The solution to the differential d x 2 d 2 y − x + 1 1 d x d y + ( x + 1 ) 2 4 y = 0 , with initial conditions y ( 0 ) = 1 , y ′ ( 0 ) = 1 can be expressed as the the curve y = f ( x ) .
The area of the above curve y = f ( x ) from x = 0 to x = e 3 2 π − 1 can be expressed as n m ∗ ( e q p π − r ) , where m , n , p , q , and r are coprime positive integers.
Find: m + n + p + q + r .
Hint: Use (and/or) prove the statement below:
Let d x 2 d 2 y + P ( x ) d x d y + Q ( x ) y = 0 and change the independent variable from x to z = z ( x ) , where z(x) is an unspecified function of x .
Show that the differential above can be transformed in this way into an equation with constant coefficients if and only if Q 2 3 Q ′ + 2 P Q is constant, in which case z = ∫ Q ( x ) d x will affect the desired result.
Note: If you which to construct such a differential choose a P ( x ) and a real constant j and solve d x d Q + 2 P ( x ) Q = j ∗ Q 2 3 for Q ( x ) , by letting w = Q − 2 1 .
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Similarly to the previous problem of this type, we can look for solutions of the form y = ( x + 1 ) m . These will work provided that m ( m − 1 ) − m + 4 = 0 and hence m = 1 ± i 3 . Matching the initial conditions gives y = 2 1 ( x 1 + i 3 + x 1 − i 3 ) . Keeping the complex numbers in makes the integral easy, being 2 1 [ 2 + i 3 1 x 2 + i 3 + 2 − i 3 1 x 2 − i 3 ] 0 e 3 2 π − 1 = 7 2 ( e 3 4 π − 1 ) making the answer 1 7 .
The last three differential equations I constructed are of the the same type. That is, they use the same theorem and construction. The last one I used was the following differential equation below.
d x 2 d 2 y − x ( x + 1 ) 1 d x d y + ( x + 1 ) 2 ( x − ln ( x + 1 ) ) 2 x 2 y = 0
If y 1 ( x ) and y 2 ( x ) are linear independent solutions to the differential equation above.
Evaluate: ∫ 0 e − 1 y 1 ( x ) 2 + y 2 ( x ) 2 d x .
Express the result to 6 decimal places.
Is there a simple substitution that would work here?
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"Of this type"...
The previous problem of yours I posted a solution was a DE of the form x 2 y ′ ′ + A x y ′ ( x ) + B y ( x ) = 0 with constants A , B . Equations of this type always permit solutions of the form y = x a , provided that a ( a − 1 ) + A a + B = 0 , a quadratic equation in a , whose two roots give the two solutions. This one just goes with powers of x + 1 instead.
My other comment in both cases is that the integration is much easier using complex numbers.
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We reduce d x 2 d 2 y − x + 1 1 d x d y + ( x + 1 ) 2 4 y = 0 to a second order differential with constant coefficients by letting z = 2 ∗ ln ( x + 1 ) .
Note: From the statement above(Hint), Q 2 3 Q ′ + 2 P Q = − 2 ⟹ z = ∫ Q ( x ) d x = 2 ∗ ∫ x + 1 1 d x = 2 ∗ l n ( x + 1 ) will reduce the above differential to a second order differential with constant coefficients.
z = 2 ∗ ln ( x + 1 ) ⟹
d x d y = d z d y ∗ ( x + 1 2 ) ⟹
and,
d x 2 d 2 y = d x d ( d z d y ∗ x + 1 2 ) = 2 ∗ ( d z d y ( − ( x + 1 ) 2 1 ) + ( x + 1 ) 1 d x d ( d z d y ) ) =
2 ∗ ( ( x + 1 ) 2 − 1 d z d y + ( x + 1 ) 1 d z d ( d z d y ) ( x + 1 ) 2 ) =
( x + 1 ) 2 4 d z 2 d 2 y − ( x + 1 ) 2 2 d z d y
Replacing d x d y and d x 2 d 2 y into the above differential we obtain:
d x 2 d 2 y − d x d y + y = 0 ⟹ m 2 − m + 1 = 0 ⟹ m = 2 1 ± 2 3 i ⟹
y ( z ) = e 2 z ∗ ( c 1 ∗ c o s ( 2 3 z ) + c 2 ∗ s i n ( 2 3 z ) ) ⟹
y ( x ) = ( x + 1 ) ∗ ( c 1 ∗ c o s ( 3 ∗ l n ( x + 1 ) ) + c 2 ∗ s i n ( 3 ∗ l n ( x + 1 ) ) )
and,
d x d y = ( 3 ∗ c 2 + c 1 ) ∗ c o s ( 3 ∗ l n ( x + 1 ) ) + ( c 2 − 3 ∗ c 1 ) ∗ s i n ( 3 ∗ l n ( x + 1 ) )
Using the initial conditions: y ( 0 ) = 1 and y ′ ( 0 ) = 1 ⟹ y ( x ) = ( x + 1 ) ∗ ( c o s ( 3 ∗ l n ( x + 1 ) ) )
Let I ( x ) = ∫ ( x + 1 ) ∗ ( c o s ( 3 ∗ l n ( x + 1 ) ) ) d x
Let u = c o s ( 3 ∗ l n ( x + 1 ) ) , d v = ( x + 1 ) d x ⟹ d u = − x + 1 3 ∗ s i n ( 3 ∗ l n ( x + 1 ) ) d x and v = 2 ( x + 1 ) 2 ⟹
I ( x ) = 2 ( x + 1 ) 2 ∗ c o s ( 3 ∗ l n ( x + 1 ) ) + 2 3 ∗ ∫ ( x + 1 ) ∗ s i n ( 3 ∗ l n ( x + 1 ) ) d x
Let u = s i n ( 3 ∗ l n ( x + 1 ) ) , d v = ( x + 1 ) d x ⟹ d u = x + 1 3 ∗ c o s ( 3 ∗ l n ( x + 1 ) ) d x and v = 2 ( x + 1 ) 2 ⟹
I ( x ) = 2 ( x + 1 ) 2 ∗ ( c o s ( 3 ∗ l n ( x + 1 ) ) + 2 3 ∗ s i n ( 3 ∗ l n ( x + 1 ) ) ) − 4 3 ∗ I ( x ) ⟹
4 7 ∗ I ( x ) = 2 ( x + 1 ) 2 ∗ ( c o s ( 3 ∗ l n ( x + 1 ) ) + 2 3 ∗ s i n ( 3 ∗ l n ( x + 1 ) ) ) ⟹
I ( x ) = 7 2 ∗ 2 ( x + 1 ) 2 ∗ ( c o s ( 3 ∗ l n ( x + 1 ) ) + 2 3 ∗ s i n ( 3 ∗ l n ( x + 1 ) ) )
⟹
Area A = I ( x ) ∣ 0 ( e 3 2 π − 1 ) = 7 2 ∗ ( e 3 4 π − 1 ) = n m ∗ ( e q p π − r )
⟹ m + n + p + q + r = 1 7 .