---
title: "MATLAB vs Python: Speed Test for Vibration Analysis [Free Download]"
description: Examine real computation times to compare MATLAB and Python loading data and generating a FFT.  The real data used and scripts can be downloaded.
---

[enDAQ Blog for Data Sensing and Analyzing](https://blog.endaq.com)

# [MATLAB vs Python: Speed Test for Vibration Analysis \[Free Download\]](https://blog.endaq.com/matlab-vs-python-speed-for-vibration-analysis-free-download)

 Written by [Steve Hanly](https://blog.endaq.com/author/steve-hanly) | Aug 19, 2016, 4:08:36 PM

What’s faster, MATLAB or Python?  There are a lot of forums out there comparing the two programming languages; but none seemed to give actual computation times for *real* analysis.  This post will.

In this post we’ll test two similar MATLAB and Python scripts as they perform some basic vibration analysis.  These scripts do the following:

1. Load in a two column CSV
2. Plot all data
3. Compute and plot the moving 1 second RMS level
4. Compute and plot a FFT

The MATLAB and Python functions are available to [download](https://endaq.com/pages/free-vibration-analysis-files) as well as the vibration data files used in the analysis.  We’ll look at data sets ranging in size from tens of thousands of points to tens of millions. For an introduction to Python, check out our article [Get Started with Python: Why and How Mechanical Engineers Should Make the Switch](https://blog.endaq.com/get-started-with-python-why-how-mechanical-engineers-should-make-the-switch).

## MATLAB and Python Background

I’m a MATLAB guy.  I’ve probably been using MATLAB for about 10 years and I must admit I love performing some “MATLAB magic.”  But I’ve learned more and more about Python over the last several years as fellow engineers here at enDAQ (a division of Midé) use it to create our [enDAQ Lab](https://endaq.com/pages/vibration-shock-analysis-software-endaq-slam-stick-lab) (formerly Slam Stick Lab) vibration analysis software package.  I’ve also frequently fielded questions from customers of our [enDAQ sensors](https://endaq.com/collections/endaq-sensors-shock-vibration-s-series) (formerly Slam Stick vibration logger products) asking how to perform their [vibration analysis](https://blog.endaq.com/vibration-analysis-fft-psd-and-spectrogram).  I’ve recommended both Python and MATLAB; but then the follow-on question is… well what’s better, MATLAB or Python?

### Python

In general [Python](https://www.python.org/) has the advantage of being free, open source, and more versatile.  Their [NumPy](http://www.numpy.org/) and [SciPy](http://www.scipy.org/) packages have similar functions to MATLAB.  Python is a pretty elegant and intuitive programming language compared to MATLAB.  It was created to be a generic language that is easy to read; and they definitely succeeded with that! Python is universally accepted as the better alternative to MATLAB for other programming needs besides data analysis.

### MATLAB

[MATLAB](http://www.mathworks.com/products/matlab/), on the other hand, was developed specifically for linear algebraic operations which could make it faster for vibration analysis applications.  The downside is that the language can be a little more difficult to read/understand; but MATLAB is generally considered more cleanly packaged because you get an extensive library of functions and an integrated development environment (IDE) in one.  For Python you need to install extra packages and the IDE (not a major lift to do though!).  

The big disadvantage of MATLAB is that it's not free, a commercial license will run you $2,150.  They also charge more, typically $1,000, for additional toolboxes; and I'd recommend the [signal processing toolbox](https://www.mathworks.com/products/signal/index.html) for vibration analysis.  Don't worry though, I didn't use any functions in that toolbox for this analysis or the ones covered in my [vibration analysis basics blog](https://blog.endaq.com/vibration-analysis-fft-psd-and-spectrogram). Here's a full [price list](https://www.mathworks.com/pricing-licensing/index.html?prodcode=ML) of the MATLAB products.  MathWorks (the makes of MATLAB) are smart with their pricing though in that they offer significantly discounted licenses to students (get the entire suite including all toolboxes for $99) and to home users ($149 for MATLAB, $45 for signal processing toolbox). So must engineering students will come out of university with a knowledge and preference for MATLAB.  They then take this preference to their future employer giving MATLAB the edge.

### MATLAB vs Python

There are a lot of blogs and forums out there comparing the two programming languages/platforms (here’s a relatively biased, but informative, [Python vs MATLAB comparison](http://www.pyzo.org/python_vs_matlab.html)).  A coworker here at enDAQ (a division of Mide) said that its difficult to compare Python directly to MATLAB: “it’s like comparing a diesel engine to a gas one, each has unique benefits and drawbacks,” he said. Maybe because of their differences, I had trouble finding an objective comparison of performance on real data sets for the type of analysis that I, or vibration customers, would be performing.  So I set out to objectively measure the difference!

## The Code

### MATLAB® Vibration Analysis Function:

I wanted the comparison between Python and MATLAB to be as apples-to-apples as possible.  I also wanted it to be doing a useful analysis, one typical for vibration testing.  I wrote the initial script in MATLAB to prompt the user for a CSV, load the CSV, and plot all data.  I then perform a simple moving RMS calculation and plot this followed by a FFT of the entire data set and plot.  The script times how long each of these major steps take.  I’m looking at moving RMS because this gives a sense of the strength of the vibration as it moves with time.  An FFT is one of the fundamental first vibration analysis steps.  Check out [my blog on FFTs](https://blog.endaq.com/vibration-analysis-fft-psd-and-spectrogram) for some more background.  Writing the MATLAB script was the easy part. Here it is below. The .m file is also available for [download](https://endaq.com/pages/free-vibration-analysis-files).

|   |  |
| --- | --- |
| 01 02 03 04 05 06 07 08 09 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 | `close``all` `clear``all`   `%``Get filename``and` `path` `    ``[fname,pathname]``=` `uigetfile(``'.csv'``,``'Select CSV File to Load, Plot, Compute RMS & FFT'``);` `    ``disp([pathname fname])`   `%``Load CSV` `    ``tic``%``start timer` `    ``data``=` `csvread([pathname fname]);` `    ``fprintf(``'%4.2f seconds - Time to Load Data\n'``,toc)` `    `  `%``Determine variables``and` `Display size` `    ``[N,m]``=` `size(data);` `    ``t``=` `data(:,``1``);``%``time``in` `seconds` `    ``x``=` `data(:,``2``);``%``array of data``for` `RMS``and` `FFT` `    ``Fs``=` `1``/``(t(``2``)``-``t(``1``));` `    ``fprintf(``'%12.0f data points\n'``,N)`   `%``Plot Data` `    ``tic``%``start timer` `    ``figure(``1``)` `    ``plot(t,x)` `    ``xlabel(``'Time (s)'``);` `    ``ylabel(``'Accel (g)'``);` `    ``title(fname);` `    ``grid on;` `    ``fprintf(``'%4.2f seconds - Time to Plot Data\n'``,toc)` `    `  `%``Determine RMS``and` `Plot` `    ``tic``%``start timer` `    ``w``=` `floor(Fs);``%``width of the window``for` `computing RMS` `    ``steps``=` `floor(N``/``w);``%``Number of steps``for` `RMS` `    ``t_RMS``=` `zeros(steps,``1``);``%``Create array``for` `RMS time values` `    ``x_RMS``=` `zeros(steps,``1``);``%``Create array``for` `RMS values` `    ``for` `i``=``1``:steps` `        ``range` `=` `((i``-``1``)``*``w``+``1``):(i``*``w);` `        ``t_RMS(i)``=` `mean(t(``range``));` `        ``x_RMS(i)``=` `sqrt(mean(x(``range``).^``2``)); ` `    ``end` `    ``figure(``2``)` `    ``plot(t_RMS,x_RMS)` `    ``xlabel(``'Time (s)'``);` `    ``ylabel(``'RMS Accel (g)'``);` `    ``title([``'RMS - '` `fname]);` `    ``grid on;` `    ``fprintf(``'%4.2f seconds - Time to Compute RMS and Plot\n'``,toc)   ` `    `  `%``Determine FFT``and` `Plot` `    ``tic` `    ``freq``=` `0``:Fs``/``length(x):Fs``/``2``;``%``frequency array``for` `FFT` `    ``xdft``=` `fft(x);``%``Compute FFT` `    ``xdft``=` `1``/``length(x).``*``xdft;``%``Normalize` `    ``xdft(``2``:end``-``1``)``=` `2``*``xdft(``2``:end``-``1``);` `    ``figure(``3``)` `    ``plot(freq,``abs``(xdft(``1``:floor(N``/``2``)``+``1``)))` `    ``xlabel(``'Frequency (Hz)'``);` `    ``ylabel(``'Accel (g)'``);` `    ``title([``'FFT - '` `fname]);` `    ``grid on;` `    ``fprintf(``'%4.2f seconds - Time to Compute FFT and Plot\n'``,toc)` |
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```
close all
clear all

%Get filename and path 
    [fname,pathname] = uigetfile('.csv','Select CSV File to Load, Plot, Compute RMS & FFT');
    disp([pathname fname])

%Load CSV
    tic %start timer
    data = csvread([pathname fname]); 
    fprintf('%4.2f seconds - Time to Load Data\n',toc)
    
%Determine variables and Display size
    [N,m] = size(data);
    t = data(:,1); %time in seconds
    x = data(:,2); %array of data for RMS and FFT
    Fs = 1/(t(2)-t(1));
    fprintf('%12.0f data points\n',N)

%Plot Data
    tic %start timer
    figure(1)
    plot(t,x)
    xlabel('Time (s)');
    ylabel('Accel (g)');
    title(fname);
    grid on;
    fprintf('%4.2f seconds - Time to Plot Data\n',toc)
    
%Determine RMS and Plot
    tic %start timer
    w = floor(Fs); %width of the window for computing RMS
    steps = floor(N/w); %Number of steps for RMS
    t_RMS = zeros(steps,1); %Create array for RMS time values
    x_RMS = zeros(steps,1); %Create array for RMS values
    for i=1:steps
        range = ((i-1)*w+1):(i*w);
        t_RMS(i) = mean(t(range));
        x_RMS(i) = sqrt(mean(x(range).^2));  
    end
    figure(2)
    plot(t_RMS,x_RMS)
    xlabel('Time (s)');
    ylabel('RMS Accel (g)');
    title(['RMS - ' fname]);
    grid on;
    fprintf('%4.2f seconds - Time to Compute RMS and Plot\n',toc)    
    
%Determine FFT and Plot
    tic 
    freq = 0:Fs/length(x):Fs/2; %frequency array for FFT
    xdft = fft(x); %Compute FFT
    xdft = 1/length(x).*xdft; %Normalize
    xdft(2:end-1) = 2*xdft(2:end-1); 
    figure(3)
    plot(freq,abs(xdft(1:floor(N/2)+1)))
    xlabel('Frequency (Hz)');
    ylabel('Accel (g)');
    title(['FFT - ' fname]);
    grid on;
    fprintf('%4.2f seconds - Time to Compute FFT and Plot\n',toc)

```

### Python Vibration Analysis Function:

The hard part was to write an equivalent script in Python.  I had never written any Python scripts as of two days ago.  I was pleasantly surprised with how easily I was able to “translate” this MATLAB script into Python.  There are a *ton* of resources online, I found this [NumPy for MATLAB users](https://numpy.org/doc/stable/user/numpy-for-matlab-users.html) tutorial particularly helpful.  The Pyhon script is provided below. The length of the scripts are virtually the same; the Python script is a couple lines longer to load in the necessary libraries. The .py file is available for [download](https://endaq.com/pages/free-vibration-analysis-files).

 

|   |  |
| --- | --- |
| 01 02 03 04 05 06 07 08 09 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 | `import` `matplotlib.pyplot as plt` `import` `numpy as np` `from` `scipy.fftpack``import` `fft` `import` `tkinter as tk` `from` `tkinter``import` `filedialog` `import` `time`   `#Prompt user for file` `root``=` `tk.Tk()` `root.withdraw()` `file_path``=` `filedialog.askopenfilename(filetypes``=``[(``"Two Column CSV"``,``"*.csv"``)])` `print``(file_path)`   `#Load Data (assumes two column array` `tic``=` `time.clock()` `t, x``=` `np.genfromtxt(file_path,delimiter``=``','``, unpack``=``True``)` `toc``=` `time.clock()` `print``(``"Load Time:"``,toc``-``tic)`   `#Determine variables` `N``=` `np.``int``(np.prod(t.shape))``#length of the array` `Fs``=` `1``/``(t[``1``]``-``t[``0``]) ``#sample rate (Hz)` `T``=` `1``/``Fs;` `print``(``"# Samples:"``,N)`   `#Plot Data` `tic``=` `time.clock()` `plt.figure(``1``) ` `plt.plot(t, x)` `plt.xlabel(``'Time (seconds)'``)` `plt.ylabel(``'Accel (g)'``)` `plt.title(file_path)` `plt.grid()` `toc``=` `time.clock()` `print``(``"Plot Time:"``,toc``-``tic)`   `#Compute RMS and Plot` `tic``=` `time.clock()` `w``=` `np.``int``(np.floor(Fs));``#width of the window for computing RMS` `steps``=` `np.int_(np.floor(N``/``w));``#Number of steps for RMS` `t_RMS``=` `np.zeros((steps,``1``));``#Create array for RMS time values` `x_RMS``=` `np.zeros((steps,``1``));``#Create array for RMS values` `for` `i``in` `range` `(``0``, steps):` `    ``t_RMS[i]``=` `np.mean(t[(i``*``w):((i``+``1``)``*``w)]);` `    ``x_RMS[i]``=` `np.sqrt(np.mean(x[(i``*``w):((i``+``1``)``*``w)]``*``*``2``)); ` `plt.figure(``2``) ` `plt.plot(t_RMS, x_RMS)` `plt.xlabel(``'Time (seconds)'``)` `plt.ylabel(``'RMS Accel (g)'``)` `plt.title(``'RMS - '` `+` `file_path)` `plt.grid()` `toc``=` `time.clock()` `print``(``"RMS Time:"``,toc``-``tic)`   `#Compute and Plot FFT` `tic``=` `time.clock()` `plt.figure(``3``) ` `xf``=` `np.linspace(``0.0``,``1.0``/``(``2.0``*``T), N``/``2``)` `yf``=` `fft(x)` `plt.plot(xf,``2.0``/``N``*` `np.``abs``(yf[``0``:np.``int``(N``/``2``)]))` `plt.grid()` `plt.xlabel(``'Frequency (Hz)'``)` `plt.ylabel(``'Accel (g)'``)` `plt.title(``'FFT - '` `+` `file_path)` `toc``=` `time.clock()` `print``(``"FFT Time:"``,toc``-``tic)` `plt.show()` |
|   |  |
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```
import matplotlib.pyplot as plt
import numpy as np
from scipy.fftpack import fft
import tkinter as tk
from tkinter import filedialog
import time

#Prompt user for file
root = tk.Tk()
root.withdraw()
file_path = filedialog.askopenfilename(filetypes=[("Two Column CSV","*.csv")])
print(file_path)

#Load Data (assumes two column array
tic = time.clock()
t, x = np.genfromtxt(file_path,delimiter=',', unpack=True)
toc = time.clock()
print("Load Time:",toc-tic)

#Determine variables
N = np.int(np.prod(t.shape))#length of the array
Fs = 1/(t[1]-t[0])  #sample rate (Hz)
T = 1/Fs;
print("# Samples:",N)

#Plot Data
tic = time.clock()
plt.figure(1)  
plt.plot(t, x)
plt.xlabel('Time (seconds)')
plt.ylabel('Accel (g)')
plt.title(file_path)
plt.grid()
toc = time.clock()
print("Plot Time:",toc-tic)

#Compute RMS and Plot
tic = time.clock()
w = np.int(np.floor(Fs)); #width of the window for computing RMS
steps = np.int_(np.floor(N/w)); #Number of steps for RMS
t_RMS = np.zeros((steps,1)); #Create array for RMS time values
x_RMS = np.zeros((steps,1)); #Create array for RMS values
for i in range (0, steps):
    t_RMS[i] = np.mean(t[(i*w):((i+1)*w)]);
    x_RMS[i] = np.sqrt(np.mean(x[(i*w):((i+1)*w)]**2));  
plt.figure(2)  
plt.plot(t_RMS, x_RMS)
plt.xlabel('Time (seconds)')
plt.ylabel('RMS Accel (g)')
plt.title('RMS - ' + file_path)
plt.grid()
toc = time.clock()
print("RMS Time:",toc-tic)

#Compute and Plot FFT
tic = time.clock()
plt.figure(3)  
xf = np.linspace(0.0, 1.0/(2.0*T), N/2)
yf = fft(x)
plt.plot(xf, 2.0/N * np.abs(yf[0:np.int(N/2)]))
plt.grid()
plt.xlabel('Frequency (Hz)')
plt.ylabel('Accel (g)')
plt.title('FFT - ' + file_path)
toc = time.clock()
print("FFT Time:",toc-tic)
plt.show()

```

## Vibration Data Files

We go through 7 different vibration data sets in this comparison.  Most of these recording are explained in a little more depth on our [vibration analysis basics](https://blog.endaq.com/vibration-analysis-fft-psd-and-spectrogram) blog post. All data was captured using our [enDAQ sensors](https://endaq.com/collections/endaq-sensors-shock-vibration-s-series) and I exported the data to CSV.  The first two recordings are from a 60 second recording with the sensor on a shaker table vibrating at a constant 10g, 100 Hz sinusoidal input.  One file is from the MEMS accelerometer sampling at 400 Hz; the other is from the piezoelectric accelerometer sampling at 5,000 Hz.

We also look at a recording file from the sensor sampling at 10,000 Hz on the shaker being excited with a random vibration exposure profile in accordance with[MIL-STD-810G](https://www.atec.army.mil/publications/Mil-Std-810G/Mil-Std-810G.pdf).  Two recordings look at vibrations on an aircraft.  One (aircraft.csv) is from a recording with the enDAQ sensor on the outside of a plane with a 2,500 Hz sample rate (can’t share too much about the application).  The second recording (aircraft\_takeoff.csv) is when I mounted a sensor to the seat in front of me during takeoff on a commercial flight and sampled at 2,000 Hz. My wife wasn’t too pleased with that test…

The final two recordings are looking at data of my car’s (2008 Saab 93 2.0T) engine.  The first recording (car\_engine.csv) is part of our [how-to video series](https://support.endaq.com/article/178-original-how-to-videos) that has more information.  The second and largest dataset (commute.csv) is when I mounted the sensor to my engine and record the vibrations during my morning commute which included going on the highway.  I live close by so it’s only a 20 minute recording but I was sampling at 10,000 Hz so there are over 11 million data points.

## Test Setup – Computer and Software Used

I did all the testing on my work computer which is a Dell Precision T3610.  It has an Intel Xeon 3.00 GHz processor and 8 GB of RAM.  The operating system is Windows 7 Professional 64-bit.  The MATLAB I’m using is R2014b, 64-bit.  I downloaded and ran Python 3.5.2 64-bit, NumPy 1.11.1, and SciPy 0.18.0.

All data and scripts were saved on my C drive for the testing.  I ran each twice and took the average.  I made sure the two times were comparable between the tests.  I had a fair number of programs running (MATLAB, Chrome, Outlook, Excel, Visio, and Word); but I kept all programs open during both tests (Python and MATLAB) to keep things consistent.

## The Plots Gallery

Click through below to see the vibration analysis example plots generated from the two scripts. The top are from MATLAB, the bottom from Python.  From left to right, the whole data set is plotted, then the moving RMS, then a FFT of the entire data set.  You can see that both MATLAB and Python get to the same place; but the question is how quickly did they get there?  

<https://www.flickr.com/photos/146186210@N03/28449847664/in/album-72157672537368106/>

## The Results

Below is a table with all times listed in seconds comparing how quickly MATLAB and Python performed the main functions.

### Loading a CSV

My immediate question was why the heck is MATLAB able to load in a CSV to memory *so* much faster than Python?!  Check out a log-log plot of the time difference; MATLAB is consistently an order of magnitude faster!  I couldn’t understand how/why this is the case so I restarted my computer to see if MATLAB was doing something clever with using memory that wasn’t ever really cleared.  But the results after restarting my computer were comparable.

Side note: When I first did this test I was using the [numpy.loadtxt()](http://docs.scipy.org/doc/numpy/reference/generated/numpy.loadtxt.html) function.  One of the engineers here recommended the [numpy.genfromtxt()](http://docs.scipy.org/doc/numpy/reference/generated/numpy.genfromtxt.html) function which was three times faster!  Still though not nearly as fast as MATLAB.  The comparison plots and table show data when using the faster genfromtxt() function.

### Plotting and Computing Moving RMS

Python did an equivalent job plotting and computing RMS as MATLAB.  This was relatively expected from what I had read and I was happy with Python's performance here!  One note though is that MATLAB plot windows are a little more richer with information and options for customization. Apparently [IPython](https://ipython.org/) is an interactive Python shell that's great for similar plotting customization to MATLAB.  Here's a nice [tutorial on IPython.](https://plot.ly/python/ipython-notebook-tutorial/)

### Computing FFT

The next major question though was what the heck is going on with SciPy’s FFT computation times!? 

[MATLAB’s FFT function](http://www.mathworks.com/help/matlab/math/fast-fourier-transform-fft.html) has a relatively linear dependency on the array’s length.  This is expected as they state:

> The execution time of an FFT algorithm depends on the transform length. It is fastest when the transform length is a power of two, and almost as fast when the transform length has only small prime factors. It is typically slower for transform lengths that are prime or have large prime factors. Time differences, however, are reduced to insignificance by modern FFT algorithms such as those used in MATLAB. Adjusting the transform length for efficiency is usually unnecessary in practice.

The computation time in [SciPy’s FFT function](http://docs.scipy.org/doc/scipy/reference/fftpack.html) was barely linear and very weird… For example it took 30 times longer to compute a FFT for an array length 2,465,342 than one of length 3,068,583.  Let me say that again, it took 30 times longer to compute an FFT on an array with over a half a million *less* data points!  I reran this test many times to see if something strange was happening on my computer; but it is repeatable.  When I showed this to Mide's FFT expert [Pete](https://blog.endaq.com/author/pete-scheidler) (he recently wrote a post that goes a bit deeper into the [math behind FFTs](https://blog.endaq.com/fourier-transform-basics)) he immediately began writing a couple scripts to look a little deeper into this.  Subscribe to our blog if you’re interested in what he finds out.

# Optimizing Python to Beat MATLAB

At first glance, this testing wasn't a great look for Python.  But I did some digging and spoke to a couple of the engineers here on ways to improve the Python performance.

Two suggestions were made:

1. Use the [pandas](http://pandas.pydata.org/pandas-docs/stable/) data analysis library's [read\_csv()](https://www.datacamp.com/tutorial/pandas-read-csv) function for importing
2. Truncate the array to the last power of 2 for FFT calculation

### Optimized Python Code

It only added a couple lines of code to optimize the vibration analysis script.  The major differences being another library imported and a line or two to calculate the last power of 2 and truncate the array.  Here it is below.

 

|   |  |
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| 01 02 03 04 05 06 07 08 09 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 | `import` `matplotlib.pyplot as plt` `import` `pandas as pd` `import` `numpy as np` `from scipy.fftpack``import` `fft` `import` `tkinter as tk` `from tkinter``import` `filedialog` `import` `time`   `#Prompt user``for` `file` `root = tk.Tk()` `root.withdraw()` `file_path = filedialog.askopenfilename(filetypes=[(``"Two Column CSV"``,``"*.csv"``)])` `print(file_path)`   `#Load Data (assumes two column array` `tic = time.clock()` `df = pd.read_csv(file_path,delimiter=``','``,header=None,names=[``"time"``,``"data"``])` `t = df[``"time"``]` `x = df[``"data"``]` `toc = time.clock()` `print(``"Load Time:"``,toc-tic)`   `#Determine variables` `N = np.``int``(np.prod(t.shape))#length of the array` `N2 =``2``**(N.bit_length()-``1``) #last power of``2` `Fs =``1``/(t[``1``]-t[``0``])  #sample rate (Hz)` `T =``1``/Fs;` `print(``"# Samples:"``,N)` `print(``"Next power of 2:"``,N2)`   `#Plot Data` `tic = time.clock()` `plt.figure(``1``) ` `plt.plot(t, x)` `plt.xlabel(``'Time (seconds)'``)` `plt.ylabel(``'Accel (g)'``)` `plt.title(file_path)` `plt.grid()` `toc = time.clock()` `print(``"Plot Time:"``,toc-tic)`   `#Compute RMS and Plot` `tic = time.clock()` `w = np.``int``(np.floor(Fs)); #width of the window``for` `computing RMS` `steps = np.int_(np.floor(N/w)); #Number of steps``for` `RMS` `t_RMS = np.zeros((steps,``1``)); #Create array``for` `RMS time values` `x_RMS = np.zeros((steps,``1``)); #Create array``for` `RMS values` `for` `i in range (``0``, steps):` `    ``t_RMS[i] = np.mean(t[(i*w):((i+``1``)*w)]);` `    ``x_RMS[i] = np.sqrt(np.mean(x[(i*w):((i+``1``)*w)]**``2``)); ` `plt.figure(``2``) ` `plt.plot(t_RMS, x_RMS)` `plt.xlabel(``'Time (seconds)'``)` `plt.ylabel(``'RMS Accel (g)'``)` `plt.title(``'RMS - '` `+ file_path)` `plt.grid()` `toc = time.clock()` `print(``"RMS Time:"``,toc-tic)`   `#Compute and Plot FFT` `tic = time.clock()` `plt.figure(``3``) ` `N = N2 #truncate array to the last power of``2` `xf = np.linspace(``0.0``,``1.0``/(``2.0``*T), N/``2``)` `yf = fft(x, n = N)` `plt.plot(xf,``2.0``/N * np.abs(yf[``0``:np.``int``(N/``2``)]))` `plt.grid()` `plt.xlabel(``'Frequency (Hz)'``)` `plt.ylabel(``'Accel (g)'``)` `plt.title(``'FFT - '` `+ file_path)` `toc = time.clock()` `print(``"FFT Time:"``,toc-tic)` `plt.show()` |
|   |  |
|   |  |

```
import matplotlib.pyplot as plt
import pandas as pd
import numpy as np
from scipy.fftpack import fft
import tkinter as tk
from tkinter import filedialog
import time

#Prompt user for file
root = tk.Tk()
root.withdraw()
file_path = filedialog.askopenfilename(filetypes=[("Two Column CSV","*.csv")])
print(file_path)

#Load Data (assumes two column array
tic = time.clock()
df = pd.read_csv(file_path,delimiter=',',header=None,names=["time","data"])
t = df["time"]
x = df["data"]
toc = time.clock()
print("Load Time:",toc-tic)

#Determine variables
N = np.int(np.prod(t.shape))#length of the array
N2 = 2**(N.bit_length()-1) #last power of 2
Fs = 1/(t[1]-t[0])  #sample rate (Hz)
T = 1/Fs;
print("# Samples:",N)
print("Next power of 2:",N2)

#Plot Data
tic = time.clock()
plt.figure(1)  
plt.plot(t, x)
plt.xlabel('Time (seconds)')
plt.ylabel('Accel (g)')
plt.title(file_path)
plt.grid()
toc = time.clock()
print("Plot Time:",toc-tic)

#Compute RMS and Plot
tic = time.clock()
w = np.int(np.floor(Fs)); #width of the window for computing RMS
steps = np.int_(np.floor(N/w)); #Number of steps for RMS
t_RMS = np.zeros((steps,1)); #Create array for RMS time values
x_RMS = np.zeros((steps,1)); #Create array for RMS values
for i in range (0, steps):
    t_RMS[i] = np.mean(t[(i*w):((i+1)*w)]);
    x_RMS[i] = np.sqrt(np.mean(x[(i*w):((i+1)*w)]**2));  
plt.figure(2)  
plt.plot(t_RMS, x_RMS)
plt.xlabel('Time (seconds)')
plt.ylabel('RMS Accel (g)')
plt.title('RMS - ' + file_path)
plt.grid()
toc = time.clock()
print("RMS Time:",toc-tic)

#Compute and Plot FFT
tic = time.clock()
plt.figure(3)  
N = N2 #truncate array to the last power of 2
xf = np.linspace(0.0, 1.0/(2.0*T), N/2)
yf = fft(x, n = N)
plt.plot(xf, 2.0/N * np.abs(yf[0:np.int(N/2)]))
plt.grid()
plt.xlabel('Frequency (Hz)')
plt.ylabel('Accel (g)')
plt.title('FFT - ' + file_path)
toc = time.clock()
print("FFT Time:",toc-tic)
plt.show()

```

### Overview of Optimized Results

Below is a table that has the Python computation times with the updated/optimized script. There is a significant improvement!

### Loading a CSV

I had no issue installing the [pandas library](http://pandas.pydata.org/pandas-docs/stable/) which claims "to be the fundamental high-level building block for doing practical, **real world** data analysis in Python."  The plot below shows the loading times.  Without pandas, MATLAB was loading a CSV 10 times faster than Python; now Python is twice as fast as MATLAB!

The naysayers out there (myself included) will say that in MATLAB you wouldn't need to use CSVs and could use their impressive binary [MAT file format](https://www.mathworks.com/help/pdf_doc/matlab/matfile_format.pdf).  And that's true, you should try to be using MAT files when in MATLAB.  If I load the MAT file with the same data as that 11.5 million point commute.csv file, MATLAB loads it in 0.7 seconds.  A noticeable improvement over the 11 seconds it takes when loading the CSV.  The file itself is also much smaller (54 vs 174 MB).  But SciPy has a few functions for loading and saving MAT files ([scipy.io](https://docs.scipy.org/doc/scipy/reference/generated/scipy.io.loadmat.html)).  And Python loads that same MAT file in around 0.7 seconds as well.  So it seems that MATLAB can't claim faster loading times over Python even when using their own file format!

As Jake and TheBlackCat pointed out in the comments (thank you!), loading a CSV is not a great way to go if you're loading large data files.  And I definitely agree; I used that in this testing because it's a little more well-known to the non-technical folks out there. But if you'll be loading large data sets you should be using a binary file format like [HDF5](https://www.hdfgroup.org/HDF5/) or [UFF58](http://zone.ni.com/reference/en-XX/help/372416A-01/svtconcepts/svms_uff58/).

### Truncating the FFT

I was a bit hesitant to truncate the array length to the last power of 2 because I felt that this wasn't going to be an apples-to-apples comparison to MATLAB.  I also didn't like missing the end of an array which may have had some different frequency content that a FFT would have been able to pick up. I thought about zero-padding the array to increase to the *next* power of 2; but the added zeros can smear the FFT peaks.  And with the type of data files I'm used to on enDAQ sensors (high sample rate and battery life equals millions of data points) I don't care too much about missing the end of a recording in a FFT (just do a spectrogram to capture it).  I'm much more concerned with reducing the amplitude of my frequency components though. I use that information to generate power spectral densities for determining the vibration response of my system.  

In the MATLAB plot below the FFT results are compared when truncating or zero padding the aircraft takeoff data. You can see that truncating leads to pretty similar amplitudes when compared to an unmodified array.  But check out the results when zero padding the array; it significantly reduces the FFT amplitude.  I wouldn't recommend zero padding when you need to draw conclusions from the amplitude of your FFT (which would be most vibration analysis applications).  If you're *only* interested in the frequencies themselves then zero padding is preferred because the frequency resolution would be improved and all data is still analyzed.  All that being said, there are a ton of different ways to compute a FFT and you can do scaling and windowing with zero padding to get comparable results.  I'll punt that discussion for another day though (subscribe to our blog if you're interested in finding out more).  For the purpose of optimizing Python's FFT computation time to compete with MATLAB, just truncate.  If you are worried about missing data then compute two FFTs for each half of the file and/or compute and plot a spectrogram.

So I went with truncating.  When the array was truncated to the last power of two Python is able to compute an FFT in roughly half the time compared to MATLAB!  If I do this same truncation in the MATLAB script though the computation times are comparable.  I wouldn't recommend doing the truncation for MATLAB because it doesn't need it (who really cares about 1 second faster on an 11 million data point array at the price of missing data?). Python, on the other hand, *clearly needs* this truncation.  Truncating allows Python to be as much as 1,000 times faster!  

Forget about trying to compute the FFT without truncating if you get a prime number as the array length.  Let's look at the aircraft take off data as an example again.  It's length is 1,124,434 and Python (specifically SciPy) computes the FFT in 2 seconds (MATLAB does it in 0.2).  If we truncate down to 1,048,576 (2^20) it computes in 0.14 seconds.  Now if we truncate down 5 data points to the prime number 1,124,429 the FFT computes in... well I don't know, I gave up after waiting 10 minutes!  Meanwhile MATLAB computed the FFT of this in 0.5 seconds.

### Truncated FFT Gallery

Click through the plots below (MATLAB on the left, Python on the right) to see how reducing the FFT length affects the amplitude.  There are definitely small differences but they're pretty close.  So again, if you're in Python it's worthwhile to truncate arrays before computing a FFT.  MATLAB doesn't seem to need this and would be the preferred option if you don't feel comfortable truncating and potentially missing data. 

# Python's PyFFTW Algorithm

After I initially posted this blog several folks commented (thank you!) and suggested I check out the [pyFFTW Python library](http://hgomersall.github.io/pyFFTW/) that uses the [FFTW](http://www.fftw.org/) library for computing FFTs. The FFTW is a very fast C library for computing FFTs. It apparently checks a variety of different FFT solving algorithms and determines the best one to use for a given input size. So this involves some "planning" before actually computing the FFT to figure out which algorithm is the best. MATLAB uses this same algorithm so I figured I'd give it a try! This would then be a *true *apples-to-apples comparison between MATLAB and Python for vibration analysis.

You can use their `pyfftw.interfaces` module to simple replace all instances of calling the NumPy or SciPy FFT function.  Instead of calling the **`scipy.fft()`** function I could replace that with `pyfftw.interfaces.scipy_fftpack.fft()`. Of course this meant now that I had to go out and import another library (one of the benefits and downfalls of the open source environment: so much stuff in so many places); but this wasn't too difficult.  I just used that [pip command](https://pypi.python.org/pypi/pip) and then I had pyFFTW; so I thought I was off and running!

The [pyFFTW documentation](http://hgomersall.github.io/pyFFTW/sphinx/tutorial.html) mentioned that the first call for a given transform size may be slow for the FFTW to do its planning.  Then subsequent calls would be fast.  I thought this was kind of stupid. If I'm going to run a FFT on a specific length then I should just use some power of 2, not an arbitrary number.  I wanted to find a way to solve a FFT fast for the *first *time on an arbitrary transform length. But I figured this planning stage can't take too long...

I was wrong.  For the car\_engine.csv file (1,200,048 samples) solving the first time with FFTW took **20 minutes!** The second time it took 0.4 seconds (about the same as MATLAB); but who cares! I thought this was going to be able to allow Python to compete with MATLAB!

I was about to give up when I went digging a little further and looked at the [**`fftw()`**](http://www.mathworks.com/help/matlab/ref/fftw.html) MATLAB function that lets you interface directly with the FFTW library. I noticed that MATLAB defaults the 'planner' method to 'estimate' whereas [Python's pyFFTW](https://hgomersall.github.io/pyFFTW/pyfftw/pyfftw.html) defaults to 'measure.' So I opened up MATLAB and tried to see what happens if I change the settings to 'measure' instead.  Sure enough I start getting similar computing times to Python's pyFFTW.  I was on to something; but now I needed to figure out how to change the setting in Python!

This was much more difficult than I thought.  Admittedly though, I wasn't too familiar with Python so I called in the big guns. One of our three Python experts at Midé (enDAQ is a division of Mide), [Pete](https://blog.endaq.com/author/pete-scheidler), came through with the answer!  He used the [builders method](https://hgomersall.github.io/pyFFTW/pyfftw/builders/builders.html) to relatively easily solve the FFT using FFTW in Python. For a given input array (named input\_data) you first need to create a NumPy array: **`a = np.array(input_data, dtype='float32')`**. Then to solve the FFT is done with: **`fft_obj = pyfftw.builders.rfft(a, planner_effort='FFTW_ESTIMATE')`**. Looked pretty straightforward!

He wrote a new function that tests a couple different ways to solve a FFT using pyFFTW which is included below.  You can tell an actual Python user wrote his code, it's much cleaner than mine! But let's see how this solving method stacked up compared to MATLAB.

### The Results

I'm sorry to say to the MATLAB lovers out there (myself included) that pyFFTW solved the trick!  If you're able to use that function then you can actually consistently *beat* MATLAB for solving a FFT.  Check out the table and log-log plot of the results below.  These compare solving times for MATLAB, pyFFTW with the planner set to 'estimate,' SciPy with a truncated array, and then SciPy with no truncation.

The only trouble with using pyFFTW apparently is the licensing as TheBlackCat nicely explained below in the comments. At enDAQ we've written the Python code for the [enDAQ Lab Software](https://endaq.com/pages/vibration-shock-analysis-software-endaq-slam-stick-lab) (formerly Slam Stick Lab analysis software) all in NumPy due to licensing concerns. But after this testing we've begun looking into a way to obtain a commercial license. As you can see in the results above, pyFFTW is far superior to NumPy's or SciPy's FFT functions and let's you truly compete with MATLAB on performance.

### The Code

|   |  |
| --- | --- |
| 001 002 003 004 005 006 007 008 009 010 011 012 013 014 015 016 017 018 019 020 021 022 023 024 025 026 027 028 029 030 031 032 033 034 035 036 037 038 039 040 041 042 043 044 045 046 047 048 049 050 051 052 053 054 055 056 057 058 059 060 061 062 063 064 065 066 067 068 069 070 071 072 073 074 075 076 077 078 079 080 081 082 083 084 085 086 087 088 089 090 091 092 093 094 095 096 097 098 099 100 101 102 103 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118 119 120 121 122 123 124 125 126 127 128 129 130 131 132 133 134 135 136 137 138 139 140 141 142 143 144 145 146 147 148 149 150 151 152 153 154 155 156 157 158 159 160 161 162 163 164 165 166 167 168 169 170 171 172 173 174 175 176 177 178 179 180 181 182 183 184 185 186 187 188 189 190 191 192 193 | `import` `matplotlib.pyplot as plt` `import` `pandas as pd` `import` `numpy as np` `import` `tkinter as tk` `from` `tkinter``import` `filedialog` `import` `time` `import` `pyfftw` `import` `os`   `#####` `# Functions for testing various FFT methods` `#####`     `def` `fftw_builder_test(input_data):` `    ``pyfftw.forget_wisdom()      ``# This is just here to keep the tests honest, normally pyfftw will remember setup parameters and go more quickly when it is run a second time` `    ``a``=` `np.array(input_data, dtype``=``'float32'``)  ``# This turns the input list into a numpy array. We can make it a 32 bit float because the data is all real, no imaginary component` `    ``fft_obj``=` `pyfftw.builders.rfft(a)          ``# This creates an object which generates the FFT` `    ``return` `fft_obj()                           ``# And calling the object returns the FFT`     `def` `fftw_fast_builder_test(input_data):``# See fftw_builder_test for comments` `    ``pyfftw.forget_wisdom()` `    ``a``=` `np.array(input_data, dtype``=``'float32'``)` `    ``fft_obj``=` `pyfftw.builders.rfft(a, planner_effort``=``'FFTW_ESTIMATE'``)  ``# FFTW_ESTIMATE is a lower effort planner than the default. This seems to work more quickly for over 8000 points` `    ``return` `fft_obj()`   `def` `fftw_test(input_data):` `    ``pyfftw.forget_wisdom()                 ``# This is just here to keep the tests honest` `    ``outLength``=` `len``(input_data)``/``/``2` `+` `1`      `# For a real FFT, the output is symetrical. fftw returns only half the data in this case` `    ``a``=` `pyfftw.empty_aligned(``len``(input_data), dtype``=``'float32'``)     ``# This is the input array. It will be cleared when the fft object is created` `    ``outData``=` `pyfftw.empty_aligned(outLength, dtype``=``'complex64'``)   ``# This is the output array. Not that the size and type must be appropriate` `    ``fft_obj``=` `pyfftw.FFTW(a, outData, flags``=``(``'FFTW_ESTIMATE'``,),planning_timelimit``=``1.0``) ``# NB: The flags tuple has a comma` `    ``a[:]``=` `np.array(input_data, dtype``=``'float32'``)   ``# We have to fill the array after fft_obj is created. NB: 'a[:] =' puts data into the existing array, 'a =' creates a new array` `    ``return` `fft_obj()                       ``# Calling the object returns the FFT of the data now in a. The result is also in outData`     `def` `fftw_test_complex(input_data): ``# This is fftw_test but running a complex FFT as opposed to a real input FFT. See fftw_test for comments` `    ``pyfftw.forget_wisdom()` `    ``outLengthMod``=` `len``(input_data)``/``/``2` `+` `1`   `# Size of expected return data` `    ``outLength``=` `len``(input_data)            ``# For a complex input FFT, we get more data` `    ``a``=` `pyfftw.empty_aligned(``len``(input_data), dtype``=``'complex64'``)   ``# The FFTW determines the type of FFT by the type of input` `    ``outData``=` `pyfftw.empty_aligned(outLength, dtype``=``'complex64'``)` `    ``fft_obj``=` `pyfftw.FFTW(a, outData, flags``=``(``'FFTW_ESTIMATE'``,),planning_timelimit``=``1.0``)` `    ``a[:]``=` `np.array(input_data, dtype``=``'complex64'``)` `    ``return` `fft_obj()[``0``:outLengthMod]`     `def` `fftw_test_default(input_data): ``# This is fftw_test with different FFTW options. See fftw_test for comments` `    ``pyfftw.forget_wisdom()` `    ``outLength``=` `len``(input_data)``/``/``2` `+` `1` `    ``a``=` `pyfftw.empty_aligned(``len``(input_data), dtype``=``'float32'``)` `    ``outData``=` `pyfftw.empty_aligned(outLength, dtype``=``'complex64'``)` `    ``fft_obj``=` `pyfftw.FFTW(a, outData)` `    ``a[:]``=` `np.array(input_data, dtype``=``'float32'``)` `    ``return` `fft_obj()`     `def` `fftw_test_no_limit(input_data):``# This is fftw_test with different FFTW options. See fftw_test for comments` `    ``pyfftw.forget_wisdom()` `    ``outLength``=` `len``(input_data)``/``/``2` `+` `1` `    ``a``=` `pyfftw.empty_aligned(``len``(input_data), dtype``=``'float32'``)` `    ``outData``=` `pyfftw.empty_aligned(outLength, dtype``=``'complex64'``)` `    ``fft_obj``=` `pyfftw.FFTW(a, outData, flags``=``(``'FFTW_ESTIMATE'``,))` `    ``a[:]``=` `np.array(input_data, dtype``=``'float32'``)` `    ``return` `fft_obj()`     `def` `fftw_test_no_flag(input_data):     ``# This is fftw_test with different FFTW options. See fftw_test for comments` `    ``pyfftw.forget_wisdom()` `    ``outLength``=` `len``(input_data)``/``/``2` `+` `1` `    ``a``=` `pyfftw.empty_aligned(``len``(input_data), dtype``=``'float32'``)` `    ``outData``=` `pyfftw.empty_aligned(outLength, dtype``=``'complex64'``)` `    ``fft_obj``=` `pyfftw.FFTW(a, outData,planning_timelimit``=``1.0``)` `    ``a[:]``=` `np.array(input_data, dtype``=``'float32'``)` `    ``return` `fft_obj()`     `def` `numpy_test(inputData):` `    ``return` `np.fft.rfft(inputData)      ``# Numpy is nice and simple!`     `#####` `# Helper Functions` `#####`   `def` `write_csv(csv_file_name, headers, data):       ``# Helper function for writing to the CSV file` `    ``outString``=` `""` `    ``for` `header``in` `headers:` `        ``outString``+``=` `"%s,"` `%` `(data.get(header, ""))` `    ``outString``+``=` `"\n"` `    ``with``open``(csv_file_name,``'a'``) as f:` `        ``f.write(outString)`     `#Prompt user for file` `###` `# RUN TIME OPTION!` `# Set include_plots to True if you want to actually see the plot outputs. They will all be stored up and displayed` `# at the end of the test` `include_plots``=` `True` `if` `include_plots:` `    ``root``=` `tk.Tk()` `    ``root.withdraw()` `file_paths``=` `filedialog.askopenfilenames(filetypes``=``[(``"Two Column CSV"``,``"*.csv"``)])` `out_path``=` `filedialog.asksaveasfilename(defaultextension``=``".csv"``)` `print``(file_paths)`   `# CSV Setup` `output_headers``=` `[``"File"``,``"File Size"``,``"Number of Points"``,``"FFT Time"``,``"FFT Function"``,``"Load Time"``,``"Plot Time"``,``"RMS Time"` `]` `with``open``(out_path,``'w+'``) as f:` `    ``f.write(``","``.join(output_headers)``+``"\n"``)`   `# Tests to run:` `# Format { "Name" : Function, etc } Test order is undefined` `#test_functions = {"FFTW" : fftw_test, "FFTW-Complex" : fftw_test_complex, "FFTW-Builder": fftw_builder_test, "FFTW-Default" : fftw_test_default, "FFTW-NoLimit": fftw_test_no_limit, "FFTW-NoFlag": fftw_test_no_flag}` `test_functions``=` `{``"FFTW"` `: fftw_test,``"Builder"``: fftw_fast_builder_test}` `figure_count``=` `1` `# Loop through each file` `for` `file_path``in` `file_paths:` `    ``# output_data holds the test info and results. This is written to the file after the FFT is complete` `    ``output_data``=` `{``"File"` `: os.path.split(file_path)[``-``1``]}` `    ``output_data[``"File Size"``]``=` `os.path.getsize(file_path)` `    ``tic``=` `time.clock()` `    ``df``=` `pd.read_csv(file_path,delimiter``=``','``,header``=``None``,names``=``[``"time"``,``"data"``])` `    ``t``=` `df[``"time"``]` `    ``x``=` `df[``"data"``]` `    ``toc``=` `time.clock()` `    ``output_data[``"Load Time"``]``=` `toc``-``tic` `    ``print``(``"Load Time:"``,toc``-``tic)`   `    ``N``=` `np.``int``(np.prod(t.shape))``#length of the array` `    ``# Determine variables` `    ``Fs``=` `1``/``(t[``1``]``-``t[``0``]) ``#sample rate (Hz)` `    ``T``=` `1``/``Fs;` `    ``output_data[``"Number of Points"``]``=` `N` `    ``print``(``"# Samples:"``,N)`   `    ``# Plot Data` `    ``if` `include_plots:` `        ``plt.figure(figure_count)` `        ``figure_count``+``=` `1` `        ``plt.plot(t, x) ``#x` `        ``plt.xlabel(``'Time (seconds)'``)` `        ``plt.ylabel(``'Accel (g)'``)` `        ``plt.title(file_path)` `        ``plt.grid()`   `    ``# Compute RMS and Plot` `    ``tic``=` `time.clock()` `    ``w``=` `np.``int``(np.floor(Fs))        ``#width of the window for computing RMS` `    ``steps``=` `np.int_(np.floor(N``/``w))  ``#Number of steps for RMS` `    ``t_RMS``=` `np.zeros((steps,``1``))     ``#Create array for RMS time values` `    ``x_RMS``=` `np.zeros((steps,``1``))     ``#Create array for RMS values` `    ``for` `i``in` `range` `(``0``, steps):` `        ``t_RMS[i]``=` `np.mean(t[(i``*``w):((i``+``1``)``*``w)])` `        ``x_RMS[i]``=` `np.sqrt(np.mean(x[(i``*``w):((i``+``1``)``*``w)]``*``*``2``))` `    ``if` `include_plots:` `        ``plt.figure(figure_count)` `        ``figure_count``+``=` `1` `        ``plt.plot(t_RMS, x_RMS)` `        ``plt.xlabel(``'Time (seconds)'``)` `        ``plt.ylabel(``'RMS Accel (g)'``)` `        ``plt.title(``'RMS - '` `+` `file_path)` `        ``plt.grid()` `    ``toc``=` `time.clock()` `    ``output_data[``"RMS Time"``]``=` `toc``-``tic` `    ``print``(``"RMS Time:"``,toc``-``tic)`   `    ``# Compute and Plot FFT` `    ``# Run through each FFT function in test_functions, and test each one.` `    ``# File data is not reloaded` `    ``for` `func_name``in` `test_functions:` `        ``output_data[``"FFT Function"``]``=` `func_name` `        ``tic``=` `time.clock()` `        ``fftData``=` `test_functions[func_name](x)         ``# Execute the FFT` `        ``xf``=` `np.linspace(``0.0``,``1.0``/``(``2.0``*``T),``len``(fftData))` `        ``if` `include_plots:` `            ``plt.figure(figure_count)` `            ``figure_count``+``=` `1` `            ``plt.plot(xf,``2.0``/``N``*` `np.``abs``(fftData))      ``#[0:np.int(N/2)]` `            ``plt.grid()` `            ``plt.xlabel(``'Frequency (Hz)'``)` `            ``plt.ylabel(``'Accel (g)'``)` `            ``plt.title(``'FFT (%s) - %s'` `%` `(func_name, file_path))` `        ``toc``=` `time.clock()` `        ``output_data[``"FFT Time"``]``=` `toc``-``tic` `        ``print``(``"FFT Time:"``,toc``-``tic)` `        ``write_csv(out_path, output_headers, output_data)` `if` `include_plots:` `    ``print``(``"Plotting..."``)` `    ``plt.show()` `print``(``"Done!"``)` |
|   |  |
|   |  |

```
import matplotlib.pyplot as plt
import pandas as pd
import numpy as np
import tkinter as tk
from tkinter import filedialog
import time
import pyfftw
import os

#####
# Functions for testing various FFT methods
#####

def fftw_builder_test(input_data):
    pyfftw.forget_wisdom()       # This is just here to keep the tests honest, normally pyfftw will remember setup parameters and go more quickly when it is run a second time
    a = np.array(input_data, dtype='float32')   # This turns the input list into a numpy array. We can make it a 32 bit float because the data is all real, no imaginary component
    fft_obj = pyfftw.builders.rfft(a)           # This creates an object which generates the FFT
    return fft_obj()                            # And calling the object returns the FFT

def fftw_fast_builder_test(input_data): # See fftw_builder_test for comments
    pyfftw.forget_wisdom()
    a = np.array(input_data, dtype='float32')
    fft_obj = pyfftw.builders.rfft(a, planner_effort='FFTW_ESTIMATE')   # FFTW_ESTIMATE is a lower effort planner than the default. This seems to work more quickly for over 8000 points
    return fft_obj()

def fftw_test(input_data):
    pyfftw.forget_wisdom()                  # This is just here to keep the tests honest
    outLength = len(input_data)//2 + 1      # For a real FFT, the output is symetrical. fftw returns only half the data in this case
    a = pyfftw.empty_aligned(len(input_data), dtype='float32')      # This is the input array. It will be cleared when the fft object is created
    outData = pyfftw.empty_aligned(outLength, dtype='complex64')    # This is the output array. Not that the size and type must be appropriate
    fft_obj = pyfftw.FFTW(a, outData, flags=('FFTW_ESTIMATE',),planning_timelimit=1.0)  # NB: The flags tuple has a comma
    a[:] = np.array(input_data, dtype='float32')    # We have to fill the array after fft_obj is created. NB: 'a[:] =' puts data into the existing array, 'a =' creates a new array
    return fft_obj()                        # Calling the object returns the FFT of the data now in a. The result is also in outData

def fftw_test_complex(input_data):  # This is fftw_test but running a complex FFT as opposed to a real input FFT. See fftw_test for comments
    pyfftw.forget_wisdom()
    outLengthMod = len(input_data)//2 + 1   # Size of expected return data
    outLength = len(input_data)             # For a complex input FFT, we get more data
    a = pyfftw.empty_aligned(len(input_data), dtype='complex64')    # The FFTW determines the type of FFT by the type of input
    outData = pyfftw.empty_aligned(outLength, dtype='complex64')
    fft_obj = pyfftw.FFTW(a, outData, flags=('FFTW_ESTIMATE',),planning_timelimit=1.0)
    a[:] = np.array(input_data, dtype='complex64')
    return fft_obj()[0:outLengthMod]

def fftw_test_default(input_data):  # This is fftw_test with different FFTW options. See fftw_test for comments
    pyfftw.forget_wisdom()
    outLength = len(input_data)//2 + 1
    a = pyfftw.empty_aligned(len(input_data), dtype='float32')
    outData = pyfftw.empty_aligned(outLength, dtype='complex64')
    fft_obj = pyfftw.FFTW(a, outData)
    a[:] = np.array(input_data, dtype='float32')
    return fft_obj()

def fftw_test_no_limit(input_data): # This is fftw_test with different FFTW options. See fftw_test for comments
    pyfftw.forget_wisdom()
    outLength = len(input_data)//2 + 1
    a = pyfftw.empty_aligned(len(input_data), dtype='float32')
    outData = pyfftw.empty_aligned(outLength, dtype='complex64')
    fft_obj = pyfftw.FFTW(a, outData, flags=('FFTW_ESTIMATE',))
    a[:] = np.array(input_data, dtype='float32')
    return fft_obj()

def fftw_test_no_flag(input_data):      # This is fftw_test with different FFTW options. See fftw_test for comments
    pyfftw.forget_wisdom()
    outLength = len(input_data)//2 + 1
    a = pyfftw.empty_aligned(len(input_data), dtype='float32')
    outData = pyfftw.empty_aligned(outLength, dtype='complex64')
    fft_obj = pyfftw.FFTW(a, outData,planning_timelimit=1.0)
    a[:] = np.array(input_data, dtype='float32')
    return fft_obj()

def numpy_test(inputData):
    return np.fft.rfft(inputData)       # Numpy is nice and simple!

#####
# Helper Functions
#####

def write_csv(csv_file_name, headers, data):        # Helper function for writing to the CSV file
    outString = ""
    for header in headers:
        outString += "%s," % (data.get(header, ""))
    outString += "\n"
    with open(csv_file_name, 'a') as f:
        f.write(outString)

#Prompt user for file
###
# RUN TIME OPTION!
# Set include_plots to True if you want to actually see the plot outputs. They will all be stored up and displayed
# at the end of the test
include_plots = True
if include_plots:
    root = tk.Tk()
    root.withdraw()
file_paths = filedialog.askopenfilenames(filetypes=[("Two Column CSV","*.csv")])
out_path = filedialog.asksaveasfilename(defaultextension=".csv")
print(file_paths)

# CSV Setup
output_headers = ["File", "File Size", "Number of Points", "FFT Time", "FFT Function", "Load Time", "Plot Time", "RMS Time" ]
with open(out_path, 'w+') as f:
    f.write(",".join(output_headers)+"\n")

# Tests to run:
# Format { "Name" : Function, etc } Test order is undefined
#test_functions = {"FFTW" : fftw_test, "FFTW-Complex" : fftw_test_complex, "FFTW-Builder": fftw_builder_test, "FFTW-Default" : fftw_test_default, "FFTW-NoLimit": fftw_test_no_limit, "FFTW-NoFlag": fftw_test_no_flag}
test_functions = {"FFTW" : fftw_test, "Builder": fftw_fast_builder_test}
figure_count = 1
# Loop through each file
for file_path in file_paths:
    # output_data holds the test info and results. This is written to the file after the FFT is complete
    output_data = {"File" : os.path.split(file_path)[-1]}
    output_data["File Size"] = os.path.getsize(file_path)
    tic = time.clock()
    df = pd.read_csv(file_path,delimiter=',',header=None,names=["time","data"])
    t = df["time"]
    x = df["data"]
    toc = time.clock()
    output_data["Load Time"] = toc-tic
    print("Load Time:",toc-tic)

    N = np.int(np.prod(t.shape))#length of the array
    # Determine variables
    Fs = 1/(t[1]-t[0])  #sample rate (Hz)
    T = 1/Fs;
    output_data["Number of Points"] = N
    print("# Samples:",N)

    # Plot Data
    if include_plots:
        plt.figure(figure_count)
        figure_count += 1
        plt.plot(t, x)  #x
        plt.xlabel('Time (seconds)')
        plt.ylabel('Accel (g)')
        plt.title(file_path)
        plt.grid()

    # Compute RMS and Plot
    tic = time.clock()
    w = np.int(np.floor(Fs))         #width of the window for computing RMS
    steps = np.int_(np.floor(N/w))   #Number of steps for RMS
    t_RMS = np.zeros((steps,1))      #Create array for RMS time values
    x_RMS = np.zeros((steps,1))      #Create array for RMS values
    for i in range (0, steps):
        t_RMS[i] = np.mean(t[(i*w):((i+1)*w)])
        x_RMS[i] = np.sqrt(np.mean(x[(i*w):((i+1)*w)]**2))
    if include_plots:
        plt.figure(figure_count)
        figure_count += 1
        plt.plot(t_RMS, x_RMS)
        plt.xlabel('Time (seconds)')
        plt.ylabel('RMS Accel (g)')
        plt.title('RMS - ' + file_path)
        plt.grid()
    toc = time.clock()
    output_data["RMS Time"] = toc-tic
    print("RMS Time:",toc-tic)

    # Compute and Plot FFT
    # Run through each FFT function in test_functions, and test each one.
    # File data is not reloaded
    for func_name in test_functions:
        output_data["FFT Function"] = func_name
        tic = time.clock()
        fftData = test_functions[func_name](x)          # Execute the FFT
        xf = np.linspace(0.0, 1.0/(2.0*T), len(fftData))
        if include_plots:
            plt.figure(figure_count)
            figure_count += 1
            plt.plot(xf, 2.0/N * np.abs(fftData))       #[0:np.int(N/2)]
            plt.grid()
            plt.xlabel('Frequency (Hz)')
            plt.ylabel('Accel (g)')
            plt.title('FFT (%s) - %s' % (func_name, file_path))
        toc = time.clock()
        output_data["FFT Time"] = toc-tic
        print("FFT Time:",toc-tic)
        write_csv(out_path, output_headers, output_data)
if include_plots:
    print("Plotting...")
    plt.show()
print("Done!")

```

# Conclusions

A couple major take-aways:

1. Python is an impressive ***free*** alternative to MATLAB
2. [Python's SciPy FFT function](http://docs.scipy.org/doc/numpy/reference/routines.fft.html) is inferior to [MATLAB's](http://www.mathworks.com/help/matlab/math/fast-fourier-transform-fft.html), especially when dealing with data sets that have a length not equal to a power of 2 
     - Forget about even trying to compute a FFT on an array that has a length equal to a prime number in SciPy or Numpy
     - Best practice in SciPy or NumPy is to truncate the array to the last power of 2
3. [pyFFTW](https://hgomersall.github.io/pyFFTW/pyfftw/pyfftw.html) is far superior to SciPy's or NumPy's FFT function and offers comparable performance to MATLAB 
     - The only downside is the licensing issue if you are distributing any software
4. The [pandas library](http://pandas.pydata.org/pandas-docs/stable/) is a must have for Python users loading CSV files

I originally concluded that MATLAB has better built in functions compared to Python. But the truth is that Python has those same functions and computing abilities!  The only trouble is that you have to go digging a bit to find them and compile it all together. And the extra bit of work is a hurdle for a user like me: someone with a lot of MATLAB experience and a company paying for my commercial license.

This testing completely opened my eyes to the possibilities of Python though.  It’s intriguing to have a truly *free* alternative to MATLAB and one that can get you the same analysis results.  For folks that are turned off by the high price of MATLAB then Python is a great option.  If cost is not a concern and you’re mostly interested in technical analysis of matrices, then MATLAB may be a little easier to work with. But if you are going to be doing any programming besides technical analysis, Python seems to be the far better option.

I’m curious to see what you think though, do you prefer MATLAB or Python? Select your opinion below.  I also encourage you to download the data to try the testing for yourself! And if you'd like to do more with Python for vibration data analysis, check out our post [Top 12 Vibration Metrics to Monitor & How to Calculate Them](https://blog.endaq.com/top-vibration-metrics-to-monitor-how-to-calculate-them) which provides source code on how all of these calculations were done in Python. 

Do you prefer MATLAB or Python?

MATLAB

Python

[free polls](http://www.poll-maker.com)

 

 

For an introduction to Python, check out our article [Get Started with Python: Why and How Mechanical Engineers Should Make the Switch](https://blog.endaq.com/get-started-with-python-why-how-mechanical-engineers-should-make-the-switch).

[View full post](https://blog.endaq.com/matlab-vs-python-speed-for-vibration-analysis-free-download)

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