- The function f(x) is infinitely differentiable
- The function f(x) and all its derivatives exist at x=\xi
- The function f(x) can be expressed as a series of the form: f(x) = \sum_{k=0}^{\infty} a_k (x-\xi)^k
Differentiating term by term: \begin{align*} f(x) &= a_0 + a_1(x-\xi) + a_2(x-\xi)^2 + \cdots \\ \\ f'(x) &= a_1 + 2a_2(x-\xi) + 3a_3(x-\xi)^2 + \cdots \\ \\ f''(x) &= 2a_2 + 2\times 3 a_3(x-\xi) + 3 \times 4 a_4(x-\xi)^2 +\cdots \\ \\ f'''(x) &= 2 \times 3 a_3 + 2 \times 3 \times 4 a_4 (x-\xi) + 3 \times 4 \times 5 a_5(x-\xi)^2 + \cdots \end{align*}
Solve for f(x) around the point x=\xi: \begin{align*} f(\xi) &= a_0 \\ f'(\xi) &= a_1 \\ f''(\xi) &= 2a_2 \\ f'''(\xi) &= 2 \times 3a_3 \end{align*} this can be expressed more generally as: f^{(k)}(\xi) = a_k k! so: a_k = \frac{f^{(k)}(\xi)}{k!} Substituting this into the original series: f(x) = \sum_{k=0}^{\infty} \frac{f^{(k)}(\xi)}{k!} (x-\xi)^k This is the Taylor expansion for a single variable.
- In general the Taylor series is only valid in a small region of x values. Often the series will diverge if |x-\xi| > 1 , so in general the series is only valid for \xi - 1 \le x \le \xi + 1. However this is not the case for all functions.
- When the function f(x) is not expanded completely there is some uncertainty in the expansion, this is denoted as: f(x) = S_n(x) + R_n (x) Where S_n(x) is the sum of the first n terms and R_n (x) is the sum of the remaining terms. As n \to \infty : S_n (x) \to f(x) and R_n(x) \to 0
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