= (1−x2)dx2d2y−2xdxdy+n(n+1)y=0 .........................................1)
This equation is called LEGENDRE'S polynomial equation .
substituting -
=y=a0xm+a1xm+1+a2xm+2+.....(a0=0),
Now , series first take of the form -
=a0m(m−1)xm−2+a1(m+1)mxm−1+.......[ar+2(m+r+2)(m+r+1)−(m+r)(m+r+1)−n(n+1)ar]xm+r+....=0
Equating to zero the co-efficient of the lowest power of x , i.e. of xm−2, we get -
=a0m(m−1)=0,m=0,1 [∵ a0=0]
Equating to zero the coefficient of xm−1 and xm−r ,we get a1(m+1)m=0.....................2)
ar+2(m+r+2)(m+r+1)−(m+r)(m+r+1)−n(n+1)ar=0...............................(3)
When m=0, (2) is satisfied and therefore ,a1=0. Then (3) gives , taking r=0,1,2........in turn ,
a2=2−n(n+1)a0 , a3=3!(n−1)(n+2)a1
a4=4.3−(n−2)(n+3)a2=4!n(n−2)(n+1)(n+3)a0
a5=5.4−(n−3)(n+4)a3=5!(n−1)(n−3)(n+2)(n+4)a1,etc
Hence for m=0 , there are two independent solutions of (1),
y1=a0(1−2!n(n+1)x2+4!(n−2)n(n+1)(n+3)x4−............4)
y2=a1(x−3!(n−1)(n+2)x3+5!(n−3)(n−1)(n+2)(n+4)x5−.....) ......................5)
When m=1 , (2) shows that a1=0. Therefore (3) gives ,
a3=a5=a7=0
and a2=3!−(n−1)(n+2)a0
a4=5!(n−3)(n−1)(n+2)(n+4)a0,etc
Thus for m=1 , we get the solution of (5) again , Hence y=y1+y2 is a general solution of (1).
So our general solution of given differential equation is y1+y2
Comments