[maths]u(x,y)=\sum_{k=0}^{\infty }\frac{4}{\pi (2k+1)}e^{\frac{-\pi (2k+1)}{h}x}sin\frac{\pi (2k+1)}{h}y[/maths]
Last night I solved for the solution above to the partial differential equation:
[maths]\frac{\partial^2u }{\partial x^2}+\frac{\partial^2u }{\partial y^2}=0[/maths]
for
x > 0
0 < y < h
modelling the steady state two dimensional heat distribution in a slab with boundary conditions:
u = 0 when y = 0, all x > 0
u = 0 when y = h, all x > 0
u approaches 0 when x = 1, for 0 < y < h
u = 1 when x = 0, for 0 < y < h
So either way I must work with π and e.