Приклади рядів Тейлора поширених функцій

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Trigonometric functions: sin⁡x\sin x and cos⁡x\cos x

We will begin by finding the series for sin⁡x\sin x

The first question we must tackle, which is of the utmost importance, is:

What is sin⁡0\sin 0?

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Exponential function: exe^x

Question: if f(x)=exf(x)=e^x, what is f(0)f(0)?

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Hyperbolic Function: 11−x\frac1{1-x}

There are several ways to find the Taylor series for this function. One way is to try to get rid of the denominator:

Note that, if we multiply (1−x)(1-x) by (1+x)(1+x), we get 1−x21-x^2 by difference of squares.

Similarly, by multiplying (1−x)(1-x) by ∑n=0kxn\sum_{n=0}^k x^n, we obtain a telescoping series of ∑n=0k(xn−xn+1)\sum_{n=0}^k(x^n-x^{n+1}), which results in 1−xn+11-x^{n+1}.

Thus we have 11−x=∑n=0kxn(1−x)(∑n=0kxn)=∑n=0kxn1−xk+1\frac{1}{1-x}=\frac{\sum_{n=0}^kx^n}{(1-x)\left(\sum_{n=0}^kx^n\right)}=\frac{\sum_{n=0}^kx^n}{1-x^{k+1}}

Now, if ∣x∣>1|x|>1, as kk grows, the denominator simply gets bigger and bigger, which does not help us in "removing" the denominator. The function is not defined where x=1x=1, so we will only consider ∣x∣<1|x|<1 (we will address x=−1x=-1 later).

For ∣x∣<1|x|<1, lim⁡k→∞xk+1=0\lim_{k\to\infty} x^{k+1}=0, so 11−x=lim⁡k→∞∑n=0kxn1−xk+1=∑n=0∞xn1−0=∑n=0∞xn  for ∣x∣<1\frac1{1-x}=\lim_{k\to\infty}\frac{\sum_{n=0}^kx^n}{1-x^{k+1}}=\frac{\sum_{n=0}^\infty x^n}{1-0}=\sum_{n=0}^\infty x^n\;\text{for }|x|<1

Now, consider x=−1x=-1. The series at x=−1x=-1 is ∑n=0∞(−1)n=1−1+1−1+1−1+1−1…\sum_{n=0}^\infty(-1)^n=1-1+1-1+1-1+1-1\ldots The partial sums of this series are {1,0,1,0,1,0…}\{1,0,1,0,1,0\ldots\}. Since the series does not converge to a point, it is not a convergent series and is neither 00 nor 11 (nor is it 11−(−1)=12\frac{1}{1-(-1)}=\frac12). Therefore we consider the series only to converge for ∣x∣<1|x|<1, and not for x=−1x=-1.

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Natural Logarithm: ln⁡x\ln x

We obviously cannot have a Taylor series centered at x=0x=0 for f(x)=ln⁡x,f(x) = \ln x, so we will instead pick x=1x=1 as an obvious convenient location.

All we need to do is to start differentiating ln⁡x\ln x and hope we find a pattern. Fortunately, we will: f(x)=ln⁡xf(x) = \ln x f′(x)=1xf'(x) = \frac{1}{x} f′′(x)=−1x2f''(x) = -\frac{1}{x^2} f(3)(x)=2x3f^{(3)}(x) = \frac{2}{x^3} ...... One can easily see from the Power Rule and a straightforward proof by induction that: f(n)(x)=(−1)n−1(n−1)!xnf^{(n)}(x) = \frac{(-1)^{n-1}(n-1)!}{x^n} for all positive integers n.n. It is now clear to see that f(1)=0f(1) = 0 and f(n)(1)=(−1)n−1(n−1)!f^{(n)}(1) = (-1)^{n-1}(n-1)! for all positive integers n.n. Now, all that remains is to write out the Taylor series: f(x)=∑n=0∞f(n)(1)n!(x−1)nf(x) = \sum_{n=0}^{\infty}\frac{f^{(n)}(1)}{n!}(x-1)^n ln⁡x=∑n=1∞(−1)n−1n(x−1)n=x−11−(x−1)22+(x−1)33−(x−1)44+...\ln x = \sum_{n=1}^{\infty}\frac{(-1)^{n-1}}{n}(x-1)^n\\ = \frac{x-1}{1} - \frac{(x-1)^2}{2} + \frac{(x-1)^3}{3} - \frac{(x-1)^4}{4} + ... You will sometimes see this written as: ln⁡(x+1)=∑n=1∞(−1)n−1nxn=x1−x22+x33−x44+...\ln(x+1) = \sum_{n=1}^{\infty}\frac{(-1)^{n-1}}{n}x^n = \frac{x}{1} - \frac{x^2}{2} + \frac{x^3}{3} - \frac{x^4}{4} + ...

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e^x is 1+ x + x^2/2! + x^3/3! + .....

Type a concept, like “slope” or “photosynthesis”.

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