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Descriptive solution of the inverse heat-conduction problem in the B-spline basis

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Abstract

The article presents a stable algorithm of solving an integral equation of the first kind taking into account the a priori information on the sought solution.

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Abbreviations

ϕ (x):

sought solutlon of the integral equation

K(y, x):

kernel of the integral equation

f(y):

exact right-hand side of the integral equation

\(\varphi ^{(l_i )} (x_i^* )(i = 1,...,N_r )\) :

derivative of li-th order of the function ϕ(x) at the point x *1

d1 (i=1, ..., Nr):

constraints imposed on the values\(\varphi ^{(l_i )} (x)\)

\(\tilde f_i (i = 1,...,n)\) :

measured values of the righthand side of the integral equation

ξi :

measurement noise

Pm,z,v :

domain of the descriptive solutions

\(\tilde x_i (i = 1,...,N + m + 1)\) :

nodes of the B-spline Bj,m of the m-th degree

N:

dimensionality of the domain of the solutions

αj :

coefficients of the solution in the base of the B-splines

φ(α):

quadratic functional

pi :

weighting factors contained in φ(α)

gi(α) (i=1, ..., Nr):

linear form determining the permissible domain Ω dN for the coefficientsα j

Nopt :

optimum dimensionality of the domain of the solutions

ei(N) (i=1, ..., n):

discrepancy of the i-th measurement

ϕN(x),α * :

rms solution

ϕN(x, α**):

descriptive solution of the integral equation

Literature cited

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Translated from Inzhenerno-Fizicheskii Zhurnal, Vol. 45, No. 5, pp. 760–765, November, 1983.

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Voskoboinikov, Y.E., Preobrazhenskii, N.G. Descriptive solution of the inverse heat-conduction problem in the B-spline basis. Journal of Engineering Physics 45, 1254–1258 (1983). https://doi.org/10.1007/BF01254728

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  • DOI: https://doi.org/10.1007/BF01254728

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