Marcos Duarte

Here will see an introduction to data filtering and the most basic filters typically used in signal processing of biomechanical data.

You should be familiar with the basic properties of signals before proceeding.

In data acquisition with an instrument, it's common that the noise has higher frequencies and lower amplitudes than the desired signal. To remove this noise from the signal, a procedure known as filtering or smoothing is employed in the signal processing.

Filtering is a process to attenuate from a signal some unwanted component or feature. A filter usually removes certain frequency components from the data according to its frequency response.

Frequency response is the quantitative measure of the output spectrum of a system or device in response to a stimulus, and is used to characterize the dynamics of the system.

Smoothing is the process of removal of local (at short scale) fluctuations in the data while preserving a more global pattern in the data (such local variations could be noise or just a short scale phenomenon that is not interesting). A filter with a low-pass frequency response performs smoothing.

With respect to the filter implementation, it can be classified as analog filter or digital filter.

An analog filter is an electronic circuit that performs filtering of the input electrical signal (analog data) and outputs a filtered electrical signal (analog data). A simple analog filter can be implemmented with a electronic circuit with a resistor and a capacitor. A digital filter, is a system that implement the filtering of a digital data (time-discrete data).

An example of a low-pass (smoothing) filter is the moving average, which is performed taking the arithmetic mean of subsequences of $m$ terms of the data. For instance, the moving averages with window sizes (m) equal to 2 and 3 are:

$$ \begin{array}{} &y_{MA(2)} = \frac{1}{2}[x_1+x_2,\; x_2+x_3,\; \cdots,\; x_{n-1}+x_n] \\ &y_{MA(3)} = \frac{1}{3}[x_1+x_2+x_3,\; x_2+x_3+x_4,\; \cdots,\; x_{n-2}+x_{n-1}+x_n] \end{array} $$Which has the general formula:

$$ y[i] = \sum_{j=0}^{m-1} x[i+j] \;\;\;\; for \;\;\; i=1, \; \dots, \; n-m+1 $$Where $n$ is the number (length) of data.

Let's implement a simple version of the moving average filter.

First, let's import the necessary Python libraries and configure the environment:

In [1]:

```
# Import the necessary libraries
import numpy as np
import matplotlib.pyplot as plt
%matplotlib inline
import seaborn as sns
#sns.set()
sns.set_context("notebook", font_scale=1.2, rc={"lines.linewidth": 2, "lines.markersize": 10})
from IPython.display import HTML, display
import sys
sys.path.insert(1, r'./../functions') # add to pythonpath
```

A naive moving-average function definition:

In [2]:

```
def moving_average(x, window):
"""Moving average of 'x' with window size 'window'."""
y = np.empty(len(x)-window+1)
for i in range(len(y)):
y[i] = np.sum(x[i:i+window])/window
return y
```

Let's generate some data to test this function:

In [3]:

```
signal = np.zeros(300)
signal[100:200] += 1
noise = np.random.randn(300)/10
x = signal + noise
window = 11
y = moving_average(x, window)
# plot
fig, ax = plt.subplots(1, 1, figsize=(8, 4))
ax.plot(x, 'b.-', linewidth=1, label = 'raw data')
ax.plot(y, 'r.-', linewidth=2, label = 'moving average')
ax.legend(frameon=False, loc='upper right', fontsize=10)
ax.set_xlabel("Time [s]")
ax.set_ylabel("Amplitude")
plt.show()
```

Later we will look on better ways to calculate the moving average.

In signal processing, a digital filter is a system that performs mathematical operations on a signal to modify certain aspects of that signal. A digital filter (in fact, a causal, linear time-invariant (LTI) digital filter) can be seen as the implementation of the following difference equation in the time domain:

$$ \begin{array}{} y_n &= \;\; b_0x_n + \; b_1x_{n-1} + \cdots + b_Mx_{n-M} - \; a_1y_{n-1} - \cdots - a_Ny_{n-N} \\ & = \;\; \sum_{k=0}^M b_kx_{n-k} - \sum_{k=1}^N a_ky_{n-k} \end{array} $$Where the output $y$ is the filtered version of the input $x$, $a_k$ and $b_k$ are the filter coefficients (real values), and the order of the filter is the larger of N or M.

This general equation is for a recursive filter where the filtered signal y is calculated based on current and previous values of $x$ and on previous values of $y$ (the own output values, because of this it is said to be a system with feedback). A filter that does not re-use its outputs as an input (and it is said to be a system with only feedforward) is called nonrecursive filter (the $a$ coefficients of the equation are zero). Recursive and nonrecursive filters are also known as infinite impulse response (IIR) and finite impulse response (FIR) filters, respectively.

A filter with only the terms based on the previous values of $y$ is also known as an autoregressive (AR) filter. A filter with only the terms based on the current and previous values of $x$ is also known as an moving-average (MA) filter. The filter with all terms is also known as an autoregressive moving-average (ARMA) filter. The moving-average filter can be implemented by making $n$ $b$ coefficients each equals to $1/n$ and the $a$ coefficients equal to zero in the difference equation.

Another form to characterize a digital filter is by its transfer function. In simple terms, a transfer function is the ratio in the frequency domain between the input and output signals of a filter.

For continuous-time input signal $x(t)$ and output $y(t)$, the transfer function $H(s)$ is given by the ratio between the Laplace transforms of input $x(t)$ and output $y(t)$:

Where $s = \sigma + j\omega$; $j$ is the imaginary unit and $\omega$ is the angular frequency, $2\pi f$.

In the steady-state response case, we can consider $\sigma=0$ and the Laplace transforms with complex arguments reduce to the Fourier transforms with real argument $\omega$.

For discrete-time input signal $x(t)$ and output $y(t)$, the transfer function $H(z)$ will be given by the ratio between the z-transforms of input $x(t)$ and output $y(t)$, and the formalism is similar.

The transfer function of a digital filter (in fact for a linear, time-invariant, and causal filter), obtained by taking the z-transform of the difference equation shown earlier, is given by:

$$ H(z) = \frac{Y(z)}{X(z)} = \frac{b_0 + b_1 z^{-1} + b_2 z^{-2} + \cdots + b_N z^{-N}}{1 + a_1 z^{-1} + a_2 z^{-2} + \cdots + a_M z^{-M}} $$$$ H(z) = \frac{\sum_{k=0}^M b_kz^{-k}}{1 + \sum_{k=1}^N a_kz^{-k}} $$And the order of the filter is the larger of N or M.

Similar to the difference equation, this transfer function is for a recursive (IIR) filter. If the $a$ coefficients are zero, the denominator is equal to one, and the filter becomes nonrecursive (FIR).

The Fourier transform is a mathematical operation to transform a signal which is function of time, $g(t)$, into a signal which is function of frequency, $G(f)$, and it is defined by:

$$ \mathcal{F}[g(t)] = G(f) = \int_{-\infty}^{\infty} g(t) e^{-j 2\pi f t} dt $$

Its inverse operation is:

$$ \mathcal{F}^{-1}[G(f)] = g(t) = \int_{-\infty}^{\infty} G(f) e^{j 2\pi f t} df $$

The function $G(f)$ is the representation in the frequency domain of the time-domain signal, $g(t)$, and vice-versa. The functions $g(t)$ and $G(f)$ are referred to as a Fourier integral pair, or Fourier transform pair, or simply the Fourier pair. See this text for an introduction to Fourier transform.

In relation to the frequencies that are not removed from the data (and a boundary is specified by the critical or cutoff frequency), a filter can be a low-pass, high-pass, band-pass, and band-stop. The frequency response of such filters is illustrated in the next figure.

The critical or cutoff frequency for a filter is defined as the frequency where the power (the amplitude squared) of the filtered signal is half of the power of the input signal (or the output amplitude is 0.707 of the input amplitude).

For instance, if a low-pass filter has a cutoff frequency of 10 Hz, it means that at 10 Hz the power of the filtered signal is 50% of the power of the original signal (and the output amplitude will be about 71% of the input amplitude).

The gain of a filter (the ratio between the output and input powers) is usually expressed in the decibel (dB) unit.

The decibel (dB) is a logarithmic unit used to express the ratio between two values.

In the case of the filter gain measured in the decibel unit:

Where $A_{out}$ and $A_{in}$ are respectively the amplitudes of the output (filtered) and input (raw) signals.

For instance, the critical or cutoff frequency for a filter, the frequency where the power (the amplitude squared) of the filtered signal is half of the power of the input signal, is given in decibel as:

$$ 10\,log\left(0.5\right) \approx -3 dB $$If the power of the filtered signal is twice the power of the input signal, because of the logarithm, the gain in decibel is $10\,log\left(2\right) \approx 3 dB$.

If the output power is attenuated by ten times, the gain is $10\,log\left(0.1\right) \approx -10 dB$, but if the output amplitude is attenuated by ten times, the gain is $20\,log\left(0.1\right) \approx -20 dB$, and if the output amplitude is amplified by ten times, the gain is $20 dB$.

For each 10-fold variation in the amplitude ratio, there is an increase (or decrease) of $20 dB$.

The decibel unit is useful to represent large variations in a measurement, for example, $-120 dB$ represents an attenuation of 1,000,000 times.

A decibel is one tenth of a bel, a unit named in honor of Alexander Graham Bell.

A common filter employed in biomechanics and motor control fields is the Butterworth filter. This filter is used because its simple design, it has a more flat frequency response and linear phase response in the pass and stop bands, and it is simple to use.

The Butterworth filter is a recursive filter (IIR) and both $a$ and $b$ filter coefficients are used in its implementation.

Let's implement the Butterworth filter. We will use the function `butter`

to calculate the filter coefficients:

`butter(N, Wn, btype='low', analog=False, output='ba')`

Where `N`

is the order of the filter, `Wn`

is the cutoff frequency specified as a fraction of the Nyquist frequency (half of the sampling frequency), and `btype`

is the type of filter (it can be any of {'lowpass', 'highpass', 'bandpass', 'bandstop'}, the default is 'lowpass'). See the help of `butter`

for more details. The filtering itself is performed with the function `lfilter`

:

`lfilter(b, a, x, axis=-1, zi=None)`

Where `b`

and `a`

are the Butterworth coefficients calculated with the function `butter`

and `x`

is the variable with the data to be filtered.

In [4]:

```
from scipy import signal
freq = 100
t = np.arange(0, 1, .01)
w = 2*np.pi*1 # 1 Hz
y = np.sin(w*t) + 0.1*np.sin(10*w*t)
# Butterworth filter
b, a = signal.butter(2, 5/(freq/2), btype = 'low')
y2 = signal.lfilter(b, a, y) # standard filter
# plot
fig, ax1 = plt.subplots(1, 1, figsize=(9, 4))
ax1.plot(t, y, 'r.-', linewidth=2, label = 'raw data')
ax1.plot(t, y2, 'b.-', linewidth=2, label = 'filter @ 5 Hz')
ax1.legend(frameon=False, fontsize=14)
ax1.set_xlabel("Time [s]")
ax1.set_ylabel("Amplitude")
plt.show()
```

The plot above shows that the Butterworth filter introduces a phase (a delay or lag in time) between the raw and the filtered signals. We will see how to account for that later.

Let's look at the values of the `b`

and `a`

Butterworth filter coefficients for different orders and see a characteristic of them; from the general difference equation shown earlier, it follows that the sum of the `b`

coefficients minus the sum of the `a`

coefficients (excluding the first coefficient of `a`

) is one:

In [5]:

```
from scipy import signal
print('Low-pass Butterworth filter coefficients')
b, a = signal.butter(1, .1, btype = 'low')
print('Order 1:', '\nb:', b, '\na:', a, '\nsum(b)-sum(a):', np.sum(b)-np.sum(a[1:]))
b, a = signal.butter(2, .1, btype = 'low')
print('Order 2:', '\nb:', b, '\na:', a, '\nsum(b)-sum(a):', np.sum(b)-np.sum(a[1:]))
```

How much the amplitude of the filtered signal is attenuated in relation to the amplitude of the raw signal (gain or magnitude) as a function of frequency is given in the frequency response plot. The plots of the frequency and phase responses (the bode plot) of this filter implementation (Butterworth, lowpass at 5 Hz, second-order) is shown below:

In [6]:

```
from scipy import signal
b, a = signal.butter(2, 5/(freq/2), btype = 'low')
w, h = signal.freqz(b, a) # compute the frequency response of a digital filter
angles = np.rad2deg(np.unwrap(np.angle(h))) # angle of the complex argument
w = w/np.pi*freq/2 # angular frequency from radians to Hz
h = 20*np.log10(np.absolute(h)) # in decibels
fig, (ax1, ax2) = plt.subplots(2, 1, sharex = True, figsize=(9, 6))
ax1.plot(w, h, linewidth=2)
ax1.set_ylim(-80, 1)
ax1.set_title('Frequency response')
ax1.set_ylabel("Magnitude [dB]")
ax1.plot(5, -3.01, 'ro')
ax11 = plt.axes([.16, .59, .2, .2]) # inset plot
ax11.plot(w, h, linewidth=2)
ax11.plot(5, -3.01, 'ro')
ax11.set_ylim([-6, .5])
ax11.set_xlim([0, 10])
ax2.plot(w, angles, linewidth=2)
ax2.set_title('Phase response')
ax2.set_xlabel("Frequency [Hz]")
ax2.set_ylabel("Phase [degrees]")
ax2.plot(5, -90, 'ro')
plt.show()
```

The inset plot in the former figure shows that at the cutoff frequency (5 Hz), the power of the filtered signal is indeed attenuated by 3 dB.

The phase-response plot shows that at the cutoff frequency, the Butterworth filter presents about 90 degrees of phase between the raw and filtered signals. A 5 Hz signal has a period of 0.2 s and 90 degrees of phase corresponds to 0.05 s of lag. Looking at the plot with the raw and filtered signals employing or not the phase correction, we can see that the delay is indeed about 0.05 s.

The order of a filter is related to the inclination of the 'wall' in the frequency response plot that attenuates or not the input signal at the vicinity of the cutoff frequency. A vertical wall exactly at the cutoff frequency would be ideal but this is impossble to implement.

A Butterworth filter of first order attenuates 6 dB of the power of the signal each doubling of the frequency (per octave) or, which is the same, attenuates 20 dB each time the frequency varies by an order of 10 (per decade). In more technical terms, one simply says that a first-order filter rolls off -6 dB per octave or that rolls off -20 dB per decade. A second-order filter rolls off -12 dB per octave (-40 dB per decade), and so on, as shown in the next figure.

In [7]:

```
from butterworth_plot import butterworth_plot
butterworth_plot()
```

The phase introduced by the Butterworth filter can be corrected in the digital implementation by cleverly filtering the data twice, once forward and once backwards. So, the lag introduced in the first filtering is zeroed by the same lag in the opposite direction at the second pass. The result is a zero-phase shift (or zero-phase lag) filtering.

However, because after each pass the output power at the cutoff frequency is attenuated by two, by passing twice the second order Butterworth filter, the final output power will be attenuated by four. We have to correct the actual cutoff frequency value so that when employing the two passes, the filter will attenuate only by two.

The following formula gives the desired cutoff frequency for a second-order Butterworth filter according to the number of passes, $n$, (see Winter, 2009):

For instance, for two passes, $n=2$, $ C=\sqrt[4]{2^{\frac{1}{2}} - 1} \approx 0.802 $.

The actual filter cutoff frequency will be:

For instance, for a second-order Butterworth filter with zero-phase shift and a desired 10 Hz cutoff frequency, the actual cutoff frequency should be 12.47 Hz.

Let's implement this forward and backward filtering using the function `filtfilt`

and compare with the single-pass filtering we just did it.

In [8]:

```
from scipy.signal import butter, lfilter, filtfilt
freq = 100
t = np.arange(0, 1, .01)
w = 2*np.pi*1 # 1 Hz
y = np.sin(w*t) + 0.1*np.sin(10*w*t)
# Butterworth filter
b, a = butter(2, 5/(freq/2), btype = 'low')
y2 = lfilter(b, a, y) # standard filter
# Correct the cutoff frequency for the number of passes in the filter
C = 0.802
b, a = butter(2, (5/C)/(freq/2), btype = 'low')
y3 = filtfilt(b, a, y) # filter with phase shift correction
# plot
fig, ax1 = plt.subplots(1, 1, figsize=(9, 4))
ax1.plot(t, y, 'r.-', linewidth=2, label = 'raw data')
ax1.plot(t, y2, 'b.-', linewidth=2, label = 'filter @ 5 Hz')
ax1.plot(t, y3, 'g.-', linewidth=2, label = 'filtfilt @ 5 Hz')
ax1.legend(frameon=False, fontsize=14)
ax1.set_xlabel("Time [s]")
ax1.set_ylabel("Amplitude")
plt.show()
```

Here are four different versions of a function to implement the moving-average filter:

In [9]:

```
def moving_averageV1(x, window):
"""Moving average of 'x' with window size 'window'."""
y = np.empty(len(x)-window+1)
for i in range(len(y)):
y[i] = np.sum(x[i:i+window])/window
return y
def moving_averageV2(x, window):
"""Moving average of 'x' with window size 'window'."""
xsum = np.cumsum(x)
xsum[window:] = xsum[window:] - xsum[:-window]
return xsum[window-1:]/window
def moving_averageV3(x, window):
"""Moving average of 'x' with window size 'window'."""
return np.convolve(x, np.ones(window)/window, 'same')
from scipy.signal import lfilter
def moving_averageV4(x, window):
"""Moving average of 'x' with window size 'window'."""
return lfilter(np.ones(window)/window, 1, x)
```

Let's test these versions:

In [10]:

```
x = np.random.randn(300)/10
x[100:200] += 1
window = 10
y1 = moving_averageV1(x, window)
y2 = moving_averageV2(x, window)
y3 = moving_averageV3(x, window)
y4 = moving_averageV4(x, window)
# plot
fig, ax = plt.subplots(1, 1, figsize=(10, 5))
ax.plot(x, 'b-', linewidth=1, label = 'raw data')
ax.plot(y1, 'y-', linewidth=2, label = 'moving average V1')
ax.plot(y2, 'm--', linewidth=2, label = 'moving average V2')
ax.plot(y3, 'r-', linewidth=2, label = 'moving average V3')
ax.plot(y4, 'g-', linewidth=2, label = 'moving average V4')
ax.legend(frameon=False, loc='upper right', fontsize=12)
ax.set_xlabel("Data #")
ax.set_ylabel("Amplitude")
plt.show()
```

A test of the performance of the four versions (using the magick IPython function `timeit`

):

In [11]:

```
%timeit moving_averageV1(x, window)
%timeit moving_averageV2(x, window)
%timeit moving_averageV3(x, window)
%timeit moving_averageV4(x, window)
```

The version with the cumsum function produces identical results to the first version of the moving average function but it is much faster (the fastest of the four versions).

Only the version with the convolution function produces a result without a phase or lag between the input and output data, although we could improve the other versions to acount for that (for example, calculating the moving average of `x[i-window/2:i+window/2]`

and using `filtfilt`

instead of `lfilter`

).

And avoid as much as possible the use of loops in Python! The version with the for loop is about one hundred times slower than the other versions.

The root-mean square (RMS) is a measure of the absolte amplitude of the data and it is useful when the data have positive and negative valuess. The RMS is defined as:

$$ RMS = \sqrt{\frac{1}{N}\sum_{i=1}^{N} x_i^2} $$Similar to the moving-average measure, the moving RMS is defined as:

$$ y[i] = \sqrt{\sum_{j=0}^{m-1} (x[i+j])^2} \;\;\;\; for \;\;\; i=1, \; \dots, \; n-m+1 $$Here are two implementations for a moving-RMS filter (very similar to the moving-average filter):

In [12]:

```
import numpy as np
from scipy.signal import filtfilt
def moving_rmsV1(x, window):
"""Moving RMS of 'x' with window size 'window'."""
window = 2*window + 1
return np.sqrt(np.convolve(x*x, np.ones(window)/window, 'same'))
def moving_rmsV2(x, window):
"""Moving RMS of 'x' with window size 'window'."""
return np.sqrt(filtfilt(np.ones(window)/(window), [1], x*x))
```

Let's filter electromyographic data:

In [13]:

```
# load data file with EMG signal
data = np.loadtxt('./../data/emg.csv', delimiter=',')
data = data[300:1000,:]
time = data[:, 0]
data = data[:, 1] - np.mean(data[:, 1])
```

In [14]:

```
window = 50
y1 = moving_rmsV1(data, window)
y2 = moving_rmsV2(data, window)
```

In [15]:

```
# plot
fig, ax = plt.subplots(1, 1, figsize=(9, 5))
ax.plot(time, data, 'k-', linewidth=1, label = 'raw data')
ax.plot(time, y1, 'r-', linewidth=2, label = 'moving RMS V1')
ax.plot(time, y2, 'b-', linewidth=2, label = 'moving RMS V2')
ax.legend(frameon=False, loc='upper right', fontsize=12)
ax.set_xlabel("Time [s]")
ax.set_ylabel("Amplitude")
ax.set_ylim(-.1, .1)
plt.show()
```

Similar, but not the same, results.
An advantage of the filter empolying the convolution method is that it behaves better to abrupt changes in the data, such as when filtering data that change from a baseline at zero to large positive values. The filter with the `filter`

or `filtfilt`

function would introduce negative values in this case.

Another advantage for the convolution method is that it is much faster:

In [16]:

```
print('Filter with convolution:')
%timeit moving_rmsV1(data, window)
print('Filter with filtfilt:')
%timeit moving_rmsV2(data, window)
```

The moving-median filter is similar in concept than the other moving filters but uses the median instead. This filter has a sharper response to abrupt changes in the data than the moving-average filter:

In [17]:

```
from scipy.signal import medfilt
x = np.random.randn(300)/10
x[100:200] += 1
window = 11
y = np.convolve(x, np.ones(window)/window, 'same')
y2 = medfilt(x, window)
# plot
fig, ax = plt.subplots(1, 1, figsize=(10, 4))
ax.plot(x, 'b-', linewidth=1, label = 'raw data')
ax.plot(y, 'r-', linewidth=2, label = 'moving average')
ax.plot(y2, 'g-', linewidth=2, label = 'moving median')
ax.legend(frameon=False, loc='upper right', fontsize=12)
ax.set_xlabel("Data #")
ax.set_ylabel("Amplitude")
plt.show()
```

The library pandas has several types of moving-filter functions.

How to remove noise from a signal is rarely a trivial task and this problem gets worse with numerical differentiation of the data because the amplitudes of the noise with higher frequencies than the signal are amplified with differentiation (for each differentiation step, the SNR decreases).

To demonstrate this problem, consider the following function representing some experimental data:

The first component, with large amplitude (1) and small frequency (1 Hz), represents the signal and the second component, with small amplitude (0.1) and large frequency (10 Hz), represents the noise. The signal-to-noise ratio (SNR) for these data is equal to (1/0.1)$^2$ = 100. Let's see what happens with the SNR for the first and second derivatives of $f$:

$$ f\:'\:= \omega cos(\omega t) + \omega cos(10\omega t) $$$$ f\:''= -\omega^2 sin(\omega t) - 10\omega^2 sin(10\omega t) $$For the first derivative, SNR = 1, and for the second derivative, SNR = 0.01!

The following plots illustrate this problem:

In [18]:

```
t = np.arange(0,1,.01)
w = 2*np.pi*1 # 1 Hz
#signal and noise derivatives:
s = np.sin(w*t); n = 0.1*np.sin(10*w*t)
sd = w*np.cos(w*t); nd = w*np.cos(10*w*t)
sdd = -w*w*np.sin(w*t); ndd = -w*w*10*np.sin(10*w*t)
plt.rc('axes', labelsize=16, titlesize=16)
plt.rc('xtick', labelsize=12)
plt.rc('ytick', labelsize=12)
fig, (ax1,ax2,ax3) = plt.subplots(3, 1, sharex = True, figsize=(8, 6))
ax1.set_title('Differentiation of signal and noise')
ax1.plot(t, s, 'b.-', linewidth=1, label = 'signal')
ax1.plot(t, n, 'g.-', linewidth=1, label = 'noise')
ax1.plot(t, s+n, 'r.-', linewidth=2, label = 'signal+noise')
ax2.plot(t, sd, 'b.-', linewidth=1)
ax2.plot(t, nd, 'g.-', linewidth=1)
ax2.plot(t, sd + nd, 'r.-', linewidth=2)
ax3.plot(t, sdd, 'b.-', linewidth=1)
ax3.plot(t, ndd, 'g.-', linewidth=1)
ax3.plot(t, sdd + ndd, 'r.-', linewidth=2)
ax1.legend(frameon=False, fontsize=10)
ax1.set_ylabel('f')
ax2.set_ylabel("f '")
ax3.set_ylabel("f ''")
ax3.set_xlabel("Time (s)")
fig.tight_layout(pad=0)
plt.show()
```

Let's see how the use of a low-pass Butterworth filter can attenuate the high-frequency noise and how the derivative is affected.

We will also calculate the Fourier transform of these data to look at their frequencies content.

In [19]:

```
from scipy import signal, fftpack
freq = 100
t = np.arange(0,1,.01);
w = 2*np.pi*1 # 1 Hz
y = np.sin(w*t)+0.1*np.sin(10*w*t)
# Butterworth filter
# Correct the cutoff frequency for the number of passes in the filter
C = 0.802
b, a = signal.butter(2, (5/C)/(freq/2), btype = 'low')
y2 = signal.filtfilt(b, a, y)
# 2nd derivative of the data
ydd = np.diff(y,2)*freq*freq # raw data
y2dd = np.diff(y2,2)*freq*freq # filtered data
# frequency content
yfft = np.abs(fftpack.fft(y))/(y.size/2) # raw data
y2fft = np.abs(fftpack.fft(y2))/(y.size/2) # filtered data
freqs = fftpack.fftfreq(y.size, 1./freq)
yddfft = np.abs(fftpack.fft(ydd))/(ydd.size/2)
y2ddfft = np.abs(fftpack.fft(y2dd))/(ydd.size/2)
freqs2 = fftpack.fftfreq(ydd.size, 1./freq)
```

And the plots:

In [20]:

```
fig, ((ax1,ax2),(ax3,ax4)) = plt.subplots(2, 2, figsize=(11, 5))
ax1.set_title('Temporal domain', fontsize=14)
ax1.plot(t, y, 'r', linewidth=2, label = 'raw data')
ax1.plot(t, y2, 'b', linewidth=2, label = 'filtered @ 5 Hz')
ax1.set_ylabel('f')
ax1.legend(frameon=False, fontsize=12)
ax2.set_title('Frequency domain', fontsize=14)
ax2.plot(freqs[:yfft.size/4], yfft[:yfft.size/4],'r', linewidth=2,label='raw data')
ax2.plot(freqs[:yfft.size/4],y2fft[:yfft.size/4],'b--',linewidth=2,label='filtered @ 5 Hz')
ax2.set_ylabel('FFT(f)')
ax2.legend(frameon=False, fontsize=12)
ax3.plot(t[:-2], ydd, 'r', linewidth=2, label = 'raw')
ax3.plot(t[:-2], y2dd, 'b', linewidth=2, label = 'filtered @ 5 Hz')
ax3.set_xlabel('Time [s]')
ax3.set_ylabel("f ''")
ax4.plot(freqs[:yddfft.size/4], yddfft[:yddfft.size/4], 'r', linewidth=2, label = 'raw')
ax4.plot(freqs[:yddfft.size/4],y2ddfft[:yddfft.size/4],'b--',linewidth=2, label = 'filtered @ 5 Hz')
ax4.set_xlabel('Frequency [Hz]')
ax4.set_ylabel("FFT(f '')");
```

In 1977, Pezzack, Norman and Winter published a paper where they investigated the effects of differentiation and filtering processes on experimental data (the angle of a bar manipulated in space). Since then, these data have became a benchmark to test new algorithms. Let's work with these data (available at http://isbweb.org/data/pezzack/index.html). The data have the angular displacement measured by video and the angular acceleration directly measured by an accelerometer, which we will consider as the true acceleration.

In [21]:

```
# load data file
time, disp, disp2, aacc = np.loadtxt('./../data/Pezzack.txt', skiprows=6, unpack=True)
dt = np.mean(np.diff(time))
# plot data
fig, (ax1,ax2) = plt.subplots(1, 2, sharex = True, figsize=(11, 4))
plt.suptitle("Pezzack's benchmark data", fontsize=20)
ax1.plot(time, disp, 'b.-')
ax1.set_xlabel('Time [s]')
ax1.set_ylabel('Angular displacement [rad]', fontsize=12)
ax2.plot(time, aacc, 'g.-')
ax2.set_xlabel('Time [s]')
ax2.set_ylabel('Angular acceleration [rad/s$^2$]', fontsize=12)
plt.subplots_adjust(wspace=0.3)
```

The challenge is how to obtain the acceleration using the disclacement data dealing with the noise.

A simple double differentiation of these data will amplify the noise:

In [22]:

```
# acceleration using the 2-point forward difference algorithm:
aacc2 = np.diff(disp,2)/dt/dt # aacc2 has 2 points less than aacc
# plot data
fig, ax1 = plt.subplots(1, 1, figsize=(11, 4))
plt.suptitle("Pezzack's benchmark data", fontsize=20)
ax1.plot(time, aacc, 'g', label='Analog acceleration (true value)')
ax1.plot(time[1:-1], aacc2, 'r', label='Acceleration by 2-point difference')
ax1.set_xlabel('Time [s]', fontsize=12)
ax1.set_ylabel('Angular acceleration [rad/s$^2$]', fontsize=12)
plt.legend(frameon=False, fontsize=12, loc='upper left');
```

The source of noise in these data is due to random small errors in the digitization process which occur at each frame, because that the frequency content of the noise is up to half of the sampling frequency, higher the frequency content of the movement being analyzed.

Let's try different filters (Butterworth, Savitzky-Golay, and spline) to attenuate this noise.

Both Savitzky-Golay and the spline functions are based on fitting polynomials to the data and they allow to differentiate the polynomials in order to get the derivatives of the data (instead of direct numerical differentiation of the data).

The Savitzky-Golay and the spline functions have the following signatures:

`savgol_filter(x, window_length, polyorder, deriv=0, delta=1.0, axis=-1, mode='interp', cval=0.0)`

`splrep(x, y, w=None, xb=None, xe=None, k=3, task=0, s=None, t=None, full_output=0, per=0, quiet=1)`

And to evaluate the spline derivatives:

`splev(x, tck, der=0, ext=0)`

And let's employ the root-mean-square error (RMSE) metric to compare their performance:

In [23]:

```
from scipy import signal, interpolate
# Butterworth filter
# Correct the cutoff frequency for the number of passes in the filter
C = 0.802
b, a = signal.butter(2, (9/C)/((1/dt)/2))
dispBW = signal.filtfilt(b, a, disp)
aaccBW = np.diff(dispBW, 2)/dt/dt # aaccBW has 2 points less than aacc
# Add (pad) data to the extremities to avoid problems with filtering
disp_pad = signal._arraytools.odd_ext(disp, n=11)
time_pad = signal._arraytools.odd_ext(time, n=11)
# Savitzky-Golay filter
aaccSG = signal.savgol_filter(disp_pad,window_length=5,polyorder=3,deriv=2,delta=dt)[11:-11]
# Spline smoothing
tck = interpolate.splrep(time_pad, disp_pad, k=5, s=0.15*np.var(disp_pad)/np.size(disp_pad))
aaccSP = interpolate.splev(time_pad, tck, der=2)[11:-11]
# RMSE:
rmseBW = np.sqrt(np.mean((aaccBW-aacc[1:-1])**2))
rmseSG = np.sqrt(np.mean((aaccSG-aacc)**2))
rmseSP = np.sqrt(np.mean((aaccSP-aacc)**2))
```

And the plots:

In [24]:

```
# plot data
fig, ax1 = plt.subplots(1, 1, figsize=(11, 4))
plt.suptitle("Pezzack's benchmark data", fontsize=20)
ax1.plot(time, aacc, 'g', label='Analog acceleration: (True value)')
ax1.plot(time[1:-1], aaccBW, 'r', label='Butterworth 9 Hz: RMSE = %0.2f' %rmseBW)
ax1.plot(time,aaccSG,'b', label='Savitzky-Golay 5 points: RMSE = %0.2f' %rmseSG)
ax1.plot(time,aaccSP,'m', label='Quintic spline, s=0.0005: RMSE = %0.2f' %rmseSP)
ax1.set_xlabel('Time [s]')
ax1.set_ylabel('Angular acceleration [rad/s$^2$]', fontsize=12)
plt.legend(frameon=False, fontsize=12, loc='upper left');
```

At this case, the Butterworth, Savitzky-Golay, and spline filters produced similar results with good fits to the original curve. However, with all of them, particularly with the spline smoothing, it is necessary some degree of tuning for choosing the right parameters. The Butterworth filter is the easiest one because the cutoff frequency choice sound more familiar for human movement analysis.

Let's now analyse the kinematic data of a ball tossed to the space. These data were obtained using Tracker, which is a free video analysis and modeling tool built on the Open Source Physics (OSP) Java framework.

The data are from the analysis of the video *balltossout.mov* from the mechanics video collection which can be obtained in the Tracker website.

In [25]:

```
t, x, y = np.loadtxt('./../data/balltoss.txt', skiprows=2, unpack=True)
dt = np.mean(np.diff(t))
print('Time interval: %f s' %dt)
print('x and y values:')
x, y
```

Out[25]:

In [26]:

```
plt.rc('axes', labelsize=14)
plt.rc('xtick', labelsize=14)
plt.rc('ytick', labelsize=14)
fig, (ax1,ax2,ax3) = plt.subplots(1, 3, figsize=(12, 3))
plt.suptitle('Kinematics of a ball toss', fontsize=20, y=1.05)
ax1.plot(x, y, 'go')
ax1.set_ylabel('y [m]')
ax1.set_xlabel('x [m]')
ax2.plot(t, x, 'bo')
ax2.set_ylabel('x [m]')
ax2.set_xlabel('Time [s]')
ax3.plot(t, y, 'ro')
ax3.set_ylabel('y [m]')
ax3.set_xlabel('Time [s]')
plt.subplots_adjust(wspace=0.35)
```

Calculate the velocity and acceleration numerically:

In [27]:

```
# forward difference algorithm:
vx, vy = np.diff(x)/dt, np.diff(y)/dt
ax, ay = np.diff(vx)/dt, np.diff(vy)/dt
# central difference algorithm:
vx2, vy2 = (x[2:]-x[:-2])/(2*dt), (y[2:]-y[:-2])/(2*dt)
ax2, ay2 = (vx2[2:]-vx2[:-2])/(2*dt), (vy2[2:]-vy2[:-2])/(2*dt)
```

In [28]:

```
fig, axarr = plt.subplots(2, 3, sharex = True, figsize=(11, 6))
axarr[0,0].plot(t, x, 'bo')
axarr[0,0].set_ylabel('x [m]')
axarr[0,1].plot(t[:-1], vx, 'bo', label='forward difference'); axarr[0,1].set_ylabel('vx [m/s]')
axarr[0,1].plot(t[1:-1], vx2, 'm+', markersize=10, label='central difference')
axarr[0,1].legend(frameon=False, fontsize=10, loc='upper left', numpoints=1)
axarr[0,2].plot(t[:-2], ax, 'bo')
axarr[0,2].set_ylabel('ax [m/s$^2$]')
axarr[0,2].plot(t[2:-2], ax2, 'm+', markersize=10)
axarr[1,0].plot(t, y, 'ro')
axarr[1,0].set_ylabel('y [m]')
axarr[1,1].plot(t[:-1], vy, 'ro')
axarr[1,1].set_ylabel('vy [m/s]')
axarr[1,1].plot(t[1:-1], vy2, 'm+', markersize=10)
axarr[1,2].plot(t[:-2], ay, 'ro')
axarr[1,2].set_ylabel('ay [m/s$^2$]')
axarr[1,2].plot(t[2:-2], ay2, 'm+', markersize=10)
axarr[1,1].set_xlabel('Time [s]')
plt.tight_layout(w_pad=-.5, h_pad=0)
plt.suptitle('Kinematics of a ball toss', fontsize=20, y=1.05);
```