I'm having an awful time understanding the following. It's from the
website,
http://math.etsu.edu/multicalc/Chap2/Chap2-4/part4.htm
Given a wave equations, the separation yields the following
solutions .
1). T( t) = A1 cos( awt) +B1 sin(awt)
2). Phi( x) = A2 cos( wx) +B2 sin( wx)
let w = n pi / l
Then the solution to the wave equation is
3). u (x,t) = [ A1 cos ( a*n*pi*t / l ) +B1 sin ( a*n*pi*t / l ) ] B2
sin ( n*pi*x/ l )
Let's apply the following ICs to the solution above:
4). u (x, 0) = f (x)
5). du/dt (x, 0) = 0
Second IC implies that Phi (x) T ' (0) = 0.
Given the T above, T ' = - a w A1 sin ( awt) + a w B1 sin (awt)
Choose T ' (0) = 0 to avoid trivial solution.
Then
6). 0 = - a w A1 sin ( 0) + a w B1 cos(0) = a w B1 = B2
(below is the part I don't understand)
As a result, we must have
7). T(t) = A1 cos ( a*n*pi*t / l )
(how does one know this? how do I go from T' to T being simplified to
above? )
then define bn = A1 B2
So subject to the ICs, we get
8). u(x,t) = bn cos (a*n*pi*t / l) sin ( n*pi*x / l)
Thanks for the help.
So, using T'(0) = 0, sin(0) = 0 and cos(0) = 1 we get 0 = a*w*B1,
hence B1 = 0.
Thus u = A1*B2*cos(a*n*pi*t/L)*sin(n*pi*x/L).
By the way: the link you posted is broken: I get a "page not found"
error.
R.G. Vickson
Typical. It worked yesterday ..
> > Then
>
> > 6). 0 = - a w A1 sin ( 0) + a w B1 cos(0) = a w B1 = B2
>
> > (below is the part I don't understand)
>
> > As a result, we must have
>
> > 7). T(t) = A1 cos ( a*n*pi*t / l )
>
> > (how does one know this? how do I go from T' to T being simplified to
> > above? )
>
> > then define bn = A1 B2
>
> > So subject to the ICs, we get
>
> > 8). u(x,t) = bn cos (a*n*pi*t / l) sin ( n*pi*x / l)
>
> > Thanks for the help.
Han de Bruijn