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| List-$I$ (Relation) | List-$II$ (Law) |
| $A$. $\oint \overrightarrow{E} \cdot d\vec{l} = -\frac{d}{dt} \oint \overrightarrow{B} \cdot d\vec{a}$ | $I$. Ampere's circuital law |
| $B$. $\oint \vec{B} \cdot d\vec{l} = \mu_0(I + \epsilon_0 \frac{d\phi_E}{dt})$ | $II$. Faraday's laws of electromagnetic induction |
| $C$. $\oint \overrightarrow{E} \cdot d\vec{a} = \frac{1}{\epsilon_0} \int \rho dv$ | $III$. Ampere-Maxwell law |
| $D$. $\oint \overrightarrow{B} \cdot d\vec{l} = \mu_0 I$ | $IV$. Gauss's law of electrostatics |
| List-$I$ | List-$II$ |
| $(a)$ Gauss’ law for electrostatics | $(i)$ $\oint \vec{E} \cdot d\vec{A} = \frac{Q}{\epsilon_0}$ |
| $(b)$ Gauss’ law for magnetism | (ii) $\oint \vec{B} \cdot d\vec{l} = \mu_0 [i_c + \epsilon_0 \frac{d\phi_E}{dt}]$ |
| $(c)$ Faraday’s law | (iii) $\oint \vec{B} \cdot d\vec{A} = 0$ |
| $(d)$ Ampere-Maxwell’s law | (iv) $\oint \vec{E} \cdot d\vec{l} = -\frac{d\phi_B}{dt}$ |
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