Complementary Filter Design Typical KAGRA LVDTs and Geophones using \(\mathcal{H}_\infty\) Synthesis

In this tutorial, we will synthesize optimal complementary filters for blending an LVDT and a geophone. The noise models are modeled according to KAGRA’s sensors typical noise spectrum and details of the modeling procedure can found in this tutorial: LVDT and geophone noise modeling here. The noise models are loaded with kontrol.load_transfer_function().

kontrol.ComplementaryFilter is a class for complementary filter synthesis using \(\mathcal{H}_2\) and \(\mathcal{H}_\infty\) methods. The detailed of this method is described in the arXiv article Optimal Sensor Fusion Method for Active Vibration Isolation Systems in Ground-Based Gravitational-Wave Detectors. For the purpose of complementary filter synthesis, kontrol.ComplementaryFilter requires minimal specification of noise1 and noise2 in the initialization stage. These are the tranfer function models for the sensor noises. Optional arguments include weight1 and weight2. These are the freqeuncy dependent specifications for noise1 and noise2 respectively. filter1 and filter2 can be specified if synthesis function is not need. f can also be specified as the frequency axis in Hz. kontrol.ComplementaryFilter.h2synthesis() and kontrol.ComplementaryFilter.hinfsynthesis() are the corresponding methods for synthesizing the complementary filters of a generalized plant as:

Generalized plant for complementary filter synthesis

noise1, noise2, weight1, and weight2 correspond to \(\tilde{N}_1(s)\), \(\tilde{N}_2(s)\), \(W_1(s)\), and \(W_2(s)\) in the figure. \(H_1(s)\) is the complementary filter we seek to optimize and it’s refered to filter1 in one of the attributes of kontrol.ComplementaryFilter when a synthesis method is called. The other complementary filter is simply filter2 in the attribute. kontrol.ComplementaryFilter.noise_super() is a method that estimate the amplitude spectral density of the super sensor noise.

[1]:
# Load and plot the noise models here.
import numpy as np
import matplotlib.pyplot as plt

import kontrol


f = np.logspace(-2, 1, 1024)
noise1 = kontrol.load_transfer_function("noise_lvdt.pkl")
noise2 = kontrol.load_transfer_function("noise_geophone.pkl")

plt.rcParams["font.size"] = 12
plt.figure(figsize=(6, 4))
plt.loglog(f, abs(noise1(1j*2*np.pi*f)), lw=3, label="Sensor noise 1")
plt.loglog(f, abs(noise2(1j*2*np.pi*f)), lw=3, label="Sensor noise 2")
plt.legend(loc=0)
plt.grid(which="both")
plt.ylabel(r"Amplitude spectral density ($\mu \rm{m}/\sqrt{\rm{Hz}}$)")
plt.xlabel("Frequency (Hz)")
plt.show()
../_images/tutorials_complementary_filter_synthesis_for_typical_lvdt_and_geophone_1_0.png
[2]:
# Make complementary filters here

# Read the paper for details for why these weights are chosen
weight1 = 1/noise2
weight2 = 1/noise1

comp = kontrol.ComplementaryFilter(noise1, noise2, weight1, weight2, f=f)

# Alternatively, set the attributes directly
# comp = kontrol.ComplementaryFilter()
# comp.noise1 = noise1
# comp.noise2 = noise2
# comp.weight1 = 1/noise2
# comp.weight2 = 1/noise1

_, _ = comp.hinfsynthesis()
[3]:
# Plot the filters here
plt.figure(figsize=(6, 8))
plt.subplot(211)
plt.loglog(f, abs(comp.filter1(1j*2*np.pi*f)), lw=3, label="Complementary filter 1")
plt.loglog(f, abs(comp.filter2(1j*2*np.pi*f)), lw=3, label="Complementary filter 2")
plt.legend(loc=0)
plt.grid(which="both")
plt.ylabel("Magnitude")
plt.xlabel("Frequency (Hz)")

plt.subplot(212)
plt.semilogx(f, 180/np.pi*np.angle(comp.filter1(1j*2*np.pi*f)), lw=3, label="Complementary filter 1")
plt.semilogx(f, 180/np.pi*np.angle(comp.filter2(1j*2*np.pi*f)), lw=3, label="Complementary filter 2")
plt.legend(loc=0)
plt.grid(which="both")
plt.ylabel("Phase (degree)")
plt.xlabel("Frequency (Hz)")
plt.show()
../_images/tutorials_complementary_filter_synthesis_for_typical_lvdt_and_geophone_3_0.png
[4]:
# Plot the predicted super sensor noise here
plt.figure(figsize=(6, 4))
plt.loglog(f, abs(noise1(1j*2*np.pi*f)), lw=3, label="Sensor noise 1")
plt.loglog(f, abs(noise2(1j*2*np.pi*f)), lw=3, label="Sensor noise 2")
plt.loglog(f, comp.noise_super(), lw=3, label="Super sensor noise")
plt.legend(loc=0)
plt.grid(which="both")
plt.ylabel(r"Amplitude spectral density ($\mu \rm{m}/\sqrt{\rm{Hz}}$)")
plt.xlabel("Frequency (Hz)")
plt.show()
../_images/tutorials_complementary_filter_synthesis_for_typical_lvdt_and_geophone_4_0.png
[6]:
# Output to Foton format
print("Filter 1:\n", comp.filter1.foton(root_location="n"))
print("")
print("Filter 2:\n", comp.filter2.foton(root_location="n"))
Filter 1:
 zpk([0.018186+i*0.011488;0.018186+i*-0.011488;0.048464+i*0.049906;0.048464+i*-0.049906;0.244541;0.343148+i*0.100487;0.343148+i*-0.100487;0.660487+i*0.655936;0.660487+i*-0.655936;1.53144;2.75745;9.48737;1.219e+20],[0.0185509;0.024324+i*0.073156;0.024324+i*-0.073156;0.063128+i*0.054238;0.063128+i*-0.054238;0.086811+i*0.027231;0.086811+i*-0.027231;0.0941082;0.460347;0.460394;2.76016;2.76016;2.71844e+07],0.966407,"n")

Filter 2:
 zpk([0.00560866;0.002725+i*0.009636;0.002725+i*-0.009636;0.0617431;0.0621602;0.133397;0.095793+i*0.104738;0.095793+i*-0.104738;0.4589;0.460372;2.75933;2.76016;2.7174e+07],[0.0185509;0.024324+i*0.073156;0.024324+i*-0.073156;0.063128+i*0.054238;0.063128+i*-0.054238;0.086811+i*0.027231;0.086811+i*-0.027231;0.0941082;0.460347;0.460394;2.76016;2.76016;2.71844e+07],0.0097132,"n")