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: \[ \boxed{2} \]
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,