The entropy \( S \) of a black hole is given by the equation: \[ S = \beta k_B A, \] where \( k_B \) is the Boltzmann constant and \( A \) is the area of the black hole. The units of \( k_B \) are: \[ [k_B] = \text{J/K} = \frac{\text{ML}^2}{\text{T}^2 \text{K}}. \] The area \( A \) has the dimensions of \( \text{L}^2 \) (since area is measured in square units of length). Thus, the dimensions of \( S \) (entropy) are: \[ [S] = \frac{\text{ML}^2}{\text{T}^2 \text{K}} \times \text{L}^2 = \frac{\text{M L}^4}{\text{T}^2 \text{K}}. \] Since entropy \( S \) is dimensionless (as it represents disorder or randomness), the dimensions of \( \beta \) must cancel out the units of \( k_B \) and \( A \). Therefore, \( \beta \) must have the dimensions of \( \text{L}^2 \). Hence, the dimension of \( \beta \) is: \[ \boxed{\text{L}^2}. \]
Match List-I with List-II.
Choose the correct answer from the options given below :
A temperature difference can generate e.m.f. in some materials. Let $ S $ be the e.m.f. produced per unit temperature difference between the ends of a wire, $ \sigma $ the electrical conductivity and $ \kappa $ the thermal conductivity of the material of the wire. Taking $ M, L, T, I $ and $ K $ as dimensions of mass, length, time, current and temperature, respectively, the dimensional formula of the quantity $ Z = \frac{S^2 \sigma}{\kappa} $ is:
A quantity \( X \) is given by: \[ X = \frac{\epsilon_0 L \Delta V}{\Delta t} \] where:
- \( \epsilon_0 \) is the permittivity of free space,
- \( L \) is the length,
- \( \Delta V \) is the potential difference,
- \( \Delta t \) is the time interval.
The dimension of \( X \) is the same as that of: