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QJEEM24Phdd31: JEE Main 2024 Physics - Class 12 JEEM24Phdd31 Solution: To measure the internal resistance of a battery, potentiometer…

To measure the internal resistance of a battery, potentiometer is used. For R=10ΩR=10 \Omega , the balance point is observed at l=500 cml=500 \mathrm{~cm} and for R=1Ω\mathrm{R}=1 \Omega the balance point is observed at l=400 cml=400 \mathrm{~cm} . The internal resistance of the battery is approximately :

Multiple Choice Options

  • A 0.1Ω0.1 \Omega
  • B 0.3Ω0.3 \Omega
  • C 0.2Ω0.2 \Omega
  • D 0.4Ω0.4 \Omega

Step-by-Step Verified Solution

To measure the internal resistance of a battery using a potentiometer, we need to understand the principle behind it. The potentiometer is used to measure the voltage across the battery (emf) under different conditions. The balance length corresponds to the emf of the battery when no current is drawn, whereas under load, it corresponds to the terminal voltage.

Let's denote the emf of the battery by EE and the internal resistance by rr . According to Ohm's law, when a resistance RR is connected across the battery, the terminal voltage VV is given by:

V=E−IrV = E - Ir

where II is the current through the circuit.

From the problem, the balance length ll is proportional to the voltage across the potentiometer wire. Thus, we can write:

V1V2=l1l2\frac{V_1}{V_2} = \frac{l_1}{l_2}

In the first condition, when R=10ΩR = 10 \Omega and the balance length l1=500 cml_1 = 500 \, \text{cm} :

V1=E−I1rV_1 = E - I_1 r

For the second condition, when R=1ΩR = 1 \Omega and the balance length l2=400 cml_2 = 400 \, \text{cm} :

V2=E−I2rV_2 = E - I_2 r

Given that:

V1V2=500400=54\frac{V_1}{V_2} = \frac{500}{400} = \frac{5}{4}

Now let's denote the internal emf of the battery as EE . We can use Ohm’s Law in the calculation of I1I_1 and I2I_2 :

I1=ER1+r=E10+rI_1 = \frac{E}{R_1 + r} = \frac{E}{10 + r}

I2=ER2+r=E1+rI_2 = \frac{E}{R_2 + r} = \frac{E}{1 + r}

Now, rewriting the values of V1V_1 and V2V_2 we have:

V1=E−I1r=E(1−r10+r)=E1010+rV_1 = E - I_1 r = E \left(1 - \frac{r}{10 + r}\right) = E \frac{10}{10 + r}

V2=E−I2r=E(1−r1+r)=E11+rV_2 = E - I_2 r = E \left(1 - \frac{r}{1 + r}\right) = E \frac{1}{1 + r}

Using the ratio:

V1V2=10E10+rE1+r=10⋅(1+r)1⋅(10+r)=10+10r10+r\frac{V_1}{V_2} = \frac{\frac{10E}{10 + r}}{\frac{E}{1 + r}} = \frac{10 \cdot (1 + r)}{1 \cdot (10 + r)} = \frac{10 + 10r}{10 + r}

Given:

V1V2=54\frac{V_1}{V_2} = \frac{5}{4}

So, we can set up the equation:

10+10r10+r=54\frac{10 + 10r}{10 + r} = \frac{5}{4}

Cross multiplying gives:

4(10+10r)=5(10+r)4(10 + 10r) = 5(10 + r)

Expanding both sides:

40+40r=50+5r40 + 40r = 50 + 5r

Rearranging terms to solve for rr :

40r−5r=50−4040r - 5r = 50 - 40

35r=1035r = 10

r=1035=27≈0.285 Ωr = \frac{10}{35} = \frac{2}{7} \approx 0.285 \, \Omega

Since this value is closest to 0.3Ω0.3 \Omega , the correct option is:

Option B: 0.3Ω0.3 \Omega

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