Open main menu
Home
Random
Recent changes
Special pages
Community portal
Preferences
About Wikipedia
Disclaimers
Incubator escapee wiki
Search
User menu
Talk
Dark mode
Contributions
Create account
Log in
Editing
Sensor fusion
(section)
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
== Example calculations == Two example sensor fusion calculations are illustrated below. Let <math>{{x}}_1</math> and <math>{x}_2</math> denote two estimates from two independent sensor measurements, with noise [[variance]]s <math>\scriptstyle\sigma_1^2</math> and <math>\scriptstyle\sigma_2^2</math> , respectively. One way of obtaining a combined estimate <math>{{x}}_3</math> is to apply [[inverse-variance weighting]], which is also employed within the Fraser-Potter fixed-interval smoother, namely <ref name="May82">{{cite book | author = Maybeck, S. | year = 1982 | title = Stochastic Models, Estimating, and Control | publisher = Academic Press | location = River Edge, NJ }}</ref> : <math>{{x}}_3 = \sigma_3^{2} (\sigma_1^{-2}{{x}}_1 + \sigma_2^{-2}{{x}}_2)</math> , where <math> \scriptstyle\sigma_3^{2} = (\scriptstyle\sigma_1^{-2} + \scriptstyle\sigma_2^{-2})^{-1}</math> is the variance of the combined estimate. It can be seen that the fused result is simply a linear combination of the two measurements weighted by their respective [[Fisher information|information]]. It is worth noting that if <math>{{x}}</math> is a [[random variable]]. The estimates <math>{{x}}_1</math> and <math>{{x}}_2</math> will be correlated through common process noise, which will cause the estimate <math>{{x}}_3</math> to lose conservativeness. <ref>{{Cite book |last=Forsling |first=Robin |url=https://urn.kb.se/resolve?urn=urn:nbn:se:liu:diva-199098 |title=The Dark Side of Decentralized Target Tracking : Unknown Correlations and Communication Constraints |date=2023-12-15 |publisher=Linköping University Electronic Press |isbn=978-91-8075-409-5 |series=Linköping Studies in Science and Technology. Dissertations |volume=2359 |location=Linköping |language=en |doi=10.3384/9789180754101}}</ref> Another (equivalent) method to fuse two measurements is to use the optimal [[Kalman filter]]. Suppose that the data is generated by a first-order system and let <math>{\textbf{P}}_k</math> denote the solution of the filter's [[Riccati equation]]. By applying [[Cramer's rule]] within the gain calculation it can be found that the filter gain is given by:{{Citation needed|date=December 2019|reason=removed citation to predatory publisher content}} : <math> {\textbf{L}}_k = \begin{bmatrix} \tfrac{\scriptstyle\sigma_2^{2}{\textbf{P}}_k}{\scriptstyle\sigma_2^{2}{\textbf{P}}_k + \scriptstyle\sigma_1^{2}{\textbf{P}}_k + \scriptstyle\sigma_1^{2} \scriptstyle\sigma_2^{2}} & \tfrac{\scriptstyle\sigma_1^{2}{\textbf{P}}_k}{\scriptstyle\sigma_2^{2}{\textbf{P}}_k + \scriptstyle\sigma_1^{2}{\textbf{P}}_k + \scriptstyle\sigma_1^{2} \scriptstyle\sigma_2^{2}} \end{bmatrix}.</math> By inspection, when the first measurement is noise free, the filter ignores the second measurement and vice versa. That is, the combined estimate is weighted by the quality of the measurements.
Edit summary
(Briefly describe your changes)
By publishing changes, you agree to the
Terms of Use
, and you irrevocably agree to release your contribution under the
CC BY-SA 4.0 License
and the
GFDL
. You agree that a hyperlink or URL is sufficient attribution under the Creative Commons license.
Cancel
Editing help
(opens in new window)