
Given the differential equation:
\(\frac{dy}{dx} \tan y = \sin(x + y) + \sin(x - y)\)
First, simplify the right side using the sum-to-product identities:
\(\sin(x + y) + \sin(x - y) = 2 \sin x \cos y\)
Thus, the equation becomes:
\(\frac{dy}{dx} \tan y = 2 \sin x \cos y\)
Rewrite \(\tan y\) as \(\frac{\sin y}{\cos y}\):
\(\frac{dy}{dx} \frac{\sin y}{\cos y} = 2 \sin x \cos y\)
Multiply both sides by \(\cos y\):
\(\frac{dy}{dx} \sin y = 2 \sin x \cos^2 y\)
Separate the variables:
\(\frac{\sin y}{\cos^2 y} dy = 2 \sin x dx\)
This can be rewritten as:
\(\sin y \sec^2 y dy = 2 \sin x dx\)
Integrate both sides:
\(\int \sin y \sec^2 y \, dy = \int 2 \sin x \, dx\)
Substitute \(\sin y \sec^2 y\) as \(\tan y \sec y\) and integrate:
\(\int \tan y \sec y \, dy = \sec y + C_1\)
On the right side:
\(\int 2 \sin x \, dx = -2 \cos x + C_2\)
Equate both expressions:
\(\sec y + C_1 = -2 \cos x + C_2\)
Simplify to find the general solution:
\(\sec y = -2 \cos x + C\)
where \(C=C_2-C_1\).
Hence, the correct answer is:
\(\sec y = -2 \cos x + C\)

Let \( f : \mathbb{R} \to \mathbb{R} \) be a twice differentiable function such that \( f(x + y) = f(x) f(y) \) for all \( x, y \in \mathbb{R} \). If \( f'(0) = 4a \) and \( f \) satisfies \( f''(x) - 3a f'(x) - f(x) = 0 \), where \( a > 0 \), then the area of the region R = {(x, y) | 0 \(\leq\) y \(\leq\) f(ax), 0 \(\leq\) x \(\leq\) 2 is :
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure. 
The angular velocity of the system after the particle sticks to it will be: