Bending Analysis of Functionally Graded Plates in the Context of Different Theories of Thermoelasticity

<table>Through-the-thickness variation of dimensionless temperature <svg height="11.6" id="M170" style="vertical-align:-0.0pt" version="1.1" viewbox="0 0 10.6125 11.6" width="10.6125" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
<g transform="matrix(.017,-0,0,-.017,.062,11.537)"><path d="M592 498l-30 -3q-13 63 -31 89q-13 19 -33.5 25.5t-75.5 6.5h-70v-493q0 -60 16 -75.5t86 -19.5v-28h-286v28q68 4 83.5 19.5t15.5 75.5v493h-62q-60 0 -83 -7t-33 -24q-12 -17 -32 -90h-29q10 116 12 180h20q10 -16 21 -20.5t34 -4.5h395q19 0 28.5 5t21.5 20h21
q2 -89 11 -177z" id="x54"></path></g>
</svg> of FGM square plate for different values of the time parameter <svg height="10.125" id="M171" style="vertical-align:-0.1638pt" version="1.1" viewbox="0 0 9.1875 10.125" width="9.1875" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
<g transform="matrix(.017,-0,0,-.017,.062,9.85)"><path d="M298 36l-68 -35q-25 -13 -42 -13q-98 0 -98 119v290h-69l-4 11l28 29h45v72l65 67l14 -2v-137h113q8 -8 6 -21t-12 -19h-107v-256q0 -96 59 -96q29 0 61 17z" id="x74"></path></g><g transform="matrix(.017,-0,0,-.017,5.247,9.85)"><path d="M113 -12q-24 0 -39.5 16t-15.5 42q0 24 16 40.5t40 16.5t40 -16.5t16 -40.5q0 -26 -16 -42t-41 -16z" id="x2E"></path></g>
</svg></table>

Mathematical Problems in Engineering

fig1

Figure 1

Figure 1: Bending Analysis of Functionally Graded Plates in the Context of Different Theories of Thermoelasticity 