We know one dimensional equation for a rod is given as,
δtδu=c2δx2δ2u
It's solution can be given as u(x,t)=(C1cos(px)+C2sin(px))e−c2p2t
At x = 0 ,u(x,t)=0=u(0,t)=C1e−c2p2t
Hence, C1=0
u(x,t)=C2sin(px)e−c2p2t
Using condition u(a,t) = 0
Hence, C2sin(px)e−c2p2t=0
But actually it is not equal to zero to get the desired solution
then, sin(px)=0
pa=nπ
Hence, p=anπ
Putting the value of p in above equation, we get
u(x,t)=C2sinanπxe−a2n2π2kt
where, n = 0,1,2,3.....
u(x,t)=∑1∞bnsinanπxe−a2n2π2kt .......(A)
It is given that u(x,0) = f(x)
So, f(x)=∑1∞bnsinanπx
then bn=a2∫0af(x)sinanπxdx (Using Fourier Sine Series)
Putting this value of bn in equation (A) we get the desired equation.
u(x,t)=∑1∞a2∫0af(x)sinanπxdx(sinanπxe−a2n2π2kt)
Comments