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Question: Two rods A and B (ohmic conductions at same temperatures) of same length are joined in series and a ...

Two rods A and B (ohmic conductions at same temperatures) of same length are joined in series and a current / passes through it. The ratio of free electrons density (nn), resistivity (ρ\rho) and cross-section area (AA) of both rods are 2, 2 and 0.5 respectively. List-I gives physical quantity of situation and List-II gives corresponding result. Match the list.

A

Ratio of drift velocity of free electron in rod A to that of rod B is

B

The ratio of electric field inside rod A to that of rod B is

C

Ratio of potential difference between points 1 and 2 to that of point 2 and 3 is

D

Ratio of average time taken by free electron to move from point 1 to 2 to that of point 2 to 3 is

E

0.5

F

1

G

2

H

4

I

3

Answer

P-2, Q-4, R-4, S-2

Explanation

Solution

The problem involves two rods A and B of the same length joined in series, meaning the current II flowing through them is the same. We are given the ratios of free electron density (nn), resistivity (ρ\rho), and cross-section area (AA) for rod A to rod B. We need to find the ratios of drift velocity, electric field, potential difference, and time taken for electrons.

Given data:

  1. Rods are in series, so IA=IB=II_A = I_B = I.
  2. Length LL is the same for both rods: LA=LB=LL_A = L_B = L.
  3. Ratio of free electron density: nAnB=2\frac{n_A}{n_B} = 2.
  4. Ratio of resistivity: ρAρB=2\frac{\rho_A}{\rho_B} = 2.
  5. Ratio of cross-section area: AAAB=0.5\frac{A_A}{A_B} = 0.5.

Let's calculate each quantity:

(P) Ratio of drift velocity of free electron in rod A to that of rod B (vdA/vdBv_{dA}/v_{dB}): The current II is related to drift velocity (vdv_d) by the formula: I=neAvdI = n e A v_d Since II is constant for both rods: IA=IBI_A = I_B nAeAAvdA=nBeABvdBn_A e A_A v_{dA} = n_B e A_B v_{dB} vdAvdB=nBABnAAA=(nBnA)×(ABAA)\frac{v_{dA}}{v_{dB}} = \frac{n_B A_B}{n_A A_A} = \left(\frac{n_B}{n_A}\right) \times \left(\frac{A_B}{A_A}\right) vdAvdB=(1nA/nB)×(1AA/AB)\frac{v_{dA}}{v_{dB}} = \left(\frac{1}{n_A/n_B}\right) \times \left(\frac{1}{A_A/A_B}\right) Substitute the given ratios: vdAvdB=(12)×(10.5)=0.5×2=1\frac{v_{dA}}{v_{dB}} = \left(\frac{1}{2}\right) \times \left(\frac{1}{0.5}\right) = 0.5 \times 2 = 1 So, (P) matches with (2).

(Q) The ratio of electric field inside rod A to that of rod B (EA/EBE_A/E_B): The electric field EE is related to resistivity ρ\rho and current density JJ by: E=ρJE = \rho J Current density J=IAJ = \frac{I}{A}. So, E=ρIAE = \frac{\rho I}{A}. For rod A and rod B: EA=ρAIAAE_A = \frac{\rho_A I}{A_A} EB=ρBIABE_B = \frac{\rho_B I}{A_B} EAEB=(ρAI/AA)(ρBI/AB)=(ρAρB)×(ABAA)\frac{E_A}{E_B} = \frac{(\rho_A I / A_A)}{(\rho_B I / A_B)} = \left(\frac{\rho_A}{\rho_B}\right) \times \left(\frac{A_B}{A_A}\right) EAEB=(ρAρB)×(1AA/AB)\frac{E_A}{E_B} = \left(\frac{\rho_A}{\rho_B}\right) \times \left(\frac{1}{A_A/A_B}\right) Substitute the given ratios: EAEB=(2)×(10.5)=2×2=4\frac{E_A}{E_B} = (2) \times \left(\frac{1}{0.5}\right) = 2 \times 2 = 4 So, (Q) matches with (4).

(R) Ratio of potential difference between points 1 and 2 to that of point 2 and 3 (VA/VBV_A/V_B): Points 1 and 2 define rod A, and points 2 and 3 define rod B. The potential difference VV across a length LL with electric field EE is: V=ELV = E L Since LA=LB=LL_A = L_B = L: VAVB=EALAEBLB=EAEB\frac{V_A}{V_B} = \frac{E_A L_A}{E_B L_B} = \frac{E_A}{E_B} From (Q), we found EAEB=4\frac{E_A}{E_B} = 4. So, VAVB=4\frac{V_A}{V_B} = 4 So, (R) matches with (4).

(S) Ratio of average time taken by free electron to move from point 1 to 2 to that of point 2 to 3 (tA/tBt_A/t_B): The time tt taken to travel a length LL with drift velocity vdv_d is: t=Lvdt = \frac{L}{v_d} Since LA=LB=LL_A = L_B = L: tAtB=LA/vdALB/vdB=vdBvdA\frac{t_A}{t_B} = \frac{L_A/v_{dA}}{L_B/v_{dB}} = \frac{v_{dB}}{v_{dA}} From (P), we found vdAvdB=1\frac{v_{dA}}{v_{dB}} = 1. So, tAtB=1vdA/vdB=11=1\frac{t_A}{t_B} = \frac{1}{v_{dA}/v_{dB}} = \frac{1}{1} = 1 So, (S) matches with (2).

Matching the lists: (P) - (2) (Q) - (4) (R) - (4) (S) - (2)