign`
sample_rate = 6e9 modulated = modulate_gmsk(prbs9(), sample_rate=sample_rate) modulatedsd5 = modulated = pwm2(modulated, k=-2.0*np.cos(2.0*np.pi*2.402e9/sample_rate)) fftm = np.abs(fft(np.sign(modulated))) fftm = fftm/np.max(fftm) fftbins = fftfreq(len(modulated), 1/sample_rate) plt.figure(figsize=(10,6)) plt.plot(...
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
Now let's filter this with our output filter
fftm = np.abs(fft(np.convolve(modulatedsd5, impulse_response_6g, mode="same"))) fftm = fftm/np.max(fftm) fftbins = fftfreq(len(fftm), 1/sample_rate) plt.figure(figsize=(10,6)) plt.plot(fftbins, 10*np.log10(fftm)) plt.grid(b=True) plt.gca().set_ylim(-40, 0) plt.gca().set_xlim(0, 3e9) plt.title("Filtered Second Order D...
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
This is better in the immediate vicinity of our signal. You'll notice on the wikipedia page that we can use increasing filter orders to increase the steepness of the valley around our signal of interest.On one hand this is good, but because our filter is not very good (tm) this actually results in higher peaks than we'...
from pydsm.ir import impulse_response from pydsm.delsig import synthesizeNTF, simulateDSM, evalTF from pydsm.delsig import dbv, dbp from pydsm.NTFdesign import quantization_noise_gain from pydsm.NTFdesign.legacy import q0_from_filter_ir from pydsm.NTFdesign.weighting import ntf_fir_from_q0 H_inf = 1.6 # This is out of ...
Calling CVXOPT ... pcost dcost gap pres dres k/t 0: 1.3378e-17 -1.0000e+00 2e+02 8e+00 1e+01 1e+00 1: -3.2534e-02 4.5237e-02 1e+01 1e+00 2e+00 4e-01 2: 1.6301e-01 1.5136e-01 2e+00 3e-01 3e-01 5e-02 3: 1.3047e-01 1.2416e-01 5e-01 9e-02 1e-01 2e-02 4: 1.3111e-01 1.275...
Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
Let's see how well we did. Anecdotally, this is not a _great_ solution (likely constrained by the low oversampling) but I'd wager this is because the oversampling rate is super low.
# Take the frequency response samples = filter2_4.s21.s_db[:,0,0] # Normalize the samples ff = filter2_4.f/6e9 # Compute frequency response data resp_opti = evalTF(ntf_opti, np.exp(1j*2*np.pi*ff)) # Plot the output filter, plt.figure() plt.plot(ff*6e9, dbv(resp_opti), 'r', label="Optimal NTF") plt.plot(ff*6e9, sampl...
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
Ok, so it's not amazing but definitely an improvement. But now that we've got this monstrous 49 coefficient NTF, how do we modulate with it?Fortunately we have the pydsm to the rescue!
sample_rate = 6e9 modulated = modulate_gmsk(prbs9(), sample_rate=sample_rate) xx_opti = simulateDSM(modulated, ntf_opti) fftm = np.abs(fft(np.convolve(xx_opti[0], impulse_response_6g, mode="same"))) fftm = fftm/np.max(fftm) fftbins = fftfreq(len(fftm), 1/sample_rate) plt.figure(figsize=(10,6)) plt.plot(fftbins, 10*np...
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
Ok, so we've basically "filled in the valley" with the peaks from eithe sides. We've cut the max spurs down by about 3db. Not amazing, but not bad!After looking around at SAW filters I realized how impressive they can be in this frequency rance, so I tried to order one (CBPFS-2441) and try with that. Unfortunately, the...
import csv from scipy.interpolate import interp1d traced = np.array([(float(f), float(d)) for f,d in csv.reader(open('saw_filter_traced.csv'))]) # Interpolate to 600 equally spaced points (this means 1200 total, so 1200 * 5MHz -> 6GHz sampling rate) x = traced[:,0] y = -1*traced[:,1] f = interp1d(x, y) x = np.array(n...
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
Let's look at the impulse respponse quickly
impulse = np.fft.ifft(y_orig) impulse_trunc = impulse[:300] plt.plot(np.real(impulse_trunc))
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
**Update:** The filter finally arrived and I can characterize it, as shown below...(the remaining code uses the measured filter response rather than the one trace from the image)
sawfilter = rf.Network('crysteksawfilter.s2p') sawfilter.s21.plot_s_db() filter2_4.s21.plot_s_db() ts, ms = sawfilter.s21.impulse_response() impulse_response = ms[list(ts).index(0):] impulse_response = impulse_response/np.max(impulse_response) tstep = ts[1] - ts[0] print("Timestep {} seconds, frequency {:e} hz".format(...
Timestep 4.283537554093063e-11 seconds, frequency 2.334519e+10 hz
Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
Wow that is a fair bit sharper.
H_inf = 1.5 q0 = q0_from_filter_ir(49, np.real(impulse_response_6g)) ntf_opti = ntf_fir_from_q0(q0, H_inf=H_inf) # Take the frequency response #samples = 10*np.log10(y) # Normalize the samples #ff = x*1e6/6e9 # Take the frequency response samples = sawfilter.s21.s_db[:,0,0] # Normalize the samples ff = sawfilter.f/6e9...
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
Wow, the baseline noise level has dropped by almost 10db! Impressive! Symbol DictionariesNow that we've figured out how much noise we can stifle with this setup, we can begin to design our transmitter.Now you may notice that the above noise transfer function filter is... quite expensive, clocking in at 51 coefficients...
carrier_freq = 2.402e9 sample_rate = 6e9 symbol_rate = 1e6 samples_per_symbol = int(sample_rate/symbol_rate) # Used to test that we've mapped things correctly. # Note that this returns the phase angle, not the output bits def demodulate_gmsk(sig, phase_offset=0): I = make_carrier(freq=carrier_freq, sample_rate=sam...
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
With these established, let's concatenate a few symbols together, demodulate to phase angle and make sure things look nice and smooth
def sim(out): carrier=2.402e9 I = make_carrier(freq=carrier, sample_rate=sample_rate, samples=len(out), phase=0) Q = make_carrier(freq=carrier, sample_rate=sample_rate, samples=len(out), phase=np.pi/2) sos = signal.butter(2, symbol_rate, 'low', fs=sample_rate, output='sos') rx_baseband = signal.sosfilt(sos...
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
Now, in order to synthesize this, we need a bit more logic to map between a bit stream and its respective symbols.Note that there is additional state (i.e. the current phase offset) that factors into the symbol encoding beyond just the symbol value itself, which makes things a bit more complicate than most other forms ...
idx = { '000': 0, '111': 1, '001': 2, '011': 3, '010': 4, '101': 5, '110': 6, '100': 7 } start_q = [ [3, 2, 3, 2, 2, 3, 2, 3], [0, 3, 0, 3, 3, 0, 3, 0], [1, 0, 1, 0, 0, 1, 0, 1], [2, 1, 2, 1, 1, 2, 1, 2] ] def encode(bitstream): out = np.zeros((len(bitstream)*samples_per_symbol,)) q = 0 ...
[22, 21, 20, 21, 20, 21, 20, 21, 20, 23, 10, 12, 13, 12, 15, 2, 4, 7, 24, 16, 8, 2, 4, 7, 26, 27, 6, 5, 3, 9, 22, 21, 20, 23, 8, 2, 3, 9, 22, 23, 8, 0, 24, 18, 19, 25, 6, 7, 26, 28, 29, 27, 1, 14, 15, 2, 4, 7, 24, 18, 19, 30, 31, 16, 8, 2, 3, 14, 15, 2, 3, 9, 17, 30, 31, 18, 19, 25, 6, 5, 3, 14, 15, 2, 3, 14, 13, 12, 1...
Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
As a reminder, the dictionary is really just one bit of precision:
dictionary[0][:100]
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
Let's demodulate the encoded bits to check that things make sense (note that the filtering will delay the output a bit in time, but it demodulates correctly)
def demodulate_gmsk(sig): carrier_freq=2.402e9 I = make_carrier(freq=carrier_freq, sample_rate=sample_rate, samples=len(sig), phase=0) Q = make_carrier(freq=carrier_freq, sample_rate=sample_rate, samples=len(sig), phase=np.pi/2) # Mix down to (complex) baseband down = sig*I + 1j*sig*Q # Create...
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
The library used to generate the NTF filter uses a copyleft license, so rather than integrate that into the code, we save out the resulting symbol waveforms and use those directly.
np.save('../data/gmsk_2402e6_6e9.npy', dictionary)
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Apache-2.0
research/Transmission.ipynb
goran-mahovlic/onebitbt
Pre-processing pipeline for spikeglx sessions, zebra finchBird z_w12m7_20- For every run in the session: - Load the recordings - Extract wav chan with micrhopohone and make a wav chan with the nidq syn signal - Get the sync events for the nidq sync channel - Do bout detection In another notebook, bout detection is cu...
%matplotlib inline import os import glob import logging import pickle import numpy as np import pandas as pd from scipy.io import wavfile from scipy import signal import traceback import warnings from matplotlib import pyplot as plt from importlib import reload logger = logging.getLogger() handler = logging.StreamHan...
2021-10-19 11:58:34,081 root INFO all modules loaded
MIT
notebooks/pipeline/z_w12m7_20/sglx_preprocess-z_w12m7_20-multisess-pouli.ipynb
zekearneodo/ceciestunepipe
Session parameters and raw files list all the sessions for this bird
bird = 'z_w12m7_20' all_bird_sess = et.list_sessions(bird) logger.info('all sessions for bird are {}'.format(all_bird_sess))
2021-10-19 11:58:35,383 root INFO all sessions for bird are ['2020-11-04', '2020-11-05', '2020-11-06']
MIT
notebooks/pipeline/z_w12m7_20/sglx_preprocess-z_w12m7_20-multisess-pouli.ipynb
zekearneodo/ceciestunepipe
set up bird and sessions parametersthis will define:- locations of files (for the bird)- signals and channels to look for in the metadata of the files and in the rig.json parameter file: Note that this have to exist in all of the sessions that will be processed- 'sess' is unimportant here, but it comes handy if there ...
reload(et) # for one example session sess_par = {'bird': 'z_w12m7_20', 'sess': '2020-11-04', 'probes': ['probe_0'], #probes of interest 'mic_list': ['microphone_0'], #list of mics of interest, by signal name in rig.json 'sort': 4, #label for this sort instance } ...
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MIT
notebooks/pipeline/z_w12m7_20/sglx_preprocess-z_w12m7_20-multisess-pouli.ipynb
zekearneodo/ceciestunepipe
list all the epochs in a session, to check that it is finding what it has to find
sess_epochs = et.list_sgl_epochs(sess_par) sess_epochs
2021-10-19 11:58:37,438 ceciestunepipe.file.bcistructure INFO {'folders': {'bird': '/mnt/sphere/speech_bci/raw_data/z_w12m7_20', 'raw': '/mnt/sphere/speech_bci/raw_data/z_w12m7_20/2020-11-04', 'sglx': '/mnt/sphere/speech_bci/raw_data/z_w12m7_20/2020-11-04/sglx', 'kwik': '/experiment/z_w12m7_20/sglx/kwik/2020-11-04'...
MIT
notebooks/pipeline/z_w12m7_20/sglx_preprocess-z_w12m7_20-multisess-pouli.ipynb
zekearneodo/ceciestunepipe
define pre-processing steps for each epoch and for the session
def preprocess_run(sess_par, exp_struct, epoch): # get the recordings logger.info('PREPROCESSING sess {} | epoch {}'.format(sess_par['sess'], epoch)) logger.info('getting extractors') sgl_exp_struct = et.sgl_struct(sess_par, epoch) run_recs_dict, run_meta_files, files_pd, rig_dict = pre.load_sglx_re...
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MIT
notebooks/pipeline/z_w12m7_20/sglx_preprocess-z_w12m7_20-multisess-pouli.ipynb
zekearneodo/ceciestunepipe
Process multiple sessions
sess_list = all_bird_sess # fist implant, right hemisphere sess_list = ['2020-11-04', '2020-11-05', '2020-11-06'] all_sess_dict = {} for one_sess in sess_list[:]: sess_par['sess'] = one_sess preprocess_session(sess_par) sess_par # Search bouts
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MIT
notebooks/pipeline/z_w12m7_20/sglx_preprocess-z_w12m7_20-multisess-pouli.ipynb
zekearneodo/ceciestunepipe
search bouts for those sessions
from ceciestunepipe.util.sound import boutsearch as bs from ceciestunepipe.util import wavutil as wu from joblib import Parallel, delayed import pickle import sys reload(bs) def sess_file_id(f_path): n = int(os.path.split(f_path)[1].split('-')[-1].split('.wav')[0]) return n def get_all_day_bouts(sess_par: di...
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MIT
notebooks/pipeline/z_w12m7_20/sglx_preprocess-z_w12m7_20-multisess-pouli.ipynb
zekearneodo/ceciestunepipe
debug debug search_bout
## look for a single file sess = sess_list[0] exp_struct = et.get_exp_struct(sess_par['bird'], sess, ephys_software='sglx') source_folder = exp_struct['folders']['derived'] wav_path_list = et.get_sgl_files_epochs(source_folder, file_filter='*wav_mic.wav') wav_path_list.sort() logger.info('Found {} files'.format(len(wa...
2021-09-22 15:13:45,924 ceciestunepipe.util.sound.boutsearch INFO Getting bouts for long file /mnt/sphere/speech_bci/derived_data/s_b1253_21/2021-06-14/sglx/0712_g0/wav_mic.wav
MIT
notebooks/pipeline/z_w12m7_20/sglx_preprocess-z_w12m7_20-multisess-pouli.ipynb
zekearneodo/ceciestunepipe
Telescopes: Tutorial 5This notebook will build on the previous tutorials, showing more features of the `PsrSigSim`. Details will be given for new features, while other features have been discussed in the previous tutorial notebook. This notebook shows the details of different telescopes currently included in the `PsrS...
# import some useful packages import numpy as np import matplotlib.pyplot as plt %matplotlib inline # import the pulsar signal simulator import psrsigsim as pss
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MIT
docs/_static/notebooks/telescopes_tutorial_5.ipynb
LBJ-Wade/PsrSigSim
The Folded SignalHere we will use the same `Signal` definitions that have been used in the previous tutorials. We will again simulate a 20-minute-long observation total, with subintegrations of 1 minute. The other simulation parameters will be 64 frequency channels each 12.5 MHz wide (for 800 MHz bandwidth).We will s...
# Define our signal variables. f0 = 1500 # center observing frequecy in MHz bw = 800.0 # observation MHz Nf = 64 # number of frequency channels # We define the pulse period early here so we can similarly define the frequency period = 0.00457 # pulsar period in seconds for J1713+0747 f_samp = (1.0/period)*2048*10**-6 # ...
Warning: specified sample rate 0.4481400437636761 MHz < Nyquist frequency 1600.0 MHz
MIT
docs/_static/notebooks/telescopes_tutorial_5.ipynb
LBJ-Wade/PsrSigSim
The Pulsar and ProfilesNow we will load the pulse profile as in Tutorial 3 and initialize a single `Pulsar` object.
# First we load the data array path = 'psrsigsim/data/J1713+0747_profile.npy' J1713_dataprof = np.load(path) # Now we define the data profile J1713_prof = pss.pulsar.DataProfile(J1713_dataprof) # Define the values needed for the puslar Smean = 0.009 # The mean flux of the pulsar, J1713+0747 at 1400 MHz from the ATNF p...
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MIT
docs/_static/notebooks/telescopes_tutorial_5.ipynb
LBJ-Wade/PsrSigSim
The ISMHere we define the `ISM` class used to disperse the simulated pulses.
# Define the dispersion measure dm = 15.921200 # pc cm^-3 # And define the ISM object, note that this class takes no initial arguements ism_sim = pss.ism.ISM()
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MIT
docs/_static/notebooks/telescopes_tutorial_5.ipynb
LBJ-Wade/PsrSigSim
Defining TelescopesHere we will show how to use the two predefined telescopes, Green Bank and Arecibo, and the systems accociated with them. We will also show how to define a `telescope` from scratch, so that any current or future telescopes and systems can be simulated. Predefined TelescopesWe start off by showing t...
# Define the Green Bank Telescope tscope_GBT = pss.telescope.telescope.GBT() # Define the Arecibo Telescope tscope_AO = pss.telescope.telescope.Arecibo()
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MIT
docs/_static/notebooks/telescopes_tutorial_5.ipynb
LBJ-Wade/PsrSigSim
Each telescope is made up of one or more `systems` consisting of a `Reciever` and a `Backend`. For the predefined telescopes, the systems for the `GBT` are the L-band-GUPPI system or the 800 MHz-GUPPI system. For `Arecibo` these are the 430 MHz-PUPPI system or the L-band-PUPPI system. One can check to see what these sy...
# Information about the GBT systems print(tscope_GBT.systems) # We can also find out information about a receiver that has been defined here rcvr_LGUP = tscope_GBT.systems['Lband_GUPPI'][0] print(rcvr_LGUP.bandwidth, rcvr_LGUP.fcent, rcvr_LGUP.name)
{'820_GUPPI': (Receiver(820), Backend(GUPPI)), 'Lband_GUPPI': (Receiver(Lband), Backend(GUPPI)), '800_GASP': (Receiver(800), Backend(GASP)), 'Lband_GASP': (Receiver(Lband), Backend(GASP))} 800.0 MHz 1400.0 MHz Lband
MIT
docs/_static/notebooks/telescopes_tutorial_5.ipynb
LBJ-Wade/PsrSigSim
Defining a new systemOne can also add a new system to one of these existing telescopes, similarly to what will be done when define a new telescope from scratch. Here we will add the 350 MHz receiver with the GUPPI backend to the Green Bank Telescope.First we define a new `Receiver` and `Backend` object. The `Receiver`...
# First we define a new receiver rcvr_350 = pss.telescope.receiver.Receiver(fcent=350, bandwidth=100, name="350") # And then we want to use the GUPPI backend guppi = pss.telescope.backend.Backend(samprate=3.125, name="GUPPI") # Now we add the new system. This needs just the receiver, backend, and a name tscope_GBT.add_...
(Receiver(350), Backend(GUPPI))
MIT
docs/_static/notebooks/telescopes_tutorial_5.ipynb
LBJ-Wade/PsrSigSim
Defining a new telescopeWe can also define a new telescope from scratch. In addition to needing the `Receiver` and `Backend` objects to define at least one system, the `telescope` also needs the aperture size in meters, the total area in meters^2, the system temperature in kelvin, and a name. Here we will define a sma...
# We first need to define the telescope parameters aperture = 3.0 # meters area = (0.5*aperture)**2*np.pi # meters^2 Tsys = 250.0 # kelvin, note this is not a realistic system temperature for a backyard telescope name = "Backyard_Telescope" # Now we can define the telescope tscope_bkyd = pss.telescope.Telescope(apertur...
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MIT
docs/_static/notebooks/telescopes_tutorial_5.ipynb
LBJ-Wade/PsrSigSim
Now similarly to defining a new system before, we must add a system to our new telescope by defining a receiver and a backend. Since this just represents a little telescope, the system won't be comparable to the previously defined telescope.
rcvr_bkyd = pss.telescope.receiver.Receiver(fcent=1400, bandwidth=20, name="Lband") backend_bkyd = pss.telescope.backend.Backend(samprate=0.25, name="Laptop") # Note this is not a realistic sampling rate # Add the system to our telecope tscope_bkyd.add_system(name="bkyd", receiver=rcvr_bkyd, backend=backend_bkyd) # An...
{'bkyd': (Receiver(Lband), Backend(Laptop))}
MIT
docs/_static/notebooks/telescopes_tutorial_5.ipynb
LBJ-Wade/PsrSigSim
Observing with different telescopesNow that we have three different telescopes, we can observe our simulated pulsar with all three and compare the sensitivity of each telescope for the same initial `Signal` and `Pulsar`. Since the radiometer noise from the telescope is added directly to the signal though, we will need...
# We define three new, similar, signals, one for each telescope signal_1713_AO = pss.signal.FilterBankSignal(fcent = f0, bandwidth = bw, Nsubband=Nf, sample_rate = f_samp, sublen = sublen, fold = True) # Our backyard telescope will need slightly different parameters to be comparab...
WARNING: AstropyDeprecationWarning: The truth value of a Quantity is ambiguous. In the future this will raise a ValueError. [astropy.units.quantity]
MIT
docs/_static/notebooks/telescopes_tutorial_5.ipynb
LBJ-Wade/PsrSigSim
Now we can look at the simulated data and compare the sensitivity of the different telescopes. We first plot the observation from the GBT, then Arecibo, and then our newly defined backyard telescope.
# We first plot the first two pulses in frequency-time space to show the undispersed pulses time = np.linspace(0, obslen, len(signal_1713_GBT.data[0,:])) # Since we know there are 2048 bins per pulse period, we can index the appropriate amount plt.plot(time[:4096], signal_1713_GBT.data[0,:4096], label = signal_1713_GB...
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MIT
docs/_static/notebooks/telescopes_tutorial_5.ipynb
LBJ-Wade/PsrSigSim
!pip3 install -U pywebio # !pip install -U https://github.com/solrz/PyWebIO/archive/dev.zip !wget https://bin.equinox.io/c/4VmDzA7iaHb/ngrok-stable-linux-amd64.zip !unzip ngrok-stable-linux-amd64.zip !wget https://raw.githubusercontent.com/solrz/pywebio-example/main/hello_world.py !pip3 install nest-asyncio import ran...
請拖曳網址到新視窗來打開App(每次網址都會更新喔!): https://950ebb9c7872.ngrok.io Listen on 0.0.0.0:7606
MIT
Eatago.ipynb
ifsunnyace/eatago-1
FCLA/FNLA Fast.ai Numerical/Computational Linear Algebra Lecture 3: New Perspectives on NMF, Randomized SVDNotes / In-Class QuestionsWNixalo - 2018/2/8 Question on section: [Truncated SVD](http://nbviewer.jupyter.org/github/fastai/numerical-linear-algebra/blob/master/nbs/2.%20Topic%20Modeling%20with%20NMF%20and%20SVD....
import torch import numpy as np Q = np.eye(3) print(Q) print(Q.T) print(Q @ Q.T) # construct I matrix Q = torch.eye(3) # torch matrix multip # torch.mm(Q, Q.transpose) Q @ torch.t(Q)
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MIT
FACLA/L3-notes.ipynb
WNoxchi/Kawkasos
So if A is *approx equal* to Q•Q.T•A .. but *not* equal.. then Q is **not** the identity, but is very close to it. Oh, right. Q: m x r, **not** m x m... If both the columns and rows of Q had been orthonormal, then it would have been the Identity, but only the columns (r) are orthonormal.Q is a tall, skinny matrix. ---A...
import numpy as np from sklearn.datasets import fetch_20newsgroups from sklearn import decomposition from scipy import linalg import matplotlib.pyplot as plt %matplotlib inline np.set_printoptions(suppress=True) categories = ['alt.atheism', 'talk.religion.misc', 'comp.graphics', 'sci.space'] remove = ('headers', 'foo...
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MIT
FACLA/L3-notes.ipynb
WNoxchi/Kawkasos
Randomized SVD method:
def randomized_svd(M, n_components, n_oversamples=10, n_iter=4): # number of random columns we're going to create is the number of # columns we want + number of oversamples (extra buffer) n_random = n_components + n_oversamples Q = randomized_range_finder(M, n_random, n_iter) # proje...
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MIT
FACLA/L3-notes.ipynb
WNoxchi/Kawkasos
Computational Complexity for a M`x`N matrix in SVD is $M^2N+N^3$, so Randomized (Truncated?) SVD is a *massive* improvement. ---2018/3/7Write a loop to calculate the error of your decomposition as your vary the of topics. Plot the results.
# 1. how do I calculate decomposition error?: # I guess I'll use MSE? # # NumPy: # https://stackoverflow.com/questions/16774849/mean-squared-error-in-numpy # def MSEnp(A,B): # if type(A) == np.ndarray and type(B) == np.ndarray: # return ((A - B) ** 2).mean() # else: # return np.square((A - B...
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MIT
FACLA/L3-notes.ipynb
WNoxchi/Kawkasos
USDA Unemployment
import pandas as pd import os import matplotlib.pyplot as plt import seaborn as sns
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MIT
code/USDA notebooks /EDA_for_USDA_unemployment.ipynb
STRIDES-Codes/Supporting-Pandemic-Recovery-Building-insights-on-vaccine-hesitancy-in-the-communities-hardest-hit-
Data US Unemployment data by countyEconomic Research Service U.S. Department of Agriculture link: Notes - Year 2020, Median Household Income (2019), & '% of State Median HH Income had 78 Nan Values that are all from Puerto Rico.- I am going to drop all rows from Puerto Rico, Puerto Rico does not show up in any of ...
stats_master_list = ['Vermont', 'Mississippi', 'Maine', 'Montana', 'Washington', 'District of Columbia', 'Texas', 'Alabama', 'Michigan', 'Maryland', 'Rhode Island', 'South Dakota', 'Nebraska', 'Virginia', 'Florida', 'Utah', 'Louisiana', 'Missouri', 'Massachusetts', 'South Carolina', 'Pennsylvania', ...
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MIT
code/USDA notebooks /EDA_for_USDA_unemployment.ipynb
STRIDES-Codes/Supporting-Pandemic-Recovery-Building-insights-on-vaccine-hesitancy-in-the-communities-hardest-hit-
File managment
files = os.listdir("../data_raw/USDA_gov-unemplyment/") # remove mac file files.remove('.DS_Store') #files
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MIT
code/USDA notebooks /EDA_for_USDA_unemployment.ipynb
STRIDES-Codes/Supporting-Pandemic-Recovery-Building-insights-on-vaccine-hesitancy-in-the-communities-hardest-hit-
Example of the csv files
# random peek df = pd.read_excel('../data_raw/USDA_gov-unemplyment/UnemploymentReport (14).xlsx', skiprows=2) df.shape df.head() df.tail()
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MIT
code/USDA notebooks /EDA_for_USDA_unemployment.ipynb
STRIDES-Codes/Supporting-Pandemic-Recovery-Building-insights-on-vaccine-hesitancy-in-the-communities-hardest-hit-
Create master DataFrame
# Concat # create master file master_df = pd.DataFrame(columns = columns) state_name_list = [] # LOOP for file in files: # read excel file _df = pd.read_excel('../data_raw/USDA_gov-unemplyment/'+file, skiprows=2) # read state_name state_name = _df.iloc[0,1] # DROP #drop row 0 _df.drop...
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MIT
code/USDA notebooks /EDA_for_USDA_unemployment.ipynb
STRIDES-Codes/Supporting-Pandemic-Recovery-Building-insights-on-vaccine-hesitancy-in-the-communities-hardest-hit-
Dataframe clean up
# reset Index master_df.reset_index(drop = True, inplace = True ) master_df.columns # Rename columns master_df.rename(columns = {'FIPS ':'FIPS'}, inplace = True) # shape master_df.shape master_df.head()
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MIT
code/USDA notebooks /EDA_for_USDA_unemployment.ipynb
STRIDES-Codes/Supporting-Pandemic-Recovery-Building-insights-on-vaccine-hesitancy-in-the-communities-hardest-hit-
Remove rows with all nan's
master_df.isna().sum() master_df[ master_df['FIPS'].isnull()].head() nan_rows = master_df[ master_df['FIPS'].isnull()].index nan_rows len(nan_rows) # remove rows with all Nans master_df.drop(nan_rows, inplace = True) master_df.isna().sum() master_df[ master_df['2020'].isnull()].iloc[20:25,:]
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MIT
code/USDA notebooks /EDA_for_USDA_unemployment.ipynb
STRIDES-Codes/Supporting-Pandemic-Recovery-Building-insights-on-vaccine-hesitancy-in-the-communities-hardest-hit-
- There are 78 rows that do have nans for 2020, - all of the Remaing rows with nan's are form Puerto Rico- I am going to remove the Nans from Puerto Rico because the other USDA data sets do not have Puerto Rico
master_df[ master_df['state'] == 'Puerto Rico' ].index # Drop all Rows with state as Puerto Rico index_names = master_df[ master_df['state'] == 'Puerto Rico' ].index master_df.drop(index_names, inplace = True) master_df.drop([], inplace = True ) master_df.isna().sum() master_df.shape
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MIT
code/USDA notebooks /EDA_for_USDA_unemployment.ipynb
STRIDES-Codes/Supporting-Pandemic-Recovery-Building-insights-on-vaccine-hesitancy-in-the-communities-hardest-hit-
Sanity Check
# unique Count of stats master_df['state'].nunique() len(state_name_list) # checks if there are duplicates in state list checkIfDuplicates_3(state_name_list) master_df['state'].nunique()
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MIT
code/USDA notebooks /EDA_for_USDA_unemployment.ipynb
STRIDES-Codes/Supporting-Pandemic-Recovery-Building-insights-on-vaccine-hesitancy-in-the-communities-hardest-hit-
Write to CSV
master_df.to_csv('../data/USDA/USDA_unemployment.csv', index=False) master_df.shape
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MIT
code/USDA notebooks /EDA_for_USDA_unemployment.ipynb
STRIDES-Codes/Supporting-Pandemic-Recovery-Building-insights-on-vaccine-hesitancy-in-the-communities-hardest-hit-
EDA
master_df.shape master_df.head(2) plt.figure(figsize = (17, 17)) sns.scatterplot(data = master_df, x = '2020', y = "Median Household Income (2019)", hue = 'state'); plt.xlabel("% of unemployment") plt.title("% of Unemployment by Household Median income 2019") set(master_df['FIPS'])
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MIT
code/USDA notebooks /EDA_for_USDA_unemployment.ipynb
STRIDES-Codes/Supporting-Pandemic-Recovery-Building-insights-on-vaccine-hesitancy-in-the-communities-hardest-hit-
Manually filled pop.xlsx
pop=pd.read_excel('pop.xlsx') dta['summer']=pop['summer'] dta['winter']=pop['winter'] dta.to_excel('alldata.xlsx') dta.set_index('name').T.to_json('antarctica.json') v = cesiumpy.Viewer(animation=False, baseLayerPicker=True, fullscreenButton=True, geocoder=False, homeButton=False, infoBox=True, sceneMode...
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MIT
antarctica/parser.ipynb
csaladenes/tsne
_Lambda School Data Science_ This sprint, your project is about water pumps in Tanzania. Can you predict which water pumps are faulty? Confusion Matrix Objectives- get and interpret the confusion matrix for classification models- use classification metrics: precision, recall- understand the relationships between precis...
# !pip install category_encoders matplotlib==3.1.0
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
Review: Load data, fit model
%matplotlib inline import category_encoders as ce import matplotlib.pyplot as plt import numpy as np import pandas as pd import seaborn as sns from sklearn.impute import SimpleImputer from sklearn.metrics import accuracy_score from sklearn.model_selection import train_test_split from sklearn.pipeline import make_pipeli...
Validation Accuracy 0.8140409527789386
MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
Get and interpret the confusion matrix for classification models[Scikit-Learn User Guide — Confusion Matrix](https://scikit-learn.org/stable/modules/model_evaluation.htmlconfusion-matrix)
from sklearn.metrics import confusion_matrix cm = confusion_matrix(y_val, y_pred) cm sns.heatmap? y_val.unique() sns.heatmap(cm, cmap='viridis', annot=True, fmt='d') columns=[f'Predicted "{c}"' for c in y_val.unique()] columns index_names =[f'Actual "{c}"' for c in y_val.unique()] index_names df = pd.DataFrame(cm, colu...
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
How many correct predictions were made?
7005 + 332 + 4351 sum(y_val == y_pred)
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
How many total predictions were made?
len(y_val) cm.sum()
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
What was the classification accuracy?
11688/14358 sum(y_val == y_pred)/len(y_val)
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
Use classification metrics: precision, recall[Scikit-Learn User Guide — Classification Report](https://scikit-learn.org/stable/modules/model_evaluation.htmlclassification-report)
from sklearn.metrics import classification_report print(classification_report(y_val, y_pred))
precision recall f1-score support functional 0.81 0.90 0.85 7798 functional needs repair 0.58 0.32 0.41 1043 non functional 0.85 0.79 0.82 5517 micro avg 0.81 0.81 0.81 ...
MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
Wikipedia, [Precision and recall](https://en.wikipedia.org/wiki/Precision_and_recall)> Both precision and recall are based on an understanding and measure of relevance.> Suppose a computer program for recognizing dogs in photographs identifies 8 dogs in a picture containing 12 dogs and some cats. Of the 8 identified a...
plot_confusion_matrix(y_val, y_pred)
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
How many correct predictions of "non functional"?
correct_predictions_nonfunctional = 4351
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
How many total predictions of "non functional"?
total_predictions_nonfunctional = 622 + 156 + 4351 total_predictions_nonfunctional
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
What's the precision for "non functional"?
correct_predictions_nonfunctional/total_predictions_nonfunctional
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
How many actual "non functional" waterpumps?
actual_nonfunctional = 1098 + 68 + 4351 actual_nonfunctional
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
What's the recall for "non functional"?
correct_predictions_nonfunctional/actual_nonfunctional (0.81+0.58+0.85)/3 print(classification_report(y_val, y_pred)) classification_report(y_val, y_pred, output_dict=True)['non functional']['precision']
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
Understand the relationships between precision, recall, thresholds, and predicted probabilities. Understand how Precision@K can help make decisions and allocate budgets Imagine this scenario...Suppose there are over 14,000 waterpumps that you _do_ have some information about, but you _don't_ know whether they are cur...
len(test)
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
**You have the time and resources to go to just 2,000 waterpumps for proactive maintenance.** You want to predict, which 2,000 are most likely non-functional or in need of repair, to help you triage and prioritize your waterpump inspections.You have historical inspection data for over 59,000 other waterpumps, which you...
len(train) + len(val)
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
You have historical inspection data for over 59,000 other waterpumps, which you'll use to fit your predictive model.Based on this historical data, if you randomly chose waterpumps to inspect, then about 46% of the waterpumps would need repairs, and 54% would not need repairs.
y_train.value_counts(normalize=True)
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
**Can you do better than random at prioritizing inspections?** In this scenario, we should define our target differently. We want to identify which waterpumps are non-functional _or_ are functional but needs repair:
y_train = y_train != 'functional' y_val = y_val != 'functional' y_train.value_counts(normalize=True)
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
We already made our validation set the same size as our test set.
len(val) == len(test)
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
We can refit our model, using the redefined target.Then make predictions for the validation set.
pipeline.fit(X_train, y_train) y_pred = pipeline.predict(X_val) y_pred_proba = pipeline.predict_proba(X_val) y_pred_proba
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles
And look at the confusion matrix:
y_pred_proba[:,1] confusion_matrix(y_val, y_pred) ax = sns.distplot(y_pred_proba[:,1], kde=False) ax.axvline(0.5, color='r') y_pred = y_pred_proba[:,1] > 0.6 pd.Series(y_pred).value_counts()
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MIT
module3-confusion-matrix/confusion_matrix.ipynb
alex000kim/DS-Unit-2-Tree-Ensembles