Step 1: Evaluate \( f^2(x) \):
\[ f^2(x) = \lim_{r \to x} \frac{(2x^2f(r))^2 - f(x)f(r)x}{x^2 - r^2} \cdot \frac{r - x}{r} \]
Simplifying this expression using L'Hôpital's Rule and differentiating the terms with respect to \( r \), we eventually get:
\[ f^2(x) = 2x f(x)f'(x) - xe^{x} \]
Step 2: Rewrite the equation:
We now have the differential equation:
\[ f(x)^2 = x f(x)f'(x) - xe^{x} \]
Step 3: Substitute \( y = f(x) \):
This substitution gives \( y = f(x) \), so that \( \frac{dy}{dx} = f'(x) \), and the equation becomes:
\[ y^2 = xy \frac{dy}{dx} - xe^x \]
Step 4: Separate variables and simplify:
Let \( y = vx \), so that \( \frac{dy}{dx} = v + x \frac{dv}{dx} \). Substitute into the equation:
\[ v^2x^2 = x e^{x}(v + x \frac{dv}{dx}) - xe^x \]
Step 5: Solve the resulting differential equation:
By separating variables and integrating both sides, we obtain:
\[ \int v^2 \, dv = \int \frac{dx}{x} \]
Step 6: Integrate:
Integrating both sides, we get:
\[ e^v = \ln|x| + c \]
Step 7: Apply initial condition:
Given \( f(1) = 1 \), substitute \( x = 1 \) and \( y = 1 \) to find \( c \):
\[ e^1 = \ln 1 + c = c = 2 \]
Step 8: Find \( a \) such that \( f(a) = 0 \):
When \( y = 0 \), we solve for \( v = 0 \):
\[ a = -\frac{2}{e} \]
Step 9: Calculate \( ea \):
\[ ea = e \cdot -\frac{2}{e} = -2 \]
Thus, \( ea = 2 \).
The Correct Answer is : 2
We are given a function \( f(x) \) with the conditions \( f(1) = 1 \) and \( f(a) = 0 \). We are tasked with finding the value of \( a \), starting from the following equation: \[ f^2(x) = \lim_{r \to x} \left( \frac{2r^2(f^2(r)) - f(r)f(r)}{r^2 - x^2} - r^3 e^{f(r)} \right) \] This leads us through various steps of limits, derivatives, and integrations.
Start with the expression: \[ f^2(x) = 2x^2 f(x) \cdot \frac{2}{x} \cdot f'(x) - x^3 e^{f(x)} \] We start simplifying the derivative expression: \[ y^2 = x y \frac{dy}{dx} - x^3 \cdot e^{y/x} \] where we perform differentiation by using the chain rule.
By substitution, we get: \[ y = \frac{dy}{dx} \quad \text{and we solve for} \quad \frac{dy}{dx} = \frac{x^2}{y e^{y/x}} \] This relationship allows us to rewrite: \[ \frac{dx}{dy} = e^{-v} v \, dv = dx \]
Next, we integrate both sides of the equation: \[ e^v(x + c) + 1 + v = 0 \] Using the initial condition \( f(1) = 1 \), we set \( x = 1 \) and \( y = 1 \), which gives: \[ c = -1 - \frac{2}{e} \]
Substituting into the expression, we calculate: \[ x = a, \, y = 0 \quad \Rightarrow \quad a = \frac{2}{e} \]
The value of \( a \) is: \[ \boxed{2} \]
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: