Let us solve the differential equation x2dx2d2y−3xdxdy+4y=x+x2lnx. For this let us use the transformation x=et. Then yx′=yt′e−t, yx2′′=(yt2′′−yt′)e−2t.
Then we get the following equation
e2t(yt2′′−yt′)e−2t−3etyt′e−t+4y=et+te2t, which is equivalent to yt2′′−4yt′+4y=et+te2t.
The characteristic equation k2−4k+4=0 of the equation yt2′′−4yt′+4y=0 is equivalent to (k−2)2=0, and hence has the solutions k1=k2=2.
It follows that the general solution of the equation yt2′′−4yt′+4y=et+te2t is y(t)=(C1+C2t)e2t+yp, where yp=aet+t2(bt+c)e2t.
Then
yp′(t)=aet+(3bt2+2ct)e2t+(bt3+ct2)2e2t=aet+(2bt3+(3b+2c)t2+2ct)e2t,
yp′′(t)=aet+(6bt2+2(3b+2c)t+2c)e2t+2(2bt3+(3b+2c)t2+2ct)e2t=aet+(4bt3+(12b+4c)t2+(6b+6c)t+2c)e2t.
Then we get aet+(4bt3+(12b+4c)t2+(6b+6c)t+2c)e2t−4(aet+(2bt3+(3b+2c)t2+2ct)e2t)+4(aet+(bt3+ct2)e2t)=et+te2t.
It follows that
aet+((6b−2c)t+2c)e2t=et+te2t.
Then we get a=1, 6b−2c=1, 2c=0, and hence a=1, b=61, c=0.
Therefore, the solution of yt2′′−4yt′+4y=et+te2t is
y(t)=(C1+C2t)e2t+et+61t3e2t.
Consequently, the solution of x2dx2d2y−3xdxdy+4y=x+x2lnx is
y(x)=(C1+C2lnx)x2+x+61x2ln3x.
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