Given integral:
\[ \int_{0}^{\frac{\pi}{4}} \frac{\sin^2 x}{1 + \sin x \cos x} dx = \int_{0}^{\frac{\pi}{4}} \frac{\sin^2 x}{1 + \frac{1}{2} \sin 2x} dx = \int_{0}^{\frac{\pi}{4}} \frac{1 - \cos 2x}{2 + \sin 2x} dx \]
We separate this into two integrals:
\[ \int_{0}^{\frac{\pi}{4}} \frac{1}{2 + \sin 2x} dx - \int_{0}^{\frac{\pi}{4}} \frac{\cos 2x}{2 + \sin 2x} dx \]
Denote these integrals as \(I_1\) and \(I_2\) respectively:
\[ I_1 = \int_{0}^{\frac{\pi}{4}} \frac{dx}{2 + \sin 2x}, \quad I_2 = \int_{0}^{\frac{\pi}{4}} \frac{\cos 2x}{2 + \sin 2x} dx \]
For \(I_1\), let \(\tan x = t\), hence:
\[ dx = \frac{dt}{1 + t^2}, \quad \sin 2x = \frac{2t}{1 + t^2} \]
Substituting these into the integral:
\[ I_1 = \frac{1}{2} \int_{0}^{1} \frac{dt}{\left(t + \frac{1}{2}\right)^2 + \left(\frac{\sqrt{3}}{2}\right)^2} = \frac{\pi}{6\sqrt{3}} \]
For \(I_2\), we use:
\[ I_2 = \int_{0}^{\frac{\pi}{4}} \frac{\cos 2x}{2 + \sin 2x} dx \]
Applying another substitution and evaluating, we find:
\[ I_2 = \frac{1}{2} \ln \left(\frac{3}{2}\right) \]
Thus, the original integral becomes:
\[ I = I_1 - I_2 = \frac{\pi}{6\sqrt{3}} - \frac{1}{2} \ln \left(\frac{3}{2}\right) \]
Given that:
\[ \int_{0}^{\frac{\pi}{4}} \frac{\sin^2 x}{1 + \sin x \cos x} dx = \frac{1}{a} \ln_e \left(\frac{a}{3}\right) + \frac{\pi}{b\sqrt{3}} \]
Comparing terms, we find: \[ a = 2, \quad b = 6 \]
Therefore:
\[ a + b = 2 + 6 = 8 \]
A stationary tank is cylindrical in shape with two hemispherical ends and is horizontal, as shown in the figure. \(R\) is the radius of the cylinder as well as of the hemispherical ends. The tank is half filled with an oil of density \(\rho\) and the rest of the space in the tank is occupied by air. The air pressure, inside the tank as well as outside it, is atmospheric. The acceleration due to gravity (\(g\)) acts vertically downward. The net horizontal force applied by the oil on the right hemispherical end (shown by the bold outline in the figure) is:
Draw a rough sketch for the curve $y = 2 + |x + 1|$. Using integration, find the area of the region bounded by the curve $y = 2 + |x + 1|$, $x = -4$, $x = 3$, and $y = 0$.
Let \[ I(x) = \int \frac{dx}{(x-11)^{\frac{11}{13}} (x+15)^{\frac{15}{13}}} \] If \[ I(37) - I(24) = \frac{1}{4} \left( b^{\frac{1}{13}} - c^{\frac{1}{13}} \right) \] where \( b, c \in \mathbb{N} \), then \[ 3(b + c) \] is equal to:
A force \( \vec{f} = x^2 \hat{i} + y \hat{j} + y^2 \hat{k} \) acts on a particle in a plane \( x + y = 10 \). The work done by this force during a displacement from \( (0,0) \) to \( (4m, 2m) \) is Joules (round off to the nearest integer).