We are given the equation: \[ F = 6\pi \eta x \] where \( F \) is force, \( \eta \) is viscosity, and \( x \) is the quantity we need to find the dimensions for. We know the dimensional formula for force \( F \) is: \[ [F] = [M L T^{-2}] \] The dimensional formula for viscosity \( \eta \) is: \[ [\eta] = [M L^{-1} T^{-1}] \] Now, let the dimensional formula of \( x \) be \( [x] = [M^a L^b T^c] \).
Using the given equation: \[ [M L T^{-2}] = [M L^{-1} T^{-1}] [M^a L^b T^c] \] Equating the powers of \( M \), \( L \), and \( T \) on both sides, we get the following system of equations: \[ M: 1 = 1 + a \] \[ L: 1 = -1 + b \] \[ T: -2 = -1 + c \] Solving these equations: - From \( M: 1 = 1 + a \), we get \( a = 0 \)
- From \( L: 1 = -1 + b \), we get \( b = 2 \)
- From \( T: -2 = -1 + c \), we get \( c = -1 \)
Therefore, the dimensional formula for \( x \) is: \[ [x] = [M^1 L^1 T^{-1}] \]
Thus, the correct answer is \( [M^1 L^1 T^{-1]} \).
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: