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복잡한 신호가 단순한 여러 파형으로 구성되었다는 것을 보여주는 그림
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import numpy as np | ||
from matplotlib import pyplot as plt | ||
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def draw_sum_of_wave(a0, coeffi, w): | ||
t = np.linspace(0.0, 1.0, 1000) # 1ms 단위. ~1초 | ||
n = range(1,len(coeffi)+1) # 1,2,3,...len(coeffi) | ||
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y_a0 = a0 * np.ones(len(t)) | ||
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sin_val = [ab[0] * np.sin(i*w*t) for ab,i in zip(coeffi,n)] #an*sin(nwt) | ||
cos_val = [ab[1] * np.cos(i*w*t) for ab,i in zip(coeffi,n)] #bn*cos(nwt) | ||
yn = [(a0 + s + c) for s,c in zip(sin_val,cos_val)] | ||
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y_sum = yn[0] | ||
for y in yn[1:]: y_sum += y | ||
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plt.subplot(5,1,1) | ||
plt.plot(t, y_sum) | ||
plt.title(r"$y(t)=a_0 + \sum _{n=0}^{\infty}{a_n \sin n\omega t + b_n \cos n\omega t}$") | ||
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plt.subplot(5,1, 2) | ||
plt.plot(t, y_a0) | ||
plt.title("$y(t)=a_0$") | ||
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plt.subplot(5, 2, 5) | ||
plt.plot(t, sin_val[0]) | ||
plt.title(r"$y(t)=a_1 \sin \omega t$") | ||
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plt.subplot(5, 2, 6) | ||
plt.plot(t, cos_val[0]) | ||
plt.title(r"$y(t)=b_1 \cos \omega t$") | ||
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plt.subplot(5, 2, 7) | ||
plt.plot(t, sin_val[1]) | ||
plt.title(r"$y(t)=a_2 \sin \omega t$") | ||
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plt.subplot(5, 2, 8) | ||
plt.plot(t, cos_val[1]) | ||
plt.title(r"$y(t)=b_2 \cos \omega t$") | ||
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plt.subplot(5, 2, 9) | ||
plt.plot(t, sin_val[2]) | ||
plt.title(r"$y(t)=a_3 \sin \omega t$") | ||
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plt.subplot(5, 2, 10) | ||
plt.plot(t, cos_val[2]) | ||
plt.title(r"$y(t)=b_3 \cos \omega t$") | ||
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# plt.tight_layout() | ||
plt.show() | ||
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a0 = 0.4 | ||
coeffi = ( | ||
(0.3,0.5), (0.2,0.5), (0.2,0.3), (0.7,0.6),(1.2,0.3), (0.3,0.6),(0.2,0.3), (2.3,0.6),(1.5,1.5),(0.2,0.5),(2.3,0.6),(1.5,1.5),(0.2,0.5) | ||
) | ||
w = 2*np.pi*4 | ||
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draw_sum_of_wave(a0, coeffi, w ) |