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| = Limits = | | = Limits = |
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| | == The limit of <math>\lim_{x \rightarrow 0^+} x^x</math> == |
| | |
| | === Question === |
| | |
| | What is <math>\lim_{x \rightarrow 0^+} x^x</math>? |
| | |
| | === Solution === |
| | |
| | * Note that <math>x = e^{\ln x}</math>, so <math>x^x = (e^{\ln x})^x = e^{x \ln x}</math>. |
| | * We can further rewrite this as <math>x^x = e^{x \ln x} = e^{\frac{\ln x}{\frac{1}{x}}}</math>. |
| | * As long as <math>f</math> is continuous and the limit of <math>g</math> exists at the point in question, the limit will commute with composition: |
| | <math> |
| | \lim_{x \rightarrow t} f(g(x)) = f(\lim_{x \rightarrow t} g(x)). |
| | </math> |
| | In our case, <math>e(\cdot)</math> is continuous, so |
| | <math> |
| | \lim_{x \rightarrow 0^+} x^x = e^{\lim_{x \rightarrow 0^+} \frac{\ln x}{\frac{1}{x}}}. |
| | </math> |
| | * The question, then, is what is <math>\lim_{x \rightarrow 0^+} \frac{\ln x}{\frac{1}{x}}</math>. |
| | * As <math>x \rightarrow 0^+</math>, <math>\ln x \rightarrow -\infty</math>, <math>\frac{1}{x} \rightarrow +\infty</math>. In this situation we can apply l'Hôpital's rule: |
| | <math> |
| | \lim_{x \rightarrow 0^+} \frac{\ln x}{\frac{1}{x}} = \lim_{x \rightarrow 0^+} \frac{\frac{d}{dx} \ln x}{\frac{d}{dx} \frac{1}{x}} = \frac{\frac{1}{x}}{-\frac{1}{x^2}} = \frac{\frac{1}{x} \cdot x^2}{-\frac{1}{x^2} \cdot x^2} = -x. |
| | </math> |
| | * Hence <math>\lim_{x \rightarrow 0^+} x^x = e^0 = 1</math>. |
| | |
| | == The limits of <math>\lim_{x \rightarrow +\infty} x \sin \frac{1}{x}</math> and <math>\lim_{x \rightarrow -\infty} x \sin \frac{1}{x}</math> == |
| | |
| | === Question === |
| | |
| | What are <math>\lim_{x \rightarrow +\infty} x \sin \frac{1}{x}</math> and <math>\lim_{x \rightarrow -\infty} x \sin \frac{1}{x}</math>? |
| | |
| | === Solution === |
| | |
| | * Let us rewrite <math>x \sin \frac{1}{x}</math> as <math>\frac{\sin \frac{1}{x}}{\frac{1}{x}}</math>. |
| | * As <math>x \rightarrow +\infty</math>, <math>\frac{1}{x} \rightarrow 0</math> and <math>x \sin \frac{1}{x} \rightarrow 0</math>. |
| | * We have "<math>\frac{0}{0}</math>", so we can apply l'Hôpital's rule. |
| | * Differentiating the numerator in <math>\frac{\sin \frac{1}{x}}{\frac{1}{x}}</math>, we obtain <math>\left(\cos \frac{1}{x}\right) \left(-\frac{1}{x^2}\right)</math>. |
| | * Differentiating the denominator in <math>\frac{\sin \frac{1}{x}}{\frac{1}{x}}</math>, we obtain <math>-\frac{1}{x^2}</math>. |
| | * Thus |
| | <math> |
| | \lim_{x \rightarrow +\infty} x \sin \frac{1}{x} = \lim_{x \rightarrow +\infty} \frac{\sin \frac{1}{x}}{\frac{1}{x}} = \lim_{x \rightarrow +\infty} \frac{\left(\cos \frac{1}{x}\right) \left(-\frac{1}{x^2}\right)}{-\frac{1}{x^2}} = \lim_{x \rightarrow +\infty} \cos \frac{1}{x} = 1. |
| | </math> |
| | * Similarly we can find that <math>\lim_{x \rightarrow -\infty} x \sin \frac{1}{x} = 1</math>. |
Latest revision as of 09:53, 22 December 2020
Derivatives
The derivative of
Question
What is ?
Solution 1
- Let .
- Take of both sides: .
- Differentiate both sides: .
- Apply the chain rule on the left-hand side: .
- Apply the product rule on the right-hand side: .
- Putting it together, we have .
- Hence .
Solution 2
- Note that , so .
- Applying the chain rule, .
- Applying the product rule, .
- Therefore .
Integrals
The integral
Question
What is ?
Solution
- We can write as .
- Consider the series expansion of :
.
- We can interchange the integration and summation (we can recognize this as a special case of the Fubini/Tonelli theorems) and write
Limits
The limit of
Question
What is ?
Solution
- Note that , so .
- We can further rewrite this as .
- As long as is continuous and the limit of exists at the point in question, the limit will commute with composition:
In our case, is continuous, so
- The question, then, is what is .
- As , , . In this situation we can apply l'Hôpital's rule:
- Hence .
The limits of and
Question
What are and ?
Solution
- Let us rewrite as .
- As , and .
- We have "", so we can apply l'Hôpital's rule.
- Differentiating the numerator in , we obtain .
- Differentiating the denominator in , we obtain .
- Thus
- Similarly we can find that .