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Transfer function

About: Transfer function is a research topic. Over the lifetime, 14362 publications have been published within this topic receiving 214983 citations. The topic is also known as: system function & network function.


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Journal ArticleDOI
TL;DR: In this paper, a 2D inversion algorithm for field-based timeedomain (TD)induced polarization (IP) surveys is proposed, which is based on a 2-D complex conductivity kernel that is computed over a range of off-requencies and converted to TD through the fast Hankel transform.
Abstract: SUMMARY Field-basedtimedomain(TD)inducedpolarization(IP)surveysareusuallymodelledbytaking into account only the integral chargeability, thus disregarding spectral content. Furthermore, the effect of the transmitted waveform is commonly neglected, biasing inversion results. Given these limitations of conventional approaches, a new 2-D inversion algorithm has been developed using the full voltage decay of the IP response, together with an accurate description of the transmitter waveform and receiver transfer function. This allows reconstruction of the spectral information contained in the TD decay series. The inversion algorithm is based around a 2-D complex conductivity kernel that is computedoverarangeoffrequenciesandconvertedtotheTDthroughafastHankeltransform. Two key points in the implementation ensure that computation times are minimized. First, the speed of the Jacobian computation, time transformed from frequency domain through the same transformation adopted for the forward response is optimized. Secondly, the reduction of the number of frequencies where the forward response and Jacobian are calculated: cubic splines are used to interpolate the responses to the frequency sampling necessary in the fast Hankel transform. These features, together with parallel computation, ensure inversion times comparable with those of direct current algorithms. Thealgorithmhasbeendevelopedinalaterallyconstrainedinversionscheme,andhandles both smooth and layered inversions; the latter being helpful in sedimentary environments, where quasi-layered models often represent the actual geology more accurately than smooth minimum-structure models. In the layered inversion approach, a general method to derive the thickness derivative from the complex conductivity Jacobian is also proposed. One synthetic example of layered inversion and one field example of smooth inversion show the capability of the algorithm and illustrates a complete uncertainty analysis of the model parameters. With this new algorithm, in situ TD IP measurements give access to the spectral content of the polarization processes, opening up new applications in environmental and hydrogeophysical investigations.

100 citations

Journal ArticleDOI
TL;DR: In this work, the profile registration transfer function accounting for an error in the determined edge angle has been derived and incorporated into a Windows-based software program to be made available for general use.
Abstract: An algorithm to calculate the presampling modulation transfer function (MTF) of an imaging system from an angled edge image has its own inherent transfer function. Factors such as the angle of the sampling aperture to the edge, registration of edge function profiles using the determined edge angle, differentiation, smoothing, and folding all combine to produce the frequency response of the algorithm. In this work, the profile registration transfer function accounting for an error in the determined edge angle has been derived. This has been incorporated with other, previously reported, algorithm component transfer functions to fully characterize the MTF calculation algorithm. When registering profiles, small errors in the edge angle determination were found to result in large errors in the MTF, as the misalignment errors increase with the number of profiles. For example, registering 50 profiles a 0.07 degree error in a 7 degree edge angle (1% error) produces a 36% error in the MTF at the system cutoff frequency f=f(c) when profiles are oversampled at a frequency f(s)=8f(c)(f(c) is defined as the maximum frequency reproducible without aliasing when sampling at the limiting system Nyquist frequency f(s) = 2f(c)). These results highlight the importance of quantifying the transfer function of the algorithm used to determine an imaging system modulation transfer function. The MTF calculation algorithm and the transfer function analysis have been incorporated into a Windows-based software program to be made available for general use.

99 citations

Journal ArticleDOI
TL;DR: An application of the transfer-function approach in determining the class of all systems that share the same optimal solution is introduced, and the superiority of its computational method for systems having a small number of inputs and outputs is demonstrated.
Abstract: The transfer-function form of the stationary algebraic Riccati equation is investigated. A generalized spectral factorization technique that copes with unstable systems is introduced. This factorization is used to provide an efficient way of solving the Riccati equation and to establish the exact equivalence between the time domain and the transfer-function approaches to the linear stationary filtering and the deterministic optimal control problems. The proposed method is easily extended to cope, in the filtering problem, with coloured signals and the superiority of its computational method for systems having a small number of inputs and outputs is demonstrated. Finally, an application of the transfer-function approach in determining the class of all systems that share the same optimal solution is introduced.

99 citations

Journal ArticleDOI
TL;DR: By fitting experimentally determined edge spread function data to the analytical expression, the normalized line spread function (LSF) and the normalized modulation transfer function (MTF) can be easily calculated from four ESF fit coefficients.
Abstract: The previous work of Yin, Giger, and Doi [Med. Phys. 17, 962-966 (1990)] demonstrated that using a computerized fit of an analytic line spread function to experimentally measured data is very useful for determining the presampling modulation transfer function of an imaging system. In this report, the work of Yin et al. is extended to include an analytic expression for the edge spread function (ESF). By fitting experimentally determined edge spread function data to the analytical expression, the normalized line spread function (LSF) and the normalized modulation transfer function (MTF) can be easily calculated from four ESF fit coefficients. The extension from the line spread function to the edge spread function should be valuable in cases where slit measurements are impractical, for example, in very high resolution imaging systems where the required slit dimensions become impractically small, or in measurements of the transfer properties of scattered radiation or off-focus radiation, where large area exposures are necessary.

98 citations

Journal ArticleDOI
TL;DR: In this article, a modified phasor transformation is proposed that converts a frequency-modulated signal into an equivalent time-varying PHASOR model of the LCC resonant ballast, which explicitly models the effect of the frequency modulation on the envelopes of the outputs and facilitates ac analysis of the ballast in addition to envelope transient simulation, and is verified through comparison of experimental and simulation results.
Abstract: This paper presents analytical tools aimed at improving and simplifying the development of frequency-controlled dimming electronic ballasts. A modified phasor transformation is proposed that converts a frequency-modulated signal into an equivalent time-varying phasor. The proposed transformation is applied to develop a complete small-signal phasor model of the LCC resonant ballast, which explicitly models the effect of the frequency modulation on the envelopes of the outputs. A Spice-compatible implementation of the model is presented that facilitates ac analysis of the ballast in addition to envelope transient simulation, and is verified through comparison of experimental and simulation results. A closed-form solution of the control-to-output current transfer function for the ballast-resistor system is presented, along with key observations of the pole locations and low-frequency gain that facilitate simple and intuitive compensator design. The effects of lamp dynamics on the controller design are discussed, followed by a design example for the feedback controller.

98 citations


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Performance
Metrics
No. of papers in the topic in previous years
YearPapers
2023351
2022810
2021329
2020421
2019461
2018493