The given dimensionless quantity is written as:
\[ e^{\alpha} \varepsilon_0^{\beta} h^{\gamma} c^{\delta} \]
The dimensional formula for each term is:
Substituting their powers into the dimensionless quantity:
\[ [T A]^{\alpha} \cdot [M^{-1}L^{-3}T^4A^2]^{\beta} \cdot [ML^2T^{-1}]^{\gamma} \cdot [LT^{-1}]^{\delta} = [L^0 M^0 T^0 A^0] \]
Expanding dimensions:
\[ M^{- \beta + \gamma} L^{-3 \beta + 2\gamma + \delta} T^{\alpha + 4\beta - \gamma - \delta} A^{\alpha + 2\beta} = M^0 L^0 T^0 A^0 \]
Equating powers of \( M, L, T, A \):
From (4):
\( \alpha = -2\beta \) (5)
From (1):
\( \beta = \gamma \) (6)
Substituting \( \beta = \gamma \) into (2):
\( -3\beta + 2\beta + \delta = 0 \Rightarrow -\beta + \delta = 0 \Rightarrow \delta = \beta \) (7)
Substituting \( \beta = \gamma = \delta \) and \( \alpha = -2\beta \) into (3):
\( -2\beta + 4\beta - \beta - \beta = 0 \)
This equation is satisfied, so the solution is consistent. Let \( \beta = -n \), where \( n \) is a non-zero integer.
Then:
\( (2n, -n, -n, -n) \)
Sliding contact of a potentiometer is in the middle of the potentiometer wire having resistance \( R_p = 1 \, \Omega \) as shown in the figure. An external resistance of \( R_e = 2 \, \Omega \) is connected via the sliding contact.
The current \( i \) is :