Given differential equation:
\[ \frac{dy}{dx} - y = 1 + 4 \sin x. \]
This is a first-order linear differential equation. To solve, we use an integrating factor (IF):
\[ \text{IF} = e^{-x}. \]
Multiplying the entire equation by the integrating factor: \[ e^{-x} \frac{dy}{dx} - e^{-x} y = e^{-x} + 4e^{-x} \sin x. \]
The left-hand side becomes the derivative of \(y e^{-x}\): \[ \frac{d}{dx}(y e^{-x}) = e^{-x} + 4e^{-x} \sin x. \]
Integrating both sides:
\[ y e^{-x} = \int \left(e^{-x} + 4e^{-x} \sin x\right) dx. \]
Evaluating the integral:
\[ y e^{-x} = \int e^{-x} dx + 4 \int e^{-x} \sin x \, dx. \]
The first integral is straightforward:
\[ \int e^{-x} dx = -e^{-x}. \]
For the second integral, we use integration by parts or known results:
\[ 4 \int e^{-x} \sin x \, dx = -2e^{-x} (\sin x + \cos x). \]
Thus: \[ y e^{-x} = -e^{-x} - 2e^{-x} (\sin x + \cos x) + C. \]
Multiplying through by \(e^x\): \[ y = -1 - 2(\sin x + \cos x) + C e^x. \]
Using the initial condition \(y(\pi) = 1\):
\[ 1 = -1 - 2(\sin \pi + \cos \pi) + C e^\pi. \]
Since \(\sin \pi = 0\) and \(\cos \pi = -1\):
\[ 1 = -1 - 2(-1) + C e^\pi \implies 1 = 1 + C e^\pi \implies C = 0. \]
Thus, the solution simplifies to: \[ y = -1 - 2(\sin x + \cos x). \]
Evaluating at \(x = \frac{\pi}{2}\):
\[ y\left(\frac{\pi}{2}\right) = -1 - 2\left(\sin \frac{\pi}{2} + \cos \frac{\pi}{2}\right) = -1 - 2(1 + 0) = -3. \]
Calculating \(y\left(\frac{\pi}{2}\right) + 10\):
\[ y\left(\frac{\pi}{2}\right) + 10 = -3 + 10 = 7. \]
Consider the following sequence of reactions : 
Molar mass of the product formed (A) is ______ g mol\(^{-1}\).
In a Young's double slit experiment, three polarizers are kept as shown in the figure. The transmission axes of \( P_1 \) and \( P_2 \) are orthogonal to each other. The polarizer \( P_3 \) covers both the slits with its transmission axis at \( 45^\circ \) to those of \( P_1 \) and \( P_2 \). An unpolarized light of wavelength \( \lambda \) and intensity \( I_0 \) is incident on \( P_1 \) and \( P_2 \). The intensity at a point after \( P_3 \), where the path difference between the light waves from \( S_1 \) and \( S_2 \) is \( \frac{\lambda}{3} \), is:
