Determine: .
In this case, is the arbitrary constant from integration.
The following is a well known converging that may prove useful:
First determine what the series converges (or diverges) to; i.e, determine . Then determine ; this antiderivative will equal . Perform these two steps before evaluating at .
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To determine that S n = ∑ n = 1 ∞ n x n − 1 converges, the r a t i o t e s t can be implemented: n → ∞ lim ∣ a n a n + 1 ∣ = n → ∞ lim ∣ n x n − 1 ( n + 1 ) x n + 1 − 1 ∣ = n → ∞ lim ∣ n n + 1 x n − 1 x n ∣ ≈ n → ∞ lim ∣ x n − n + 1 ∣ = ∣ x ∣ < 1 Thus, S n converges as long as ∣ x ∣ < 1 , but the question now is to what does S n converge to?
The following is a well known g e o m e t r i c s e r i e s that converges: n = 1 ∑ ∞ x n = 1 − x 1 Notice that d x d x n = n x n − 1 ; therefore, S n = n = 1 ∑ ∞ n x n − 1 = d x d n = 1 ∑ ∞ x n = d x d 1 − x 1 = ( 1 − x ) 2 1
Determining D ( x ) using u - s u b s t i t u t i o n : D ( x ) = ∫ S n d x = ∫ ( 1 − x ) 2 1 = − ∫ u 2 d u = − 1 u − 1 + c = 1 − x 1 + c
Finally, evaluating J ( x ) at x = 0 : J ( 0 ) = D ( 0 ) − c = 1 − 0 1 + c − c = 1 1 = 1
N o t e : We can abuse the relationship of integrals and derivatives to quickly determine J ( x ) : J ( x ) = ∫ ( n = 1 ∑ ∞ n x n − 1 ) d x − c = ∫ ( d x d n = 1 ∑ ∞ x n ) d x − c = ∫ ( d x d 1 − x 1 ) d x − c J ( x ) = 1 − x 1 + c − c = 1 − x 1