Transfer functions with flat magnitude and flat delay
The-coefficient and pole-zero locations of a transfer function F(s) having m zeros and n poles may be determined by imposing a total of (m+n-l) conditions on the magnitude and phase of F(s) at the origin. If q of these conditions are used to adjust the first q even derivatives of the magnitude of F(...
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ndltd-UBC-oai-circle.library.ubc.ca-2429-400852018-01-05T17:49:56Z Transfer functions with flat magnitude and flat delay Riml, Otfried Carl Electronic networks The-coefficient and pole-zero locations of a transfer function F(s) having m zeros and n poles may be determined by imposing a total of (m+n-l) conditions on the magnitude and phase of F(s) at the origin. If q of these conditions are used to adjust the first q even derivatives of the magnitude of F(s), then (m+n-l-q) conditions may be used to adjust the first (m+n-l-q) even derivatives of the phase slope. By varying these indices m, n, and q, a family of functions may be obtained in which the Butterworth and Bessel-polynomial functions are special cases. A new approach described in this thesis yields some transfer functions which have not been treated in the literature. The step-function response is studied for the realizable solutions, and the relative merits of emphasizing flat magnitude and flat delay are compared. Applied Science, Faculty of Electrical and Computer Engineering, Department of Graduate 2012-01-14T00:39:46Z 2012-01-14T00:39:46Z 1963 Text Thesis/Dissertation http://hdl.handle.net/2429/40085 eng For non-commercial purposes only, such as research, private study and education. Additional conditions apply, see Terms of Use https://open.library.ubc.ca/terms_of_use. University of British Columbia |
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English |
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Electronic networks |
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Electronic networks Riml, Otfried Carl Transfer functions with flat magnitude and flat delay |
description |
The-coefficient and pole-zero locations of a transfer function F(s) having m zeros and n poles may be determined by imposing a total of (m+n-l) conditions on the magnitude and phase of F(s) at the origin. If q of these conditions are used to adjust the first q even derivatives of the magnitude of F(s), then (m+n-l-q) conditions may be used to adjust the first (m+n-l-q) even derivatives of the phase slope.
By varying these indices m, n, and q, a family of functions may be obtained in which the Butterworth and Bessel-polynomial functions are special cases.
A new approach described in this thesis yields some transfer functions which have not been treated in the literature.
The step-function response is studied for the realizable solutions, and the relative merits of emphasizing flat magnitude and flat delay are compared. === Applied Science, Faculty of === Electrical and Computer Engineering, Department of === Graduate |
author |
Riml, Otfried Carl |
author_facet |
Riml, Otfried Carl |
author_sort |
Riml, Otfried Carl |
title |
Transfer functions with flat magnitude and flat delay |
title_short |
Transfer functions with flat magnitude and flat delay |
title_full |
Transfer functions with flat magnitude and flat delay |
title_fullStr |
Transfer functions with flat magnitude and flat delay |
title_full_unstemmed |
Transfer functions with flat magnitude and flat delay |
title_sort |
transfer functions with flat magnitude and flat delay |
publisher |
University of British Columbia |
publishDate |
2012 |
url |
http://hdl.handle.net/2429/40085 |
work_keys_str_mv |
AT rimlotfriedcarl transferfunctionswithflatmagnitudeandflatdelay |
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1718596552344207360 |