2018 IEEE Conference on Control Technology and Applications (CCTA) 2018
DOI: 10.1109/ccta.2018.8511633
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Linearly Combining Sensor Measurements Optimally to Enforce an SPR Transfer Matrix

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Cited by 4 publications
(9 citation statements)
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“…In Figure A, it is shown that all sensor combination methods yield a modified system trueG¯false(sfalse) that is fairly similar to G ( s ) below 0.3 or 0.4 rad/s. The Bode plots of trueG˜false(sfalse) in Figure B illustrate that both interior conic sensor combination techniques from Section 3 lead to modified systems that are significantly closer to G d ( s ) for frequencies less than 0.2 rad/s than the SPR sensor combination techniques from the aforementioned work . This is most likely due to the loosened restrictions of allowing trueG¯false(sfalse) to be interior conic instead of SPR, the lack of matrix equalities in the sensor combination techniques, and the addition of a weighting transfer matrix.…”
Section: Numerical Examplesmentioning
confidence: 89%
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“…In Figure A, it is shown that all sensor combination methods yield a modified system trueG¯false(sfalse) that is fairly similar to G ( s ) below 0.3 or 0.4 rad/s. The Bode plots of trueG˜false(sfalse) in Figure B illustrate that both interior conic sensor combination techniques from Section 3 lead to modified systems that are significantly closer to G d ( s ) for frequencies less than 0.2 rad/s than the SPR sensor combination techniques from the aforementioned work . This is most likely due to the loosened restrictions of allowing trueG¯false(sfalse) to be interior conic instead of SPR, the lack of matrix equalities in the sensor combination techniques, and the addition of a weighting transfer matrix.…”
Section: Numerical Examplesmentioning
confidence: 89%
“…The increase in the upper conic bound will increase the allowable lower bound on a feedback controller, but this will not have a significant effect. The resulting modified outputs with the scriptH2‐ and scriptH‐optimal techniques, respectively, are alignleftalign-1y¯conic2(t)align-2=001.010.986x(t),align-1y¯conic(t)align-2=001.020.994x(t). The scriptH2‐ and scriptH‐optimal SPR sensor combination techniques from the work of Caverly and Forbes are also implemented without any weighting transfer matrix, yielding alignleftalign-1y¯SPR2(t)align-2=000.7360.706x(t),align-1y¯SPR(t)align-2=000.9250.887x(t…”
Section: Numerical Examplesmentioning
confidence: 99%
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