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Question: The value of resistance $R$ is being measured with the potentiometer set up in two steps shown below...

The value of resistance RR is being measured with the potentiometer set up in two steps shown below. Step-I : Es=10E_s = 10 V, r=1Ωr = 1 \Omega and zero deflection is observed at length PJ=80PJ = 80 cm. Step-II : Es=5E_s = 5 V, r=2Ωr = 2 \Omega and zero deflection is observed at length PJ=30PJ = 30 cm. Then

A

The value of RR is 1Ω1 \Omega

B

The value of RR is 2Ω2 \Omega

C

Current through RR in Step-I is 103A\frac{10}{3} A

D

Current through RR in Step-II is 54A\frac{5}{4} A

Answer

The value of RR is 2Ω2 \Omega, Current through RR in Step-I is 103A\frac{10}{3} A, Current through RR in Step-II is 54A\frac{5}{4} A

Explanation

Solution

The problem involves a potentiometer circuit used to determine an unknown resistance RR. The principle of a potentiometer states that at null deflection, the potential difference across the balancing length of the potentiometer wire is equal to the potential difference across the component in the secondary circuit.

The secondary circuit consists of a cell EsE_s, an internal resistance rr, and the unknown resistance RR. The current flowing through this secondary circuit is given by Ohm's law: Is=EsR+rI_s = \frac{E_s}{R+r}

The potential difference across the unknown resistance RR is: VR=Is×R=EsRR+rV_R = I_s \times R = \frac{E_s R}{R+r}

At null deflection, this potential difference VRV_R is balanced by the potential drop across the balancing length LL of the potentiometer wire. If kk is the potential gradient of the potentiometer wire (potential drop per unit length), then: k×L=VRk \times L = V_R So, k×L=EsRR+rk \times L = \frac{E_s R}{R+r}

We are given two steps:

Step-I: Es=10E_s = 10 V r=1Ωr = 1 \Omega L=80L = 80 cm Substituting these values into the equation: k×80=10×RR+1k \times 80 = \frac{10 \times R}{R+1} (Equation 1)

Step-II: Es=5E_s = 5 V r=2Ωr = 2 \Omega L=30L = 30 cm Substituting these values into the equation: k×30=5×RR+2k \times 30 = \frac{5 \times R}{R+2} (Equation 2)

To find RR, we can divide Equation 1 by Equation 2: k×80k×30=10RR+15RR+2\frac{k \times 80}{k \times 30} = \frac{\frac{10R}{R+1}}{\frac{5R}{R+2}} 83=10RR+1×R+25R\frac{8}{3} = \frac{10R}{R+1} \times \frac{R+2}{5R} The RR in the numerator and denominator on the right side cancels out, and 10/5=210/5 = 2: 83=2(R+2)R+1\frac{8}{3} = \frac{2(R+2)}{R+1} Now, cross-multiply: 8(R+1)=3×2(R+2)8(R+1) = 3 \times 2(R+2) 8R+8=6R+128R + 8 = 6R + 12 8R6R=1288R - 6R = 12 - 8 2R=42R = 4 R=2ΩR = 2 \Omega

So, option B is correct.

Now, let's calculate the currents through RR for both steps:

Current through RR in Step-I (Is1I_{s1}): Is1=EsR+r=10 V2Ω+1Ω=103I_{s1} = \frac{E_s}{R+r} = \frac{10 \text{ V}}{2 \Omega + 1 \Omega} = \frac{10}{3} A So, option C is correct.

Current through RR in Step-II (Is2I_{s2}): Is2=EsR+r=5 V2Ω+2Ω=54I_{s2} = \frac{E_s}{R+r} = \frac{5 \text{ V}}{2 \Omega + 2 \Omega} = \frac{5}{4} A So, option D is correct.

Option A states R=1ΩR = 1 \Omega, which is incorrect.

Thus, options B, C, and D are all correct.