Department of Electrical and Electronic Engineering
THE UNIVERSITY OF MELBOURNE, AUSTRALIA
Linear State Estimation Via Multiple Sensors Over Rate-Constrained - - PowerPoint PPT Presentation
Linear State Estimation Via Multiple Sensors Over Rate-Constrained Channels Subhrakanti Dey Joint work with Alex Leong and Girish Nair Department of Electrical and Electronic Engineering T HE U NIVERSITY OF M ELBOURNE, A USTRALIA Outline n
Department of Electrical and Electronic Engineering
THE UNIVERSITY OF MELBOURNE, AUSTRALIA
n Introduction & Motivation n Multi-terminal estimation problems n Single Sensor n Multiple Sensors n Numerical Studies n Remarks and Conclusions
n
n
q
Analog signals need to be quantized
n
q
Sensor network applications: severe bandwidth limitations
n
n
n
q
For unstable systems, states become unbounded while innovations remains of bounded variance
n
xk y1,k yM,k Fusion Center ̂ x k Sensors Process q1( ̃ y 1,k) qM( ̃ y M ,k)
n
Similar ideas of quantizing the innovations have been previously considered
n
[Nair&Evans,04] - Single sensor, stable scheme but performance difficult to analyze
n
[Msechu et al. 2008], [You et al. 2011] – Estimator not stable for unstable systems
n
[Sukhavasi and Hassibi, 2011] – Single sensor, particle filter based scheme, performance difficult to analyze
n
[Fu and deSouza, 2009] – Single sensor, logarithmic quantizer, proof of stability for bounded noise
n
Information theoretic multi-terminal estimation: CEO problem
n
+ + + Fusion centre (CEO)
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
q
if quantizer saturates, can “zoom out”
q
used to prove stability for unbounded (Gaussian) noise
n
n
n
n
q
Asymptotically optimal quantizer range and distortion given in [Hui&Neuhoff,2001], can then obtain where
q
Can generalize to lattice vector quantizers
n
q
Can obtain where
q
Difficult to generalize to vector quantizers (optimal quantizers not known in general)
n
n
n
n
n
n
n
n
n
n
n
n
n
q
Reason: For large N, quantizer saturation is rare. Choice of dv ensures that when saturation doesn’t occur.
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
xk y1,k yM,k Fusion Center ̂ x k Sensors Process q1( ̃ y 1,k) qM( ̃ y M ,k)
n
q
Sensors run individual Kalman filters using local information
q
Fusion centre combines local estimates to form global estimate
q
Global estimate same as fusion centre having access to individual sensor measurements
n
q
Can be reconstructed at fusion centre if sensors send local innovations
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
n
2 2.5 3 3.5 4 4.5 5 5.5 6 6.2 6.4 6.6 6.8 7 7.2 7.4 7.6 log2(N)
tr E[(xk ¡ ^
xkjk¡ 1 )(xk ¡ ^ xk jk¡ 1 )T ] Monte Carlo tr(P
∞)
Asymptotic tr(P
∞)
n
2 2.5 3 3.5 4 4.5 5 5.5 6 5.1 5.2 5.3 5.4 5.5 5.6 5.7 5.8 5.9 log2(N)
tr E[(xk ¡ ^
xkjk¡ 1 )(xk ¡ ^ xk jk¡ 1 )T ] Monte Carlo tr(P
∞)
Asymptotic tr(P
∞)
n
n
n
n
n
n
n
n
n
q
Packet loss and high rate quantization
q
Vector measurements: dynamic quantization for lattice vector quantizers
q
Detectability at all sensors a strong assumption
q
Low data rates?
n
Proof of stability here holds for sufficiently high bit rates
n
May need different schemes to achieve stability for lower bit rates
n
Tradeoff between estimation performance and data rate for rates close to minimum bit rates