| LIST I | LIST II | ||
|---|---|---|---|
| A. | ∇ ⋅ E = ρ/ε₀ | I. Gauss's Law in magnetostatics | |
| B. | ∇ ⋅ B = 0 | II. Faraday's Law of electromagnetic Induction | |
| C. | ∇ × E = - ∂B/∂t | III. Gauss's Law in electrostatics | |
| D. | ∇ × B = μ₀J + μ₀ε₀ ∂E/∂t | IV. Modified Ampere's Law |
\( \nabla \cdot \mathbf{E} = \frac{\rho}{\epsilon_0} \) is Gauss's Law in electrostatics (A).
\( \nabla \cdot \mathbf{B} = 0 \) is Gauss's Law in magnetostatics (B).
\( \nabla \times \mathbf{E} = -\frac{\partial \mathbf{B}}{\partial t} \) is Faraday's Law (C).
\( \nabla \times \mathbf{B} = \mu_0 \mathbf{J} + \mu_0 \epsilon_0 \frac{\partial \mathbf{E}}{\partial t} \) is the Modified Ampere's Law (D)
| 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 |
| 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 |