Function satisfies the differential equation above. If and , find .
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Consider the solution of the equation to be y = u v .
And the differential equation to be of the form:-
y ′ ′ + P y ′ + Q y = F [ Where P,Q and F are functions of x]
Now evaluate y ′ and y ′ ′ in terms of u ′ , u ′ ′ , v ′ , v ′ ′ , u , v
[Here f' represents d x d f and f'' means d x 2 d 2 f respectively]
So the equation transforms to
u v ′ ′ + u ( P + u 2 u ′ ) v ′ + ( u ′ ′ + P u ′ + Q u ) v = F
Choose u such that the coefficient of v ′ becomes 0 .
So we have P + u 2 u ′ = 0
So This is a first order linear differential equation and can be easily solved
The solution is u = e 2 − 1 ∫ P d x
Now substitute this in the equation and we have :-
u ′ ′ = 2 − 1 ( P u ′ + u P ′ )
u ′ ′ = 4 P 2 u − 2 u P ′
So the final equation becomes :-
v ′ ′ + I v = S
Where I = Q − 4 1 P 2 − 2 1 P ′
And S = F e 2 1 ∫ P d x
This is a general method and can be applied in this equation .
Here P = x 1 and Q = 4 − 4 x 2 1
So here u = e ∫ 2 x − 1 d x
So u = x 1
So now solving for v we have
v ′ ′ + I v = 0
I = 4 − 4 x 2 1 − 4 x 2 1 + 2 x 2 1 [using the formula we derived earlier]
So I = 4
So the equation for v just becomes
v ′ ′ + 4 v = 0
Which is a differential equation with constant coefficient and can be solved easily using the known methods to evaluate the Complementary Functions
The roots of the Auxiliary equation is 2 i and − 2 i
So the complementary function is just v = C cos ( 2 x ) + K sin ( 2 x ) Where C and K are arbitrary constants
And the particular integral for this is just 0 because the RHS is 0
So the complete solution of the differential equation is
y = x 1 ( C cos ( 2 x ) + K sin ( 2 x ) )
Now just using the information given in the question we see that K = C = π π
So our answer becomes
1 0 π π ( cos ( 2 0 ) + sin ( 2 0 ) )
Here the " 2 0 " inside the sin and cos are taken in radians