\( L^2 T^{-2} \)
We are asked to find the dimension of \( \left(\dfrac{1}{\mu_0 \epsilon_0}\right) \), where \( \mu_0 \) and \( \epsilon_0 \) are the permeability and permittivity of free space, respectively.
We use the relation between the speed of light \( c \), the permeability \( \mu_0 \), and the permittivity \( \epsilon_0 \):
\[ c = \frac{1}{\sqrt{\mu_0 \epsilon_0}} \]Hence,
\[ \frac{1}{\mu_0 \epsilon_0} = c^2 \]The dimension of speed \( c \) is \( [L\,T^{-1}] \), so the dimension of \( c^2 \) is \( [L^2\,T^{-2}] \).
Step 1: Write the dimensional formula of \( \mu_0 \) and \( \epsilon_0 \):
\[ [\mu_0] = [M^1 L^1 T^{-2} A^{-2}] \] \[ [\epsilon_0] = [M^{-1} L^{-3} T^{4} A^{2}] \]Step 2: Multiply \( \mu_0 \epsilon_0 \):
\[ [\mu_0 \epsilon_0] = [M^{1-1} L^{1-3} T^{-2+4} A^{-2+2}] = [L^{-2} T^{2}] \]Step 3: Take the reciprocal:
\[ \left[\frac{1}{\mu_0 \epsilon_0}\right] = [L^2 T^{-2}] \]The dimension of \( \left(\dfrac{1}{\mu_0 \epsilon_0}\right) \) is:
\[ \boxed{[L^2 T^{-2}]} \]It represents the square of velocity (i.e., \( c^2 \)).
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

| List I | List II |
|---|---|
| A. \( \oint \vec{B} \cdot d\vec{l} = \mu_0 i_c + \mu_0 \epsilon_0 \frac{d\phi_E}{dt} \) | I. Gauss' law for electricity |
| B. \( \oint \vec{E} \cdot d\vec{l} = -\frac{d\phi_B}{dt} \) | II. Gauss' law for magnetism |
| C. \( \oint \vec{E} \cdot d\vec{A} = \frac{Q}{\epsilon_0} \) | III. Faraday law |
| D. \( \oint \vec{B} \cdot d\vec{A} = 0 \) | IV. Ampere – Maxwell law |

What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)