Sobolev type inequalities of time-periodic boundary value problems for Heaviside and Thomson cables
15 pages
English

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Sobolev type inequalities of time-periodic boundary value problems for Heaviside and Thomson cables

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15 pages
English
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Description

We consider a time-periodic boundary value problem of n th order ordinary differential operator which appears typically in Heaviside cable and Thomson cable theory. We calculate the best constant and a family of the best functions for a Sobolev type inequality by using the Green function and apply its results to the cable theory. Physical meaning of a Sobolev type inequality is that we can estimate the square of maximum of the absolute value of AC output voltage from above by the power of input voltage. MSC: 46E35, 41A44, 34B27.

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Publié le 01 janvier 2012
Nombre de lectures 9
Langue English

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Takemura et al.Boundary Value Problems2012,2012:95 http://www.boundaryvalueproblems.com/content/2012/1/95
R E S E A R C HOpen Access Sobolev type inequalities of time-periodic boundary value problems for Heaviside and Thomson cables 1* 23 14 Kazuo Takemura, Yoshinori Kametaka, Kohtaro Watanabe, Atsushi Nagaiand Hiroyuki Yamagishi
* Correspondence: takemura.kazuo@nihon-u.ac.jp 1 Liberal Arts and Basic Sciences, College of Industrial Technology, Nihon University, 2-11-1 Shinei, Narashino, 275-8576, Japan Full list of author information is available at the end of the article
Abstract We consider a time-periodic boundary value problem ofnth order ordinary differential operator which appears typically in Heaviside cable and Thomson cable theory. We calculate the best constant and a family of the best functions for a Sobolev type inequality by using the Green function and apply its results to the cable theory. Physical meaning of a Sobolev type inequality is that we can estimate the square of maximum of the absolute value of AC output voltage from above by the power of input voltage. MSC:46E35; 41A44; 34B27 Keywords:Hurwitz polynomial; Sobolev inequality; best constant; Green function; n-cascaded LRCG circuits
1 Introduction Fornwe consider the following boundary value problem for an, , . . . ,= ,nth order ordinary differential operatorP(d/dt)
BVP(n) P(d/dt)u=f(t) (i) (i) u() –u() =  (i)  uL(, )
( <t< ), (in– ), (in).
The characteristic polynomial with real coefficients
n–n   nj P(z() =z+aj) =pjz(p= ) j=j=
(.)
is assumed to be a Hurwitz polynomial with real characteristic roots –a, –a, . . . , –an–. For the sake of simplicity, we impose the following assumption.
Assumption
aa≤ ∙ ∙ ∙ ≤an–,
aj=  (j= , , . . . ,n– ).
©2012 Takemura et al.; licensee Springer. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
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