2008 IEEE Instrumentation and Measurement Technology Conference 2008
DOI: 10.1109/imtc.2008.4547120
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A Group of Inverse Filters Based on Stabilized Solutions of Fredholm Integral Equations of the First Kind

Abstract: The main cause of dynamic errors is the sensor's frequency response limitation. One way of solving this problem is designing an ejfective inverse filter. Since the problem is ill-conditioned, a small uncertainty in the measurement will cause large deviation in reconstructed signals. The amplified noise has to be suppressed at the sacrifice of biasing in estimation. Based on stabilized solutions ofFredholm integral equations of the first kind, the paper presents a group of inverse filters from which correcting … Show more

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Cited by 8 publications
(5 citation statements)
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“…Inverse filters are commonly used in communication [1], speech processing, audio and acoustic systems [2,3], and instrumentation [4] to reverse the distortion of the signal incurred due to signal processing and transmission. The transfer characteristics of the system that caused the distortion should be known a priori and the inverse filter to be used should have a reciprocal transfer characteristic so as to result in an undistorted desired signal.…”
Section: Introductionmentioning
confidence: 99%
“…Inverse filters are commonly used in communication [1], speech processing, audio and acoustic systems [2,3], and instrumentation [4] to reverse the distortion of the signal incurred due to signal processing and transmission. The transfer characteristics of the system that caused the distortion should be known a priori and the inverse filter to be used should have a reciprocal transfer characteristic so as to result in an undistorted desired signal.…”
Section: Introductionmentioning
confidence: 99%
“…Additive colored Gaussian noise has nonflat power spectral density with correlated samples. Hence, y ( t ) is a random process and can be represented via Karhunen‐Loeve (KL) expansion as follows: yfalse(tfalse)=i=0Yiϕifalse(tfalse), where ϕ i ( t ) is the set of orthonormal basis functions, and Y i is Yi=0TKyfalse(tfalse)ϕifalse(tfalse)dt. Here, KL coefficients Y i are statistically independent random variables since the orthonormal basis functions satisfy the necessary and sufficient condition, as follows: 0TKRYYfalse(t1,t2false)ϕifalse(t2false)dt2=λiϕifalse(t1false), where t 1 , t 2 ∈[0, T K ] such that t 1 < t 2 as y ( t ) is WSS. Since the coefficients Y i are uncorrelated, it is therefore also true that RYYfalse(t1,t2false)=E[]yfalse(t1false)yfalse(t2false)=Efalse[YhYifalse]=λiδhi. Substituting y ( t ) from Equations and in gives alignleftalign-1Yialign-2=0TKn(t)normalϕi(t…”
Section: Mathematical Modeling Of Plidsmentioning
confidence: 99%
“…Since inverse filters have a frequency response which is reciprocal of the frequency response of the system which caused the distortions, it is expected that this can be corrected by using an inverse filter. A survey of the work done on the realization of inverse filters indicates that before the publication of the 1997 paper of Adrian Leuciuc [1], although there had been mention of digital inverse filters from time-to-time [2][3][4][5][6], only the 1964 paper of Burch, Green and Grote [6] had discussed earlier about the restoration and correction of time functions by the synthesis of inverse filters on analog computers. Thus, with the sole exception of [6] and before the 1997 work of Leuciuc [1], no procedure or circuit appears to have been presented in the open technical literature to realize any kind of inverse analog filters using the now prevalent analog circuit building blocks.…”
Section: Introductionmentioning
confidence: 99%