Constant that makes a logarithm power continuous
Let $$ f(x) = \ln\left(\frac{\sin x}{x}\right)^{\frac{1}{x^2}}, \quad x \neq 0, \qquad f(0) = \alpha. $$ Determine the value of $\alpha$ for which $f$ is continuous at $x=0$.
Explanation of Method
For $f$ to be continuous at $x=0$, $\alpha$ must equal $\lim_{x\to0}f(x)$. Using the logarithm power rule, $f(x)$ simplifies to $\dfrac{1}{x^2}\ln\left(\dfrac{\sin x}{x}\right)$, so the task reduces to evaluating this single limit. The Taylor expansion of $\sin x$ near $0$ gives $\dfrac{\sin x}{x}$ as $1$ plus a small correction of order $x^2$, and the small-argument approximation $\ln(1+u)\approx u$ then converts the logarithm into that same correction, which is exactly cancelled by dividing by $x^2$.
- Simplify $f(x)$ using the logarithm power rule.
- Expand $\dfrac{\sin x}{x}$ with the Taylor series for $\sin x$.
- Approximate the logarithm using $\ln(1+u)\approx u$ for small $u$.
- Divide by $x^2$ and take the limit to find $\alpha$.
Step 1 · Simplify $f(x)$
Using $\ln(a^b) = b\ln a$:
$$ f(x) = \ln\left(\frac{\sin x}{x}\right)^{1/x^2} = \frac{1}{x^2}\ln\left(\frac{\sin x}{x}\right). $$
Step 2 · Expand $\dfrac{\sin x}{x}$ near $x=0$
The Taylor series for $\sin x$ near $0$ is $\sin x = x - \dfrac{x^3}{6} + O(x^5)$, so:
$$ \frac{\sin x}{x} = 1 - \frac{x^2}{6} + O(x^4). $$
Step 3 · Approximate the logarithm
Since $\dfrac{\sin x}{x} \to 1$ as $x\to0$, use $\ln(1+u)\approx u$ for small $u = -\dfrac{x^2}{6}+O(x^4)$:
$$ \ln\left(\frac{\sin x}{x}\right) = \ln\left(1-\frac{x^2}{6}+O(x^4)\right) \approx -\frac{x^2}{6} + O(x^4). $$
Step 4 · Divide by $x^2$ and take the limit
Substituting into $f(x)$:
$$ f(x) = \frac{1}{x^2}\left(-\frac{x^2}{6}+O(x^4)\right) = -\frac16 + O(x^2). $$
Taking the limit as $x \to 0$:
$$ \lim_{x\to0} f(x) = -\frac16. $$
For $f$ to be continuous at $x=0$, we need $\alpha = f(0) = \lim_{x\to0}f(x)$, so:
$$ \alpha = -\frac16. $$
Summary Table
| Quantity | Expansion | Limit as $x\to0$ |
|---|---|---|
| $\dfrac{\sin x}{x}$ | $1-\dfrac{x^2}{6}+O(x^4)$ | $1$ |
| $\ln\left(\dfrac{\sin x}{x}\right)$ | $-\dfrac{x^2}{6}+O(x^4)$ | $0$ |
| $f(x)=\dfrac{1}{x^2}\ln\left(\dfrac{\sin x}{x}\right)$ | $-\dfrac16+O(x^2)$ | $-\dfrac16$ |
Additional Notes
- This limit is equivalent to saying $\left(\dfrac{\sin x}{x}\right)^{1/x^2} \to e^{-1/6}$ as $x\to0$ — exponentiating $\alpha=-\frac16$ recovers the base of that related $1^\infty$-type limit.
- Only the $x^2$-order term of the Taylor expansion of $\sin x$ mattered here, since higher-order corrections vanish once divided by $x^2$ and the limit is taken — this is a common pattern whenever a logarithm of a ratio is divided by a matching power.
- The constant $\frac16$ is directly inherited from the coefficient $\frac16$ in the Taylor series $\sin x = x - \frac{x^3}{6}+\cdots$; a different oscillatory function in place of $\sin x$ would produce a different constant here.
Result
The value of $\alpha$ that makes $f$ continuous at $x=0$ is: