Python: performing FFT on music file

Question

I am trying to perform a FFT on a song (audio file in wav format, about 3 minutes long) which I created as follows, just in case it is relevant.

ffmpeg -i "$1" -vn -ab 128k -ar 44100 -y -ac 1 "${1%.webm}.wav"

Where $1 is the name of a webm file.

This is the code which is supposed to display a FFT of the given file:

import numpy as np
import matplotlib.pyplot as plt

# presume file already converted to wav.
file = os.path.join(temp_folder, file_name)

rate, aud_data = scipy.io.wavfile.read(file)

# wav file is mono.
channel_1 = aud_data[:]

fourier = np.fft.fft(channel_1)

plt.figure(1)
plt.plot(fourier)
plt.xlabel('n')
plt.ylabel('amplitude')
plt.show()

The problem is, it takes for ever. It takes so long that I cannot even show the output, since I've had plenty of time to research and write this post and it still has not finished.

I presume that the file is too long, since

print (aud_data.shape)

outputs (9218368,), but this looks like a real world problem, so I hope there is a way to obtain an FFT of an audio file somehow.

What am I doing wrong? Thank you.

edit

A better formulation of the question would be: is the FFT of any good in music processing? For example similarity of 2 pieces.

As pointed out in the comments, my plain approach is way too slow.

Thank you.

Solution

To considerably speed up the fft portion of your analysis, you can zero-pad out your data to a power of 2:

import numpy as np
import matplotlib.pyplot as plt

# rate, aud_data = scipy.io.wavfile.read(file)
rate, aud_data = 44000, np.random.random((9218368,))

len_data = len(aud_data)

channel_1 = np.zeros(2**(int(np.ceil(np.log2(len_data)))))
channel_1[0:len_data] = aud_data

fourier = np.fft.fft(channel_1)

Here is an example of plotting the real component of the fourier transform of a few sine waves using the above method:

import numpy as np
import matplotlib.pyplot as plt

# rate, aud_data = scipy.io.wavfile.read(file)
rate = 44000
ii = np.arange(0, 9218368)
t = ii / rate
aud_data = np.zeros(len(t))
for w in [1000, 5000, 10000, 15000]:
    aud_data += np.cos(2 * np.pi * w * t)

# From here down, everything else can be the same
len_data = len(aud_data)

channel_1 = np.zeros(2**(int(np.ceil(np.log2(len_data)))))
channel_1[0:len_data] = aud_data

fourier = np.fft.fft(channel_1)
w = np.linspace(0, 44000, len(fourier))

# First half is the real component, second half is imaginary
fourier_to_plot = fourier[0:len(fourier)//2]
w = w[0:len(fourier)//2]

plt.figure(1)

plt.plot(w, fourier_to_plot)
plt.xlabel('frequency')
plt.ylabel('amplitude')
plt.show()