Match List-I with List-II
| List-I | \(F(x)\) | List-II | Particular Integral Rule |
|---|---|---|---|
| A | \(F(x)=e^{ax}\) | III | \(\dfrac{e^{ax}}{f(a)}, \quad f(a)\neq 0\) |
| B | \(F(x)=\sin ax\) | II | \(\dfrac{\sin ax}{f(-a^2)}\) |
| C | \(F(x)=xe^{ax}\) | I | \(\left(\dfrac{x}{f(a)}-\dfrac{f'(a)}{[f(a)]^2}\right)e^{ax}, \quad f(a)\neq 0\) |
| D | \(F(x)=\cos ax\) | IV | \(D^2\) is replaced by \(-a^2\) in \(f(D)\) |
Concept:
For linear differential equations with constant coefficients: \[ f(D)y = F(x) \] the Particular Integral (P.I.) is obtained using standard operator rules.
Step 1: For \(F(x)=e^{ax}\)
\[ P.I.=\frac{e^{ax}}{f(a)}, \quad f(a)\neq0 \] Therefore: \[ A \rightarrow III \]
Step 2: For \(F(x)=\sin ax\)
\[ P.I.=\frac{\sin ax}{f(-a^2)} \] Therefore: \[ B \rightarrow II \]
Step 3: For \(F(x)=xe^{ax}\)
\[ P.I.=\left(\frac{x}{f(a)}-\frac{f'(a)}{[f(a)]^2}\right)e^{ax} \] Therefore: \[ C \rightarrow I \]
Step 4: For \(F(x)=\cos ax\)
For sine or cosine functions, replace \(D^2\) by: \[ -a^2 \] in \(f(D)\). Therefore: \[ D \rightarrow IV \]
Hence, \[ A-III,\quad B-II,\quad C-I,\quad D-IV \]
\[ \therefore \text{Correct Answer is (C)} \]
| List I | List II |
|---|---|
| (A) The linear momentum of the system remains constant | (IV) The net external force acting on a system of particles is zero |
| (B) The angular momentum of the system remains constant | (III) The external torque acting on a system of particles is zero |
| (C) Inertial frame | (I) The frames relative to which an unaccelerated body appears unaccelerated |
| (D) Non-inertial frame | (II) The frames relative to which an unaccelerated body appears accelerated |
| LIST I | LIST II |
|---|---|
| A. Maxwell's First Equation | I. Modified Ampere's Law |
| B. Maxwell's Second Equation | II. Faraday's Laws of Electromagnetic Induction |
| C. Maxwell's Third Equation | III. Gauss Law in Electrostatics |
| D. Maxwell's Fourth Equation | IV. Gauss Law in Magnetostatics |
| List I | List II |
|---|---|
| (A) (∂S/∂P)T | (I) (∂P/∂T)V |
| (B) (∂T/∂V)S | (II) (∂V/∂S)P |
| (C) (∂T/∂P)S | (III) -(∂V/∂T)P |
| (D) (∂S/∂V)T | (IV) -(∂P/∂S)V |