
doi: 10.1007/bf01097577
The author gives sufficient conditions for the existence of a solution of the integral equation in the space \(L^ p_ n(0,w)\) \[ (1)\quad d/dx\int^{w}_{0}S(x,t)y(t)dt=g(x), \] where \(w>0\), S(x,t) is an \(n\times n\)-matrix of the form \([K_{i,j}(w_ ix-w_ jt)]^ n_{i,j=1}\), where \(K_{i,j}\in L^ q(-w_ jw,w_ iw)\), \(w_ k>0\), \(1/p+1/q=1\). The resolvent operator T is described. Equation (1) contains as a special case e.g. the equation \(\mu f(x)+\int_{\Delta}k(x- t)f(t)dt=h(x),\) \(x\in \Delta\), where \(\Delta\) is a system of nonoverlapping intervals \([a_ k,b_ k]\), \(k=1,2,...,n\), which plays an important role in elasticity theory (contact problems). Applications to some physical problems are given, as well.
Integral, integro-differential, and pseudodifferential operators, Systems of nonsingular linear integral equations, system of nonoverlapping intervals, Theories of friction (tribology), difference kernel, method of operator identities, resolvent operator, Contact in solid mechanics
Integral, integro-differential, and pseudodifferential operators, Systems of nonsingular linear integral equations, system of nonoverlapping intervals, Theories of friction (tribology), difference kernel, method of operator identities, resolvent operator, Contact in solid mechanics
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