Answer:
centered at x = 0.
Explanation:
Part A: The power series for g(x) can be obtained by using the formula for a geometric series with a first term of 1 and a common ratio of (x/2). Then we have:
g(x) = 4/((x+2)(x-2)) = 4/(4*(1 + x/2)*(1 - x/2))
= 1/(1 - x/2) - 1/(1 + x/2)
We can then use the power series for 1/(1-x) to find the power series for g(x):
g(x) = 1/(1 - x/2) - 1/(1 + x/2)
= (1/2) * (1 + x/2 + (x/2)^2 + (x/2)^3 + ...) - (1/2) * (1 - x/2 + (x/2)^2 - (x/2)^3 + ...)
= x + (3/4)*x^2 + (5/8)*x^3 + (35/64)*x^4 + ...
To evaluate the infinite sum when x = 1, we can substitute x = 1 into the power series and use the formula for an infinite geometric series:
g(1) = 1 + (3/4) + (5/8) + (35/64) + ...
= 1/(1 - 1/2) - 1/(1 + 1/2)
= 2 - 2/3
= 4/3
Therefore, the infinite sum when x = 1 is 4/3.
Part B: To find an upper bound for the error of the approximation sin(0.3) ≈ 0.3 - 0.3^3/3!, we can use the formula for the remainder term in a Taylor series:
Rn(x) = f^(n+1)(c) * (x-a)^(n+1) / (n+1)!
where f(x) = sin(x), a = 0.3, n = 3, and c is some number between a and x. We want to find an upper bound for |R3(0.3)|.
Taking the fourth derivative of f(x) = sin(x), we get:
f^(4)(x) = -sin(x)
Since |sin(c)| ≤ 1 for any c, we have:
|R3(0.3)| ≤ |f^(4)(c)| * (0.3-0)^4 / 4!
≤ 1 * 0.3^4 / 24
≤ 0.000625
Therefore, an upper bound for the error is 0.000625, rounded to five decimal places.
Part C: We can find the power series for h(x) by differentiating the power series for ln(1+x) term by term. The power series for ln(1+x) is:
ln(1+x) = x - x^2/2 + x^3/3 - x^4/4 + ...
Taking the derivative, we get:
h(x) = ln(1+x)'
= 1 - x + x^2 - x^3 + ...
which is the power series for (-1)^n x^n. Therefore, the power series for h(x) is:
h(x) = ∑(-1)^n x^n
centered at x = 0.