We want to show that y=c1ex+c2e2x is the general solution of y′′−3y′+2y=0 on any interval and find the particular solution for which y(0)=1.
Now,
y=c1ex+c2e2xy′=c1ex+2c2e2xy′′=c1+4c2e2x
Substituting y,y′,y′′ into the given DE yields;
(c1ex+4c2e2x)−3(c1ex+2c2e2x)+2(c1ex+c2e2x)=0⇒c1ex+4c2e2x−3c1ex−6c2e2x+2c1ex+2c2e2x=0⇒ex(c1−3c1+2c1)+e2x(4c2−6c2+2c2)=0⇒ex(0)+e2x(0)=0⇒0=0
Hence, we have shown that y=c1ex+c2e2x is the general solution of the given DE on any interval.
Next, at y(0)=1, we have;
1=c1+c2⇒c1=1−c2
Thus, the particular solution is for which y(0)=1 is; y=c1ex+c2e2x=(1−c2)ex+c2e2x
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