
#' ## Functions for frequency, phase, impulse and step response

#' Let's first define functions to plot filter
#' properties.

from pylab import *
import scipy.signal as signal

#Plot frequency and phase response
def mfreqz(b,a=1):
    w,h = signal.freqz(b,a)
    h_dB = 20 * log10 (abs(h))
    subplot(211)
    plot(w/max(w),h_dB)
    ylim(-150, 5)
    ylabel('Magnitude (db)')
    xlabel(r'Normalized Frequency (x$\pi$rad/sample)')
    title(r'Frequency response')
    subplot(212)
    h_Phase = unwrap(arctan2(imag(h),real(h)))
    plot(w/max(w),h_Phase)
    ylabel('Phase (radians)')
    xlabel(r'Normalized Frequency (x$\pi$rad/sample)')
    title(r'Phase response')
    subplots_adjust(hspace=0.5)

#Plot step and impulse response
def impz(b,a=1):
    l = len(b)
    impulse = repeat(0.,l); impulse[0] =1.
    x = arange(0,l)
    response = signal.lfilter(b,a,impulse)
    subplot(211)
    stem(x, response)
    ylabel('Amplitude')
    xlabel(r'n (samples)')
    title(r'Impulse response')
    subplot(212)
    step = cumsum(response)
    stem(x, step)
    ylabel('Amplitude')
    xlabel(r'n (samples)')
    title(r'Step response')
    subplots_adjust(hspace=0.5)

#' ## Lowpass FIR filter

#' Designing a lowpass FIR filter is very simple to do with SciPy, all you
#' need to do is to define the window length, cut off frequency and the
#' window.

#' The Hamming window is defined as:
#' $w(n) = \alpha - \beta\cos\frac{2\pi n}{N-1}$, where $\alpha=0.54$ and $\beta=0.46$

#' The next code chunk is executed in term mode, see the [Python script](FIR_design.py) for syntax.
#' Notice also that Pweave can now catch multiple figures/code chunk.

#+ term=True
print("I'm publishing a term chunk")

#' Let's define a highpass FIR filter, if you compare to original blog
#' post you'll notice that it has become easier since 2009. You don't
#' need to do ' spectral inversion "manually" anymore!

a = 12
b = 10
print(a+b)

#' $$
#' \sum_{i=1}^n x_i
#' $$
