Expansions in terms of Papkovich–Fadle eigenfunctions in the problem for a half‐strip with stiffeners

Author(s):  
Mikhail D. Kovalenko ◽  
Irina V. Menshova ◽  
Alexander P. Kerzhaev ◽  
Guangming Yu
Keyword(s):  
2021 ◽  
pp. 108128652199641
Author(s):  
Mikhail D Kovalenko ◽  
Irina V Menshova ◽  
Alexander P Kerzhaev ◽  
Guangming Yu

We construct exact solutions of two inhomogeneous boundary value problems in the theory of elasticity for a half-strip with free long sides in the form of series in Papkovich–Fadle eigenfunctions: (a) the half-strip end is free and (b) the half-strip end is firmly clamped. Initially, we construct a solution of the inhomogeneous problem for an infinite strip. Subsequently, the corresponding solutions for a half-strip are added to this solution, whereby the boundary conditions at the end are satisfied. The Papkovich orthogonality relation is used to solve the inhomogeneous problem in a strip.


2020 ◽  
Vol 55 (6) ◽  
pp. 784-790
Author(s):  
M. D. Kovalenko ◽  
I. V. Menshova ◽  
A. P. Kerzhaev ◽  
G. Yu

2004 ◽  
Vol 76 (2) ◽  
pp. 247-268
Author(s):  
Kuan-Ju Chen

AbstractIn this paper, first, we study the existence of the positive solutions of the nonlinear elliptic equations in unbounded domains. The existence is affected by the properties of the geometry and the topology of the domain. We assert that if there exists a (PS)c-sequence with c belonging to a suitable interval depending by the equation, then a ground state solution and a positive higher energy solution exist, too. Next, we study the upper half strip with a hole. In this case, the ground state solution does not exist, however there exists at least a positive higher energy solution.


1964 ◽  
Vol 14 (1) ◽  
pp. 21-24 ◽  
Author(s):  
N. A. Bowen

M. L. Cartwright has given ((2), 180–181) the following theorem, together with a neat proof of it.Theorem C.Suppose that f(z) is regular andin the half-strip Sof the complex plane.Suppose also that for some constant α in α<a<βas y→∞. Then for every δ>0.uniformly asy→∞ for α+δ≦x≦β–δ.


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