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.
Let \( f : (0, \infty) \to \mathbb{R} \) be a twice differentiable function. If for some \( a \neq 0 \), } \[ \int_0^a f(x) \, dx = f(a), \quad f(1) = 1, \quad f(16) = \frac{1}{8}, \quad \text{then } 16 - f^{-1}\left( \frac{1}{16} \right) \text{ is equal to:}\]
In the given figure, the blocks $A$, $B$ and $C$ weigh $4\,\text{kg}$, $6\,\text{kg}$ and $8\,\text{kg}$ respectively. The coefficient of sliding friction between any two surfaces is $0.5$. The force $\vec{F}$ required to slide the block $C$ with constant speed is ___ N.
(Given: $g = 10\,\text{m s}^{-2}$) 
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).
