Results 171 to 180 of about 3,037 (220)
Fredholm integral equation of the second kind with potential kernel [PDF]
A method is used to solve the Fredholm integral equation of the second kind, which is investigated from the semi-symmetric Hertz problem for two different elastic materials in three dimensions.
M A Abdou
exaly +2 more sources
On a symptotic methods for Fredholm–Volterra integral equation of the second kind in contact problems [PDF]
A method is used to obtain the general solution of Fredholm–Volterra integral equation of the second kind in the space L2(Ω)×C(0,T),0⩽t ...
M A Abdou
exaly +2 more sources
Some of the next articles are maybe not open access.
Related searches:
Related searches:
The -method and Fredholm integral equations
Computer Methods in Applied Mechanics and Engineering, 1977Abstract Instead of using approximate methods on the equation f(x) = g(x) + λ ∫ 0 1 K(x,t)f(t) dt , the τ-method is employed to obtain the exact solution of the equation h(x) = g(x) + λ ∫ 0 1 K(x,t)h(t) dt + R(x,λ) ,The analytical from of R(x, λ) determines the type of approximation which results.
Fair, Wyman, Wimp, Jet
openaire +1 more source
Parallel solution of Fredholm integral equations
Parallel Computing, 1989Nyström and Galerkin procedures are examined numerically. In both cases, parallel variants to obtain the matrices and to solve the linear matrix systems, are performed. There results superiority of the parallel variants for a large number of discretization points or functions in the Galerkin ansatz, respectively.
Esmail Babolian, L. M. Delves
openaire +1 more source
A simplification to Fredholm’s solution to the Fredholm integral equation of the second kind
Applied Mathematics and Computation, 2007The authors provide a simplification of the solution of a Fredholm integral equation of the second kind in terms of a ratio of determinants. Combinatorial arguments allow a major simplification of Fredholm's solution formula, economizing in particular on the number of multiple integrals to evaluate.
openaire +1 more source
On Solving Fredholm Integral Equations of the First Kind
Journal of the ACM, 1977A method for numerical solution of Fredholm integral equations of the first kind is derived and illustrated The solution f(x) of the integral equation is assumed to be a sample function of a wide-sense stationary random process with known autocorrelaUon function.
SAHASRABUDHE, SC, KULKARNI, AD
openaire +3 more sources
2011
It was stated in Chapter 2 that Fredholm integral equations arise in many scientific applications. It was also shown that Fredholm integral equations can be derived from boundary value problems. Erik Ivar Fredholm (1866– 1927) is best remembered for his work on integral equations and spectral theory. Fredholm was a Swedish mathematician who established
openaire +1 more source
It was stated in Chapter 2 that Fredholm integral equations arise in many scientific applications. It was also shown that Fredholm integral equations can be derived from boundary value problems. Erik Ivar Fredholm (1866– 1927) is best remembered for his work on integral equations and spectral theory. Fredholm was a Swedish mathematician who established
openaire +1 more source
On Volterra–Fredholm Equations with Partial Integrals
Differential Equations, 2001zbMATH Open Web Interface contents unavailable due to conflicting licenses.
openaire +2 more sources
On Volterra-Fredholm integral equations
Periodica Mathematica Hungarica, 1993The Ważewski method associated with the convergence of successive approximations is used in order to obtain existence and uniqueness results for the functional-integral equation of Volterra-Fredholm type of the form \[ \begin{multlined} x(t)=F \Biggl( t,x(t), \int_ 0^ t f_ 1(t,s,x(s))ds,\dots, \int_ 0^ t f_ n(t,s,x(s))ds,\\ \int_ 0^ T g_ 1(t,s,x(s))ds,\
openaire +1 more source
On nonlinear Fredholm–Volterra integral equations with hysteresis
Applied Mathematics and Computation, 2004The author improves his earlier result concerning the existence and uniqueness of solutions of the following Fredholm-Volterra system with hysteresis \[ x(t)= g(t)+ \int^t_0 p(t,s)\phi(s, x(s), w[S[x]](s))\,ds+ \int^\infty_0 q(t,s) \psi(s, x(s), w[S[x]](s))\,ds,\tag{1} \] where \(w\) denotes a hysteresis operator and \(S\) is the superposition operator
openaire +2 more sources

