Let be an infinitely differentiable real-valued function defined on the real numbers. If , , compute the values of the derivatives , but only when is odd.
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The strategy for this problem is write f ( n 1 ) in terms of the Taylor expansion of f about x = 0 and then rearrange terms until we get something that allows us to make a conclusion about the odd derivatives of f . First, note that since f is continuous, f ( 0 ) = lim n → ∞ f ( n 1 ) = lim n → ∞ n 2 + 1 n 2 = 1 . f ( n 1 ) = n 2 + 1 n 2 n 2 + 1 n 2 n 2 + 1 − 1 − 1 − 1 = f ( 0 ) + 1 ! n f ′ ( 0 ) + 2 ! n 2 f ( 2 ) ( 0 ) + 3 ! n 3 f ( 3 ) ( 0 ) + ⋯ = 1 + 1 ! n f ′ ( 0 ) + 2 ! n 2 f ( 2 ) ( 0 ) + 3 ! n 3 f ( 3 ) ( 0 ) + ⋯ = 1 ! n f ′ ( 0 ) + 2 ! n 2 f ( 2 ) ( 0 ) + 3 ! n 3 f ( 3 ) ( 0 ) + ⋯ = 1 ! n f ′ ( 0 ) ( n 2 + 1 ) + 2 ! n 2 f ( 2 ) ( 0 ) ( n 2 + 1 ) + 3 ! n 3 f ( 3 ) ( 0 ) ( n 2 + 1 ) + ⋯ = 1 ! f ′ ( 0 ) n + 2 ! f ( 2 ) ( 0 ) + ( 1 ! f ′ ( 0 ) + 3 ! f ( 3 ) ( 0 ) ) n 1 + ( 2 ! f ( 2 ) ( 0 ) + 4 ! f ( 4 ) ( 0 ) ) n 2 1 + ( 3 ! f ( 3 ) ( 0 ) + 5 ! f ( 5 ) ( 0 ) ) n 3 1 + ⋯
The coefficients of all the odd powers of n are zero, so f ′ ( 0 ) = 0 , which implies f ( 3 ) ( 0 ) = 0 which, in turn, implies f ( 5 ) ( 0 ) = 0 , and so on. Note that you can likewise determine the even derivatives of f , but since f ′ ′ ( 0 ) = 0 , instead of all being zero, the will form an alternating sequence.