2 k = 1 ∑ ∞ k 2 f ( k ) ( x ) = 3 f ( x ) , f ( 0 ) = 2 0 1 6
Find the function f : R → R that satisfies the differential equation above for all real x . Return f ′ ( 0 ) as your answer.
If you come to the conclusion that no such function exists (or there is more than one), enter 666.
Clarification : f ( k ) ( x ) denotes the k th derivative of f ( x ) .
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Yes, f ( x ) = e λ x is a good Ansatz (+1). How do we know that there aren't any other solutions of the form f ( x ) = x k e λ x ? Also, the equation ∑ k = 1 ∞ k 2 λ k = 2 3 has three complex solutions λ ; why are you rejecting the other two, besides λ = 3 1 ?
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The characteristic equation 2 λ − λ ( 1 − λ ) − 2 3 ( 1 − λ ) 3 = 0 which follows after analyzing the infinite rows only delivers a real to real function for λ 1 = 3 1 . Of course there are additionally the solutions λ 2 , 3 = 1 − + 2 i But the range of the according functions contains complex numbers! So they must be rejected and the solution for f(x) is unique.
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The fact that the roots 1 ± 2 i are non-real is not a sufficient reason to reject them. Think about f ′ ′ ( x ) + f ( x ) = 0 : non-real solutions give rise to real solutions thanks to Euler's marvelous formula ;)
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@Otto Bretscher – Okay, so let us try to find a second solution f ( x ) = 2 0 1 6 ⋅ e x ⋅ c o s ( 2 x ) constructed as a linear combination regarding the two complex values for λ with valid initial condition.
But here we realize that the infinite sum doesn't converge. That's why we must reject the complex solutions for λ .
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@Andreas Wendler – Genau! Now your solution is just perfect
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@Otto Bretscher – We need also to show that no other form is possible.
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@Abdelhamid Saadi – We needn't because another solution doesn't exist. This follows from the roots of the characteristic polynomial for λ considering the initial condition!
Let f ( x ) = y
We want to solve the equation
2 3 y = n = 1 ∑ ∞ n 2 y ( n ) − − ( 1 )
Differentiating both sides we get
2 3 y ′ = n = 1 ∑ ∞ n 2 y ( n + 1 ) − − ( 2 )
Taking (1)-(2) we get:
2 3 ( y − y ′ ) = n = 1 ∑ ∞ ( 2 n − 1 ) y ( n ) − − ( 3 )
Now doing the same thing ((3) - (3)') we get:
2 3 ( y − 2 y ′ + y ′ ′ ) = 2 n = 1 ∑ ∞ y ( n ) − y ′ = 2 S − y ′
Rearranging:
S = 4 3 ( y − 3 4 y ′ + y ′ ′ ) − − ( 4 )
Notice that
S = ( S + y ) ′ = S ′ + y ′
Substituting that into (4) gives the differential equation:
3 y − 1 1 y ′ + 7 y ′ ′ − 3 y ′ ′ ′ = 0
Solving gives:
y = c 3 e 3 x + c 2 e x sin ( 2 x ) + c 1 e x cos ( 2 x )
It is then easy to show that c 2 and c 1 has to be 0 or the sum n = 1 ∑ ∞ n 2 y ( n ) diverges.
The rest follows suit.
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The well-known entry f ( x ) = e λ x leads to the equation k = 1 ∑ ∞ k 2 λ k = 2 3 Solution is λ = 3 1 and we get f ( x ) = 2 0 1 6 ⋅ e 3 x as well as f ′ ( 0 ) = 3 2 0 1 6 = 6 7 2