Step 1: We apply integration by parts. Let:
- \( u = x \), so \( du = dx \)
- \( dv = e^{-x} dx \), so \( v = -e^{-x} \)
Step 2: Using the integration by parts formula: \[ \int u \, dv = uv - \int v \, du \] Substitute the values: \[ \int x e^{-x} \, dx = -x e^{-x} - \int -e^{-x} \, dx \]
Step 3: Simplifying the remaining integral: \[ = -x e^{-x} + e^{-x} \]
Step 4: Factor the result: \[ = -(x + 1) e^{-x} \] Thus, the correct answer is (A) \( -(x + 1) e^{-x} \).
Solve:
\[ \int \frac{\sin x}{\sin (x+a)} \, dx. \]If
\[ A = \begin{bmatrix} 1 & -1 & 0 \\ 2 & 3 & -2 \\ -2 & 0 & 1 \end{bmatrix}, \quad B = \begin{bmatrix} 3 & -15 & 5 \\ -1 & 6 & -2 \\ 1 & -5 & 2 \end{bmatrix}, \]
then find the value of \( (AB)^{-1} \).
Find the value of \[ \int \frac{\sec^2 2x}{(\cot x - \tan x)^2} \, dx. \]
State Gauss's Law in electrostatics. Using it (i) find electric field due to a point source charge \( q \) and (ii) deduce Coulomb's law between source charge \( q \) and test charge \( q_0 \).
Compare features of p-type and n-type semiconductors. Draw circuit diagram of half-wave rectifier of p-n junction diode and explain it.
What is atomic model of magnetism? Differentiate between paramagnetic, diamagnetic, and ferromagnetic substances on this basis. Also, give one example of each.