Given:
We are tasked with evaluating the following limit:
\[ \lim_{x \to 1} \ln\left( \frac{f(x+2)}{f(3)} \right)^{\frac{18}{(x-1)^2}} \]
1. Simplifying the Expression:
The given expression involves a logarithm and an exponent. We can simplify it using logarithmic properties:
\[ \ln\left( \frac{f(x+2)}{f(3)} \right)^{\frac{18}{(x-1)^2}} = \frac{18}{(x-1)^2} \ln\left( \frac{f(x+2)}{f(3)} \right) \] Thus, the limit becomes: \[ \lim_{x \to 1} \frac{18}{(x-1)^2} \ln\left( \frac{f(x+2)}{f(3)} \right) \]
2. Expanding \( f(x+2) \) Around \( x = 1 \):
We will expand \( f(x+2) \) around \( x = 1 \) using a Taylor expansion. Since \( f(3) = 18 \), \( f'(3) = 0 \), and \( f''(3) = 4 \), we use the Taylor series for \( f(x+2) \) around \( x = 1 \):
\[ f(x+2) \approx f(3) + f'(3)(x-1) + \frac{f''(3)}{2}(x-1)^2 + \cdots \] Substituting the given values, we have: \[ f(x+2) \approx 18 + \frac{4}{2}(x-1)^2 = 18 + 2(x-1)^2 \] Thus: \[ \frac{f(x+2)}{f(3)} = \frac{18 + 2(x-1)^2}{18} = 1 + \frac{2(x-1)^2}{18} \] Now, take the natural logarithm of this expression: \[ \ln\left( 1 + \frac{2(x-1)^2}{18} \right) \] For small \( (x-1) \), we can use the approximation \( \ln(1 + y) \approx y \) when \( y \) is small. So: \[ \ln\left( 1 + \frac{2(x-1)^2}{18} \right) \approx \frac{2(x-1)^2}{18} \]
3. Substituting Back into the Limit:
Substitute this approximation back into the limit expression: \[ \lim_{x \to 1} \frac{18}{(x-1)^2} \cdot \frac{2(x-1)^2}{18} \] Simplifying: \[ \lim_{x \to 1} 2 = 2 \]
Final Answer: The value of the limit is \( \boxed{2} \).
A substance 'X' (1.5 g) dissolved in 150 g of a solvent 'Y' (molar mass = 300 g mol$^{-1}$) led to an elevation of the boiling point by 0.5 K. The relative lowering in the vapour pressure of the solvent 'Y' is $____________ \(\times 10^{-2}\). (nearest integer)
[Given : $K_{b}$ of the solvent = 5.0 K kg mol$^{-1}$]
Assume the solution to be dilute and no association or dissociation of X takes place in solution.
Inductance of a coil with \(10^4\) turns is \(10\,\text{mH}\) and it is connected to a DC source of \(10\,\text{V}\) with internal resistance \(10\,\Omega\). The energy density in the inductor when the current reaches \( \left(\frac{1}{e}\right) \) of its maximum value is \[ \alpha \pi \times \frac{1}{e^2}\ \text{J m}^{-3}. \] The value of \( \alpha \) is _________.
\[ (\mu_0 = 4\pi \times 10^{-7}\ \text{TmA}^{-1}) \]