The sequence { a n } satisfies a 0 = 1 , a 1 = 2 1 3 , and a n = 2 a n − 1 + a n − 2 for all n ≥ 2 . Let S = i = 1 ∑ ∞ a i 2 − a i − 1 2 a i − 1 . What is the value of S 1 ?
This problem is shared by Muhammad A.
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This well-written solution is similar to as all other known correct solutions in using the observation that, after some manipulations, we get a telescoping series. One small issue with it (which was an issue with all submitted correct solutions) is the calculation of the telescoping series. Even though all the terms except the first one "cancel out", it does not automatically imply that the sum equals to the first term. As an example, n = 1 ∑ ∞ ( cos n 1 − cos n + 1 1 ) equals cos 1 − 1 , not just cos 1 . This is because a partial sum equals cos 1 − cos n + 1 1 , with the second term approaching 1 , not 0 as n goes to infinity. This is a small issue for an Algebra problem, but it would have been a bigger issue for an Analysis or Calculus problem.
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A very important and crucial observation. I always faced this doubt when I did not know calculus, as I could not decide whether the last term would cancel out or remain, since we do not know the parity of infinity.
So what are we supposed to do in such case?? I mean should we include the last term as well?
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Yes. Basically, we need to find what is lim n → ∞ a n .
For example, what is
n = 1 ∑ ∞ n n + 1 − n + 1 n + 2 ?
Hint: Answer is not 2.
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@Calvin Lin – Oh.. Got it!! Well, the answer should be 1, I guess.
We have: a i 2 − a i − 1 2 2 a i − 1 = ( a i + a i − 1 ) ( a i − a i − 1 ) ( a i + a i − 1 ) − ( a i − a i − 1 ) = a i − a i − 1 1 − a i + a i − 1 1 = a i − 1 + a i − 2 1 − a i + a i − 1 1 for i ≥ 2 , thus 2 S = a 1 − a 0 1 − a 1 + a 0 1 + a 1 + a 0 1 − a 2 − a 1 1 + … = a 1 − a 0 1 = 2 1 2 1 , and thus S 1 = 4 2 4
Short and sweet. If this were an Analysis question, more justification would have been required
Actually sigma runs from 1 to infinite but u started operating from i = 2
Consider that
a {i+1}-a {i}=a {i}+a {i-1}
and
\frac{a {i-1}}{a {i}^2-a {i-1}^2}=\frac{1}{2}(\frac{1}{a {i}-a {i-1}}-\frac{1}{a {i}+a_{i-1}})
for every i \in N. Hence,we have
S=\frac{1}{2}(\frac{1}{a {1}-a {0}}-\frac{1}{a {1}+a {0}})+\frac{1}{2}(\frac{1}{a {2}-a {1}}-\frac{1}{a {2}+a {1}})+\frac{1}{2}(\frac{1}{a {3}-a {2}}-\frac{1}{a {3}+a {2}})+\ldots
which equivalent with
S=\frac{1}{2}(\frac{1}{a {1}-a {0}}-\frac{1}{a {1}+a {0}})+\frac{1}{2}(\frac{1}{a {1}+a {0}}-\frac{1}{a {2}+a {1}})+\frac{1}{2}(\frac{1}{a {2}+a {1}}-\frac{1}{a {3}+a {2}})+\ldots
After several process, we get
S=\frac{1}{2}(\frac{1}{a {1}-a {0}})
which equivalent with
S=\frac{1}{2}(\frac{1}{213-1})
so that S=\frac{1}{424}. So, the value of \frac{1}{S} is 424.
Note that
a i − a i − 1 1 − a i + 1 − a i 1 = ( a i − a i − 1 ) ( a i + 1 − a i ) a i + 1 − a i − a i + a i − 1
= ( a i − a i − 1 ) ( a i + a i − 1 ) a i + 1 − 2 a i + a i − 1 = ( a i − a i − 1 ) ( a i + a i − 1 ) 2 a i − 1 = a i 2 − a i − 1 2 2 a i − 1
since a i + 1 = 2 a i + a i − 1 . Hence,
S = 2 1 i = 1 ∑ ∞ a i 2 − a i − 1 2 2 a i − 1 = 2 1 i = 1 ∑ ∞ ( a i − a i − 1 1 − a i + 1 − a i 1 )
The summation telescopes to
S = 2 1 ⋅ a 1 − a 0 1 = 4 2 4 1 ,
so S 1 = 4 2 4 .
SAME HERE !!!!
S = ∑ i = 1 ∞ ( a i + a i − 1 ) ( a i − a i − 1 ) a i − 1
= 2 1 ∑ i = 1 ∞ ( a i − a i − 1 1 − a i + a i − 1 1 ) ,
which is basically a telescoping series problem, as according to the given recurrence relation,
a i + 1 − a i = a i + a i − 1 ,
and so the second term of this expression is cancelled by the first term of the next expression as i increments & so on.
The term remaining is the first one:
S = 2 1 a 1 − a 0 1 = 4 2 4 1 .
S 1 = 4 2 4 , as required.
Using partial fractions, a i 2 − a i − 1 2 a i − 1 = 2 1 ( a i − a i − 1 1 − a i + a i − 1 1 ) .
By the recurrence relation, a i + a i − 1 = a i + 1 − a i , implying S = i = 1 ∑ ∞ 2 1 ( a i − a i − 1 1 − a i + 1 − a i 1 ) = 2 ( a 1 − a 0 ) 1 = 4 2 4 1 .
Therefore, S 1 = 4 2 4 .
Note: Here the series is calculated using the fact that it is telescoping. Formally, a partial sum of this series, after all terms in the middle cancel out, becomes a 1 − a 0 1 − a i + 1 − a i 1 . We can easily see that a i → ∞ , hence a i + 1 − a i 1 = a i + a i − 1 1 → 0 , so the sum converges to a 1 − a 0 1 .
let know that the first is 1/212
ratio:1/2
so, a/(1-r) (1/212)/2 =1/424
s=1/424 1/s=424
1 / ( ( 2 1 3 ) 2 − 1 2 ) + 2 1 3 / ( ( 2 2 1 3 + 1 ) 2 − 2 1 3 2 ) + ( 2 2 1 3 + 1 ) / ( ( 5 2 1 3 + 2 ) 2 − ( 2 2 1 3 + 1 ) 2 ) + . . . = 1 / ( 2 1 3 2 1 4 ) + 2 1 3 / ( 2 1 4 ( 3 2 1 3 + 1 ) ) + ( 2 2 1 3 + 1 ) / ( ( 3 2 1 3 + 1 ) ( 7 2 1 3 + 3 ) ) + . . . = ( 1 / 2 ) ( 1 / ( 2 1 2 ) − 1 / ( 2 1 4 ) ) + ( 1 / 2 ) ( 1 / ( 2 1 4 ) − 1 / ( 3 2 1 3 + 1 ) ) + ( 1 / 2 ) ( 1 / ( 3 2 1 3 + 1 ) − 1 / ( 7 2 1 3 + 3 ) ) + . . . = ( 1 / 2 ) ( 1 / ( 2 1 2 ) ) − ( 1 / 2 ) ( 1 / 2 1 4 ) + ( 1 / 2 ) ( 1 / 2 1 4 ) − ( 1 / 2 ) ( 1 / ( 3 2 1 3 + 1 ) + ( 1 / 2 ) ( 1 / ( 3 ∗ 2 1 3 + 1 ) ) − . . . then we get S = (1/2)(1/212) = 1/424
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The first step is to decompose the summand by partial fractions. a i 2 − a i − 1 2 a i − 1 = ( a i − a i − 1 ) ( a i + a i − 1 ) a i − 1
a i 2 − a i − 1 2 a i − 1 = 2 ( a i − a i − 1 ) 1 − 2 ( a i + a i − 1 ) 1
Now, since a n + 1 = 2 a n + a n − 1 , we get a n + 1 − a n = a n + a n − 1 . This simplifies our summand to:
2 ( a i − a i − 1 ) 1 − 2 ( a i + 1 − a i ) 1 , which telescopes, so when added, the sum will be only the first fraction.
S = 2 ( a 1 − a 0 ) 1 = 2 ( 2 1 3 − 1 ) 1 = 4 2 4 1
Giving the answer of S 1 = 4 2 4