Divide the numerator and denominator by \(\cos x\):
\[ \int_0^{\pi/4} \frac{\tan^2 x \sec^2 x \, dx}{(1 + \tan^3 x)^2}. \]
Let \(1 + \tan^3 x = t\). Then:
\[ \tan^2 x \sec^2 x \, dx = \frac{dt}{3}. \]
The limits transform as:
Substitute into the integral:
\[ \int_0^{\pi/4} \frac{\tan^2 x \sec^2 x \, dx}{(1 + \tan^3 x)^2} = \frac{1}{3} \int_1^2 \frac{dt}{t^2}. \]
Solve the integral:
\[ \frac{1}{3} \int_1^2 t^{-2} \, dt = \frac{1}{3} \left[ -\frac{1}{t} \right]_1^2. \]
Simplify:
\[ \frac{1}{3} \left[ -\frac{1}{2} - (-1) \right] = \frac{1}{3} \left[ -\frac{1}{2} + 1 \right] = \frac{1}{3} \times \frac{1}{2} = \frac{1}{6}. \]
The problem is to evaluate the definite integral \( I = \int_{0}^{\pi/4} \frac{\cos^2 x \sin^2 x}{\left( \cos^3 x + \sin^3 x \right)^2} \, dx \).
This integral can be solved using the method of substitution. The key steps are:
1. Algebraically manipulate the integrand. A common technique for trigonometric functions is to divide the numerator and denominator by a high power of \( \cos x \) to convert the expression into terms of \( \tan x \) and \( \sec^2 x \).
2. Perform a u-substitution, typically by setting \( u \) equal to an expression involving \( \tan x \).
3. Change the limits of integration to correspond to the new variable \( u \).
4. Evaluate the transformed integral, usually with the power rule for integration: \( \int u^n \, du = \frac{u^{n+1}}{n+1} \).
Step 1: To simplify the integrand, divide both the numerator and the denominator by \( \cos^6 x \). This is chosen because the denominator contains a term \( (\cos^3 x)^2 = \cos^6 x \).
\[ I = \int_{0}^{\pi/4} \frac{\frac{\cos^2 x \sin^2 x}{\cos^6 x}}{\frac{\left( \cos^3 x + \sin^3 x \right)^2}{\cos^6 x}} \, dx \]Step 2: Simplify the numerator and denominator separately.
Numerator:
\[ \frac{\cos^2 x \sin^2 x}{\cos^6 x} = \frac{\sin^2 x}{\cos^4 x} = \frac{\sin^2 x}{\cos^2 x} \cdot \frac{1}{\cos^2 x} = \tan^2 x \sec^2 x \]Denominator:
\[ \frac{\left( \cos^3 x + \sin^3 x \right)^2}{\cos^6 x} = \left( \frac{\cos^3 x + \sin^3 x}{\cos^3 x} \right)^2 = \left( 1 + \frac{\sin^3 x}{\cos^3 x} \right)^2 = (1 + \tan^3 x)^2 \]Step 3: Rewrite the integral with the simplified terms.
\[ I = \int_{0}^{\pi/4} \frac{\tan^2 x \sec^2 x}{(1 + \tan^3 x)^2} \, dx \]Step 4: Perform a u-substitution. Let \( u = 1 + \tan^3 x \).
Step 5: Differentiate \( u \) with respect to \( x \) to find \( du \).
\[ \frac{du}{dx} = \frac{d}{dx}(1 + \tan^3 x) = 3 \tan^2 x \cdot \frac{d}{dx}(\tan x) = 3 \tan^2 x \sec^2 x \]This gives us \( du = 3 \tan^2 x \sec^2 x \, dx \), which means \( \tan^2 x \sec^2 x \, dx = \frac{du}{3} \).
Step 6: Change the limits of integration based on the substitution for \( u \).
When \( x = 0 \) (lower limit):
\[ u = 1 + \tan^3(0) = 1 + 0 = 1 \]When \( x = \pi/4 \) (upper limit):
\[ u = 1 + \tan^3(\pi/4) = 1 + (1)^3 = 2 \]Step 7: Substitute \( u \), \( du \), and the new limits into the integral.
\[ I = \int_{1}^{2} \frac{1}{u^2} \left( \frac{du}{3} \right) = \frac{1}{3} \int_{1}^{2} u^{-2} \, du \]Step 8: Integrate with respect to \( u \) using the power rule.
\[ I = \frac{1}{3} \left[ \frac{u^{-1}}{-1} \right]_{1}^{2} = -\frac{1}{3} \left[ \frac{1}{u} \right]_{1}^{2} \]Step 9: Apply the new limits of integration to find the final value.
\[ I = -\frac{1}{3} \left( \frac{1}{2} - \frac{1}{1} \right) = -\frac{1}{3} \left( \frac{1 - 2}{2} \right) = -\frac{1}{3} \left( -\frac{1}{2} \right) \] \[ I = \frac{1}{6} \]Thus, the value of the integral is 1/6.
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,