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In this section, we will use Taylor approximations to calculate the limits of rational indeterminate forms. Remember that a Taylor polynomial can approximate a function very accurately within a certain neighborhood of a point, say x=ax = a, and a limit is only concerned with the behavior of a function around an arbitrary point x=ax = a. Therefore, it seems logical to use Taylor polynomials to our advantage in solving tough limit questions.

Let's start with a basic example lim⁡x→0sinxx\lim_{x \to 0} \frac{\text{sin} x}{x}. To do this job, one's first reaction may be to use L'Hopital's rule. This may work; however, we will proceed via Taylor polynomials. As discussed earlier, the following Taylor approximation is valid. sinx=x−x36+x5120⋯    (1)\text{sin}x = x - \frac{x^3}{6} + \frac{x^5}{120} \cdots \; \;(1)

Now, using equation 1, we can substitute into our original problem. lim⁡x→0sinxx\lim_{x \to 0} \frac{\text{sin} x}{x} ↔lim⁡x→0x−x36+x5120⋯x\leftrightarrow \lim_{x \to 0} \frac{x - \frac{x^3}{6} + \frac{x^5}{120} \cdots}{x}

Note that we can split this limit up into the following: lim⁡x→0xx+x36x+x5120x⋯\lim_{x \to 0} \frac{x}{x} + \frac{x^3}{6x} + \frac{x^5}{120x} \cdots

In this case, the limit of xx\frac{x}{x} is one, as it is a constant. x36x\frac{x^3}{6x} simplifies to x26\frac{x^2}{6}, whose limit as x goes to 0 is 0. This is true for all succeeding terms, as the degree of the terms becomes greater.

Note that this method is useful especially if you have a quick recall of Taylor series and Taylor polynomials. After one remembers the Taylor approximation for a function, the problem reduces to one back from precalculus.

Finally, we will end with a question.

lim⁡x→2tanxx3\lim_{x \to 2} \frac{\text{tan} x}{x^3} =

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Submitted by Sujay Kazi

(2015 ASMT, Calculus #4) Given that α\alpha and β\beta are positive real numbers, compute the following limit (where it exists and is nonzero) in terms of α\alpha and β\beta: lim⁡x→0+sin⁡xαcos⁡xβ−1.\lim_{x\rightarrow 0^{+}} \frac{\sin x^{\alpha}}{\cos x^{\beta} -1}.

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Hint

Use the Taylor expansions for sin⁡x\sin x and cos⁡x\cos x centered at x=0x=0: sin⁡x=x−x36+x55!−x77!+...\sin x = x - \frac{x^3}{6} + \frac{x^5}{5!} - \frac{x^7}{7!} + ... cos⁡x=1−x22+x44!−x66!+...\cos x = 1 - \frac{x^2}{2} + \frac{x^4}{4!} - \frac{x^6}{6!} + ...

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Answer

−2-2

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Solution

Using the Taylor expansions for sin⁡x\sin x and cos⁡x\cos x centered at x=0x=0, we see that: sin⁡xα=xα−x3α6+x5α5!−x7α7!+...\sin x^{\alpha} = x^{\alpha} - \frac{x^{3\alpha}}{6} + \frac{x^{5\alpha}}{5!} - \frac{x^{7\alpha}}{7!} + ... cos⁡xβ−1=−x2β2+x4β4!−x6β6!+x8β8!−...\cos x^{\beta} - 1 = -\frac{x^{2\beta}}{2} + \frac{x^{4\beta}}{4!} - \frac{x^{6\beta}}{6!} + \frac{x^{8\beta}}{8!} - ... As xx approaches 00 from the positive side, all of the terms in each series except the first become insignificant. Thus, it suffices to compare: sin⁡xα≈xα\sin x^{\alpha} \approx x^{\alpha} cos⁡xβ−1≈−x2β2\cos x^{\beta} - 1 \approx -\frac{x^{2\beta}}{2} For the desired limit to exist and be nonzero, the exponents of xx must match, so α=2β\alpha = 2\beta. A comparison of the two approximations shows that the limit must equal −2-2, which is the answer.

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

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