<?xml version="1.0" encoding="UTF-8"?><xml><records><record><source-app name="Biblio" version="7.x">Drupal-Biblio</source-app><ref-type>17</ref-type><contributors><authors><author><style face="normal" font="default" size="100%">SWARN SINGH</style></author><author><style face="normal" font="default" size="100%">SURUCHI SINGH</style></author><author><style face="normal" font="default" size="100%">RAJNI ARORA</style></author></authors></contributors><titles><title><style face="normal" font="default" size="100%">NEW HIGHLY ACCURATE STABLE SCHEMES FOR THE SOLUTION OF TELEGRAPHIC EQUATION WITH NEUMANN BOUNDARY CONDITIONS</style></title><secondary-title><style face="normal" font="default" size="100%">Neural, Parallel, and Scientific Computations</style></secondary-title></titles><keywords><keyword><style  face="normal" font="default" size="100%">39A10</style></keyword></keywords><dates><year><style  face="normal" font="default" size="100%">2016</style></year><pub-dates><date><style  face="normal" font="default" size="100%">2016</style></date></pub-dates></dates><urls><web-urls><url><style face="normal" font="default" size="100%">https://acadsol.eu/npsc/articles/24/NPSC-01-14.pdf</style></url></web-urls></urls><volume><style face="normal" font="default" size="100%">24</style></volume><pages><style face="normal" font="default" size="100%">13</style></pages><language><style face="normal" font="default" size="100%">eng</style></language><abstract><style face="normal" font="default" size="100%">&lt;p&gt;In this paper, we present two new three level implicit schemes to solve telegraphic equation with Neumann boundary conditions. The accuracy of the proposed schemes is of ${ O(k^2 + k^2h^2 + h^4 ) }$ and ${O(k^4 + k^4h^2 )&amp;nbsp;}$, where ${ h &amp;gt; 0 }$ and ${ k &amp;gt; 0 }$ are the mesh sizes in the space and time directions respectively. The proposed schemes are shown to be solvable and unconditionally stable. Numerical experiments are presented to demonstrate the accuracy and efficiency of the new schemes.&lt;/p&gt;
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