Please use this identifier to cite or link to this item: http://hdl.handle.net/123456789/5972
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dc.contributor.authorEssel, Emmanuel K.-
dc.contributor.authorYankson, Ernest-
dc.contributor.authorNaandam, Samuel M.-
dc.date.accessioned2021-08-26T12:13:56Z-
dc.date.available2021-08-26T12:13:56Z-
dc.date.issued2013-09-01-
dc.identifier.issn23105496-
dc.identifier.urihttp://hdl.handle.net/123456789/5972-
dc.description23p:, ill.en_US
dc.description.abstractIn this paper, we prove that the Boundary Condition Constants for the Boundary Value Problem π : ( ) ( ) ( ) ( ) ( ) ( ) ( ) ( ) 4 (1) 3 (2) 2 (4) Lφ ≡ φ x + P x φ x + P x φ x + P x φ x = λφ x { ( ) ( )} 0 4 1 ( 1) ( 1) ≡ ∑ + = = − − s s rs s Urφ mrsφ a n φ b (1≤ r,s ≤ 4) can be replaced by Boundary Condition Functions and that the Boundary Condition Functions are asymptotically equivalent for large values of λ , to the Boundary Condition Functions for the corresponding Fourier problem �, given by π F : ( ) ( ) (4) x = λφ x { ( ) ( )} 0 4 ( 1) ( 1) ≡ ∑ + = − − s rs s Urφ mrsφ a n φ b (1≤ r,s ≤ 4)en_US
dc.language.isoenen_US
dc.publisherUniversity of Cape Coasten_US
dc.subjectBoundary condition functionsen_US
dc.subjectFourth order boundary value problem and asymptotic behaviouren_US
dc.titleAsymptotic behaviour of boundary condition functions for a fourth-order boundary value problemen_US
dc.typeArticleen_US
Appears in Collections:Department of Mathematics & Statistics

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