
Originally Posted by
Follower
1. without centered at π/3, the taylor series is
Σ k:[0,∞] {[(-1)^k] * [x^(2k+1)]} / {(2k+1)!}
That is, an alternator raised to the k power multiplied by x raised to the 2k+1 power
this entire quantity divided by (2k+1) factorial, which is also equal to (2k+1) * (2k)! because a factorial follows the sequence of -1 each next term.
When it is centered at π/3, you simply subtract that by x, so:
Σ k:[0,∞] {[(-1)^k] * [(x - π/3)^(2k+1)]} / {(2k+1)!}
Then write out the first four terms, so plug in 0 to 3 and add them all up. The alternator will change the sign.
2. Maclaurin is the same as Taylor, except the center, c = 0.
There is a known Maclaurin expansion for 1/(1+x)
so in this case, we'll use that to interpret x/(1+x)
1/(1+x) = Σ k:[0,∞] {[(-1)^k] * (x^k)}
x/(1+x) = x * Σ k:[0,∞] {[(-1)^k] * (x^k)}
x/(1+x) = Σ k:[0,∞] {[(-1)^k] * [x^(k + 1)]}
Notice we kept the x outside of the series first, then multiplied it into the series because of order of operations. This added one to the power counter of the x term and changed it to k+1
Now plug in 0 to 4.
3. Finding the interval of convergence relies on first taking the ratio test as the limit approaches infinity of the An+1 term divided by the An term.
lim n->infinity |An+1 / An|
set it up so you take the recipicol of An, then multiply that by the next term in the sequence (so add 1 to anywhere n is)
as you take the limit, there are various things you might get. you might be left with an x term, this will produce a valid interval. However, if you have n terms under the x term such as lim n->infinity |x/(n+1)] after you've simplified the original multiplication, than this will produce a limit of 0. If you get 0 for your limit, the radius is infinity, and the interval of convergence is what you centered the function at, in this case it was a Maclaurin series it would be {0}. **(Not the answer)
If you get infinity for your limit, produced by something like lim n->infinity x * (n+1), then your radius is infinity and your interval is (-infinity, infinity).
Now, going back to if you get just an x term, you do -1 < whatever x term here < 1
simplify the inequality so x is just in the middle, or if it was just x, then your interval would be (-1, 1)
you have to test convergence of these two points though, to see if they lie in the functions graph. Plug in each point, -1, and 1, into the series representation for the X term, not the K terms. Test convergence, and change the (-1, 1) to [-1, 1] or (-1, 1] vice versa.
Σ k:[0,∞] {[(-1)^k] * [x^(k + 1)]}
6.
f(x) = e^x the series representation is as follows
Σ k:[0,∞] (x^k) / (k)!
centered at 1
Σ k:[0,∞] [(x-1)^k] / (k)!
7. Binomial series, you modify the original term you're given 1/{[(1+x^2)]^3/2}
to
{[(1+x^2)]^-(3/2)}
So the binomal is -3/2, your x term is squared, but it is in the form of 1+x, so this is now solvable.
Binomial series = 1 + p + p(p-1) + p(p-1)(p-2) + ... = (?) you have to find out the pattern and plug into the series representation.
The series representation takes on the form of a geometric series
Σ k:[0,∞] (?) x^k, in this case x was squared so
Σ k:[0,∞] (?) x^2k
8. Approximating an integral is easy
First you have a known series for cos(x), its
Σ k:[0,∞] {[(-1)^k] * [x^(2k)]}/[(2k)!]
plugging in 1/x^2 into that series will produce
Σ k:[0,∞] {[(-1)^k] * [x^(2k - 2)]}/[(2k)!]
when you integrate
∫ Σ k:[0,∞] {[(-1)^k] * [x^(2k - 2)]}/[(2k)!]
this produces
C (constant of integration)+ all things raised to k get pulled out as constants, the x term power needs to be added by one / divided by the x term power added by 1, thus follows:
∫ Σ k:[0,∞] {[(-1)^k] * [x^(2k - 2)]}/[(2k)!] = C + Σ k:[0,∞] {[(-1)^k] * [x^(2k - 1)]}/[(2k - 1)(2k)!]
write out a few terms of the series, then plug in the limits of integration and that is the approximation.
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