Question 1

SCQMEDIUM

A temperature difference can generate e.m.f. in some materials. Let SS be the e.m.f. produced per unit temperature difference between the ends of a wire, σ\sigma the electrical conductivity and Îș\kappa the thermal conductivity of the material of the wire. Taking M,L,T,IM, L, T, I and KK as dimensions of mass, length, time, current and temperature, respectively, the dimensional formula of the quantity Z=S2σÎșZ = \frac{S^2 \sigma}{\kappa} is:

(A)

[M0L0T0I0K0][M^0 L^0 T^0 I^0 K^0]

(B)

[M0L0T0I0K−1][M^0 L^0 T^0 I^0 K^{-1}]

(C)

[M1L2T−2I−1K−1][M^1 L^2 T^{-2} I^{-1} K^{-1}]

(D)

[M1L2T−4I−1K−1][M^1 L^2 T^{-4} I^{-1} K^{-1}]

Detailed Solution

We first find the dimensions of each quantity:

  1. e.m.f. (VV): work/charge=[ML2T−2]/[IT]=[ML2T−3I−1]\text{work} / \text{charge} = [ML^2T^{-2}] / [IT] = [ML^2T^{-3}I^{-1}].
  2. S=e.m.f./temperature=[ML2T−3I−1K−1]S = \text{e.m.f.} / \text{temperature} = [ML^2T^{-3}I^{-1}K^{-1}].
  3. Electrical conductivity σ=1ρ=lRA=l(V/I)A=[L][I][ML2T−3I−1][L2]=[M−1L−3T3I2]\sigma = \frac{1}{\rho} = \frac{l}{RA} = \frac{l}{(V/I)A} = \frac{[L][I]}{[ML^2T^{-3}I^{-1}][L^2]} = [M^{-1}L^{-3}T^3I^2].
  4. Thermal conductivity Îș\kappa is found from dQdt=ÎșAΔTl⇒Îș=[ML2T−2/T][L][L2][K]=[MLT−3K−1]\frac{dQ}{dt} = \kappa A \frac{\Delta T}{l} \Rightarrow \kappa = \frac{[ML^2T^{-2}/T] [L]}{[L^2][K]} = [MLT^{-3}K^{-1}].

Now, calculate dimensions of Z=S2σÎșZ = \frac{S^2 \sigma}{\kappa}: [Z]=([ML2T−3I−1K−1])2⋅[M−1L−3T3I2][MLT−3K−1][Z] = \frac{([ML^2T^{-3}I^{-1}K^{-1}])^2 \cdot [M^{-1}L^{-3}T^3I^2]}{[MLT^{-3}K^{-1}]} [Z]=[M2L4T−6I−2K−2]⋅[M−1L−3T3I2][MLT−3K−1][Z] = \frac{[M^2L^4T^{-6}I^{-2}K^{-2}] \cdot [M^{-1}L^{-3}T^3I^2]}{[MLT^{-3}K^{-1}]} [Z]=[M1L1T−3K−2][MLT−3K−1]=[K−1][Z] = \frac{[M^1L^1T^{-3}K^{-2}]}{[MLT^{-3}K^{-1}]} = [K^{-1}] Thus, the dimensional formula is [M0L0T0I0K−1][M^0 L^0 T^0 I^0 K^{-1}].

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