موضوع البحث هو النموذج الرياضي من نمط إغناتشاك للجسم المرن ذي البنية الجزيئية , الخاضع لحقل حرارة, و يملأ في اللحظة الابتدائية, منطقة بسيطة الترابط, محدودة في الفضاء الإقليدي.
This paper concerns the mathematical model of Ignaczak kind for
the Eringen-Nowacki micropolar elastic body with six material
constants, subjected to temperature field, and initially occupying
a bounded simply connected region.
References used
Al -Hasan , M , 2015– Proving the uniqueness of solution of the stress-temperature equations for elastic body with microstructure, Journal of Al-Baath University, Vol.37, Nr.2, p.193-210
Eslami , B. R ,Hetnarski, R.B, Ignaczak, J., Noda, N., Sumi, N., Tanigawa, Y., , 2013– Theory of Elasticity and Thermal Stresses, Solid Mechanics and its Applications , Vol.197.,Springer
Gerrit van Dijk , 2013 - Distribution Theory , De Gtuyter Graduate Lectures, Deutsche Nationalbibliothek , Berlin
This paper aims to calculate regular classical and complementary, so regular total Ignaczak solutions coupled with temperature field ,occupying R3 , and with vanishing stresses and temperature on the boundary.
This paper relates to the mathematical, linear model of micropolar
hemitropic elastic, homogeneous and isotropic body, of three
dimensional state of small deformations, in the frame of the linear
coupled dynamical micropolar, hemitropic thermoelasticity with
nine material constants.
This paper concerns the mathematical, linear model of micropolar
elastic, homogeneous and isotropic body, of axisymetric state of
small deformations, in the frame of the linear theory of micropolar
elasticity with six material constants . In the p
This paper concerns the mathematical model of Ignaczak type for
the Eringen-Nowacki micropolar elastic body of six material
constants, coupled with temperature fields, and initially occupying
a bounded simply connected region in R3.
This paper relates to the mathematical, linear model of elastic,
homogeneous and isotropic body of neglected structure and
infinitesimal elastic deformations in the linear theory of elasticity;
proposed by Hooke, and shortly called (H).