A slab of thickness L with one side (x = 0) is insulted and its other side (x = L) is maintained at a constant temperature To as shown in figure below.
A uniformly distributed internal heat source produces heat in the slab at the rate of S W/m3.
Assume the heat conduction to be steady and 1-D along x-direction. Then find the heat flux at x = L
∂2T∂x2+Sk=0
∂2T∂x2=−Sk
Integrating w.r.t. 'x'
∂T∂x=−Skx+C1
atx=0,∂T∂x=0
0=0+C1⇒C1=0
∂T∂x=−Skx
Heat flux at (x=L)=−k(∂T∂x)x=L
qx=L=−k(∂T∂x)x=L
q=−k(−Sk×L+0)
∴q=S.L