We have:
\(\alpha = \lim_{x \to 0^+} e^{\sqrt{x}} \left( \frac{e^{\sqrt{\tan x} - \sqrt{x}} - 1}{\sqrt{\tan x} - \sqrt{x}} \right)\)
Step 1: Simplify the limit expression
As \(x \to 0\), we know that \(\tan x \approx x\). Therefore, the term inside the parenthesis tends to 1.
Hence,
\(\alpha = 1\)
Step 2: Evaluate the second limit
\(\beta = \lim_{x \to 0} (1 + \sin x)^{\frac{1}{2} \cot x}\)
Taking logarithm and using the standard limit \(\lim_{x \to 0} (1 + \sin x)^{1/\sin x} = e\), we get:
\(\beta = e^{1/2}\)
Step 3: Forming the quadratic equation
\[
x^{2} - (1 + \sqrt{e})x + \sqrt{e} = 0
\]
Let this be compared with the general form:
\[
ax^{2} + bx - \sqrt{e} = 0
\]
Step 4: Comparing coefficients
On comparing, we get:
\(a = -1, \quad b = \sqrt{e} + 1\)
Step 5: Finding the required value
\[
12 \ln(a + b) = 12 \ln\left( -1 + (\sqrt{e} + 1) \right)
\]
Simplifying:
\[
12 \ln(\sqrt{e}) = 12 \times \frac{1}{2} = 6
\]
Given: The given expression for \(\alpha\) is:
\[ \alpha = \lim_{x \to 0^+} \frac{\sqrt{x} \left( e^{\sqrt{\tan x} - \sqrt{x}} - 1 \right)}{\sqrt{\tan x} - \sqrt{x}}. \]
As \( x \to 0^+ \), we observe that \( \sqrt{\tan x} \to \sqrt{x} \). The expression simplifies as the numerator and denominator converge to zero:
\[ \alpha = 1. \]
The given expression for \(\beta\) is:
\[ \beta = \lim_{x \to 0} \left( 1 + \sin x \right)^{\frac{1}{2} \cot x}. \]
Using the approximation \( \sin x \approx x \) and \( \cot x \approx \frac{1}{x} \) as \( x \to 0 \), we rewrite the expression:
\[ \beta = \left( 1 + x \right)^{\frac{1}{2x}}. \]
Using the standard limit \( \lim_{x \to 0} \left( 1 + x \right)^{\frac{1}{x}} = e \), we get:
\[ \beta = e^{\frac{1}{2}}. \]
The quadratic equation is:
\[ x^2 - \left( 1 + \sqrt{e} \right) x + \sqrt{e} = 0. \]
Compare with the general quadratic form:
\[ ax^2 + bx + c = 0. \]
From the given equation:
\[ a = 1, \quad b = -(1 + \sqrt{e}), \quad c = \sqrt{e}. \]
Substitute the values of \( a \) and \( b \):
\[ a + b = 1 - (1 + \sqrt{e}) = -\sqrt{e}. \]
\[ \ln(a + b) = \ln(-\sqrt{e}) = \ln(\sqrt{e}) + \ln(-1) = \frac{1}{2} \ln(e). \]
Finally, calculate:
\[ 12 \ln(a + b) = 12 \times \frac{1}{2} = 6. \]
Answer: 6
For \( \alpha, \beta, \gamma \in \mathbb{R} \), if \[ \lim_{x \to 0} \frac{x^2 \sin(\alpha x) + (\gamma - 1)e^{x^2}}{\sin(2x - \beta x)} = 3, \] then \( \beta + \gamma - \alpha \) is equal to:
If $\lim_{x \to 1} \frac{(x-1)(6+\lambda \cos(x-1)) + \mu \sin(1-x)}{(x-1)^3} = -1$, where $\lambda, \mu \in \mathbb{R}$, then $\lambda + \mu$ is equal to
Consider the following sequence of reactions : 
Molar mass of the product formed (A) is ______ g mol\(^{-1}\).
Given below are two statements: one is labelled as Assertion (A) and the other is labelled as Reason (R).
Assertion (A): Choke coil is simply a coil having a large inductance but a small resistance. Choke coils are used with fluorescent mercury-tube fittings. If household electric power is directly connected to a mercury tube, the tube will be damaged.
Reason (R): By using the choke coil, the voltage across the tube is reduced by a factor \( \frac{R}{\sqrt{R^2 + \omega^2 L^2}} \), where \( \omega \) is the frequency of the supply across resistor \( R \) and inductor \( L \). If the choke coil were not used, the voltage across the resistor would be the same as the applied voltage.
In light of the above statements, choose the most appropriate answer from the options given below:
Given below are two statements: one is labelled as Assertion (A) and the other is labelled as Reason (R).
Assertion (A): Electromagnetic waves carry energy but not momentum.
Reason (R): Mass of a photon is zero.
In the light of the above statements, choose the most appropriate answer from the options given below: