000 | 02978cam a2200349 a 4500 | ||
---|---|---|---|
003 | EG-GiCUC | ||
005 | 20250223031636.0 | ||
008 | 170105s2016 ua d f m 000 0 eng d | ||
040 |
_aEG-GiCUC _beng _cEG-GiCUC |
||
041 | 0 | _aeng | |
049 | _aDeposite | ||
097 | _aPh.D | ||
099 | _aCai01.12.17.Ph.D.2016.Wa.P | ||
100 | 0 | _aWael Mahmoud Mohamed | |
245 | 1 | 0 |
_aPropagation of nonlinear, coupled thermoelastic waves in elastic media under volume force and heat supply / _cWael Mahmoud Mohamed ; Supervised A. F. Ghaleb , A. A. Mosharafa , H.A.Z.Hassan |
246 | 1 | 5 | _aانتشار الموجات المرنة الحرارية غير الخطية المتزاوحة فى الأوساط المرنة تحت تأثير قوة حجمية ومصدر حرارى حجمى |
260 |
_aCairo : _bWael Mahmoud Mohamed , _c2016 |
||
300 |
_a127 P. : _bcharts ; _c25cm |
||
502 | _aThesis (Ph.D.) - Cairo University - Faculty of Science - Department of Mathematics | ||
520 | _aAnumericalsolutionispresentedforfournonlinear, one-dimensionalboundary- value problems of thermoelasticity with variable volume force and heat supply inaslaborhalf-spaceofananisotropicelasticmaterial. Onesurfaceofthebody is subjected to a given periodic displacement and Robin thermal condition, while the other surface is kept {uFB01}xed and at zero temperature. The volume force and bulk heating simulate the e{uFB00}ect of a beam of hot particles in{uFB01}ltrating the medium and coming to rest in a layer adjacent to the boundary. Particular forms for the bulk force and heating functions are considered for de{uFB01}niteness, but other choices may be treated equally well. No phase transition is considered and the domain of the solution excludes any shock wave formation. The basic {uFB01}eld equations used in this thesis have been derived elsewhere (cf. [18]) on the basis of rigorous thermodynamics and are formulated in material coordinates, making them adequate for dealing with moving boundaries. As to the used numerical scheme, it {uFB01}nds its origin in [15,23{u2013}25] and was readapted in [62]. This is a three-level, iterative {uFB01}nite-di{uFB00}erence scheme. It has been shown to exhibit unconditional stability for the case of only one dis- placement component in [62]. This result was extended in the present Thesis to include the case of three displacement components. Based on the obtained results, the used numerical method reproduces correctly the di{uFB00}erent aspects of the process of coupled thermo-mechanical wave propagation. | ||
530 | _aIssued also as CD | ||
653 | 4 | _aElastic media | |
653 | 4 | _aThermoelastic waves | |
653 | 4 | _aVolume force and heat | |
700 | 0 |
_aAdel Attaya. Mosharafa , _eSupervisor |
|
700 | 0 |
_aAhmed FouadGhaleb , _eSupervisor |
|
700 | 0 |
_aHassan Ahmed Zaky Hassan , _eSupervisor |
|
856 | _uhttp://172.23.153.220/th.pdf | ||
905 |
_aNazla _eRevisor |
||
905 |
_aSoheir _eCataloger |
||
942 |
_2ddc _cTH |
||
999 |
_c59341 _d59341 |