Bon Voyage Summations!

Calculus Level 5

Let t = 2016 t = 2016 and p = ln 2 p = \ln { 2 } . If the value of

k = 1 ( 1 n = 0 k 1 e t t n n ! ) ( 1 p ) k 1 p \large\ \sum _{ k=1 }^{ \infty }{ \left( 1 - \sum _{ n=0 }^{ k-1 }{ \frac { { e }^{ -t }{ t }^{ n } }{ n! } } \right) } { \left( 1- p \right) }^{ k-1 }p

can be represented as 1 ( 1 k ) n \large\ 1 - { \left( \frac { 1 }{ k } \right) }^{ n } , where k , n k, n are natural numbers,

Find the value of n + k n + k


The answer is 2018.

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1 solution

Leonel Castillo
Jan 6, 2018

First I will compute the sum k = 1 ( 1 p ) k 1 p \sum_{k=1}^{\infty} (1-p)^{k-1} p . This is just a typical geometric series which evaluates to 1 1 . Now I will find k = 1 p ( 1 p ) k 1 n = 0 k 1 e t t n n ! \sum_{k=1}^{\infty} p (1-p)^{k-1} \sum_{n=0}^{k-1} \frac{e^{-t}t^n}{n!} .

Trying to compute that sum in the order presented seems to be impossible so I will change the order of the variables. We see that the ranges for n n and k k are 0 n k 1 0 \leq n \leq k-1 and 1 k 1 \leq k \leq \infty which is equivalent to 0 n 0 \leq n \leq \infty and n + 1 k n+1 \leq k \leq \infty thus the sum is equal to: n = 0 e t t n n ! k = n + 1 p ( 1 p ) k 1 \sum_{n=0}^{\infty} \frac{e^{-t} t^n}{n!} \sum_{k=n+1}^{\infty} p(1-p)^{k-1} . The inner sum is now a simple geometric series which evaluates to ( 1 p ) n (1-p)^n making our complete sum equal to n = 0 e t t n ( 1 p ) n n ! \sum_{n=0}^{\infty} \frac{e^{-t} t^n (1-p)^n}{n!} and we may unite both of the numbers being raised to the nth power to get e t n = 0 ( t t p ) n n ! e^{-t} \sum_{n=0}^{\infty} \frac{(t - tp)^n}{n!} . That sum is now nothing more than the Taylor series for the exponential function so it evaluates to e t e t t p = e t p = e 2016 × log 2 = ( e log 2 ) 2016 = 2 2016 = ( 1 2 ) 2016 e^{-t} e^{t - tp} = e^{-tp} = e^{-2016 \times \log 2} = (e^{\log 2})^{-2016} = 2^{-2016} = \left(\frac{1}{2} \right)^{2016} .

Uniting both results, we see that the sum of the problem is just equal to 1 ( 1 2 ) 2016 1 - \left(\frac{1}{2} \right)^{2016} .

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