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Current Electricity question

2014 · Shift 2 · Q48
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Current Electricity question

2014 · Shift 2 · Q48

JEE AdvancedPhysicsCurrent ElectricityMCQ+3 / −1
During an experiment with a metre bridge, the galvanometer shall a null point when the jockey is pressed at 40.0 cm using a standard resistance of 90 Ω\OmegaΩ, as shown in the figure. The least count of the scale used in the meter bridge is 1 mm. The unknown resistance is JEE Advanced 2014 Paper 2 Offline Physics - Current Electricity Question 17 English
  1. A
    60 ±\pm± 0.15 Ω\OmegaΩ
  2. B
    135 ±\pm± 0.56 Ω\OmegaΩ
  3. C
    60 ±\pm± 0.25 Ω\OmegaΩ
  4. D
    135 ±\pm± 0.23 Ω\OmegaΩ
View written solutionFree

Correct answer: C

Step-by-step Solution

  1. Principle of a Metre Bridge: A metre bridge works on the principle of a balanced Wheatstone bridge. When the galvanometer shows a null deflection, the ratio of resistances is equal to the ratio of the corresponding lengths of the bridge wire. The formula for a balanced metre bridge is: RS=l100−l\frac{R}{S} = \frac{l}{100 - l}SR​=100−ll​ where:

    • R is the unknown resistance.
    • S is the standard known resistance.
    • l is the balancing length from the end connected to R.
  2. Identify Given Values: From the problem statement:

    • Standard resistance, S=90ΩS = 90 \OmegaS=90Ω
    • Balancing length, l=40.0 cml = 40.0 \text{ cm}l=40.0 cm
    • Least count of the scale, Δl=1 mm=0.1 cm\Delta l = 1 \text{ mm} = 0.1 \text{ cm}Δl=1 mm=0.1 cm. This represents the error in the length measurement.
  3. Calculate the Unknown Resistance (R): Using the metre bridge formula, we can solve for R: R=S(l100−l)R = S \left( \frac{l}{100 - l} \right)R=S(100−ll​) Substitute the given values: R=90(40.0100−40.0)R = 90 \left( \frac{40.0}{100 - 40.0} \right)R=90(100−40.040.0​) R=90(40.060.0)R = 90 \left( \frac{40.0}{60.0} \right)R=90(60.040.0​) R=90×23R = 90 \times \frac{2}{3}R=90×32​ R=60ΩR = 60 \OmegaR=60Ω

  4. Error Analysis: To find the error in R (ΔR\Delta RΔR), we use the formula for error propagation. The relation is R=Sl100−lR = S \frac{l}{100 - l}R=S100−ll​. Assuming the standard resistance S is error-free, the error in R depends on the error in measuring l.

    The relative error in R can be found by taking the logarithm and differentiating: ln⁡(R)=ln⁡(S)+ln⁡(l)−ln⁡(100−l)\ln(R) = \ln(S) + \ln(l) - \ln(100 - l)ln(R)=ln(S)+ln(l)−ln(100−l) Differentiating to find the fractional error: ΔRR=Δll+Δ(100−l)100−l\frac{\Delta R}{R} = \frac{\Delta l}{l} + \frac{\Delta(100 - l)}{100 - l}RΔR​=lΔl​+100−lΔ(100−l)​ Since Δ(100−l)\Delta(100 - l)Δ(100−l) is the error in (100-l) which is the same as the error in l, i.e., Δl\Delta lΔl, we have: ΔRR=Δll+Δl100−l\frac{\Delta R}{R} = \frac{\Delta l}{l} + \frac{\Delta l}{100 - l}RΔR​=lΔl​+100−lΔl​ ΔRR=Δl(1l+1100−l)\frac{\Delta R}{R} = \Delta l \left( \frac{1}{l} + \frac{1}{100 - l} \right)RΔR​=Δl(l1​+100−l1​) ΔRR=Δl(100−l+ll(100−l))\frac{\Delta R}{R} = \Delta l \left( \frac{100 - l + l}{l(100 - l)} \right)RΔR​=Δl(l(100−l)100−l+l​) ΔRR=100Δll(100−l)\frac{\Delta R}{R} = \frac{100 \Delta l}{l(100 - l)}RΔR​=l(100−l)100Δl​

  5. Calculate the Absolute Error (\Delta R): Now, we can find ΔR\Delta RΔR: ΔR=R(100Δll(100−l))\Delta R = R \left( \frac{100 \Delta l}{l(100 - l)} \right)ΔR=R(l(100−l)100Δl​) Substitute the known values:

    • R=60ΩR = 60 \OmegaR=60Ω
    • Δl=0.1 cm\Delta l = 0.1 \text{ cm}Δl=0.1 cm
    • l=40.0 cml = 40.0 \text{ cm}l=40.0 cm ΔR=60(100×0.140.0×(100−40.0))\Delta R = 60 \left( \frac{100 \times 0.1}{40.0 \times (100 - 40.0)} \right)ΔR=60(40.0×(100−40.0)100×0.1​) ΔR=60(1040×60)\Delta R = 60 \left( \frac{10}{40 \times 60} \right)ΔR=60(40×6010​) ΔR=60×102400\Delta R = 60 \times \frac{10}{2400}ΔR=60×240010​ ΔR=6002400=14\Delta R = \frac{600}{2400} = \frac{1}{4}ΔR=2400600​=41​ ΔR=0.25Ω\Delta R = 0.25 \OmegaΔR=0.25Ω
  6. Final Result: The unknown resistance is expressed as R±ΔRR \pm \Delta RR±ΔR. Therefore, the unknown resistance is 60±0.25Ω60 \pm 0.25 \Omega60±0.25Ω.

  7. Conclusion: Comparing our result with the given options: A: 60 ±\pm± 0.15 Ω\OmegaΩ B: 135 ±\pm± 0.56 Ω\OmegaΩ C: 60 ±\pm± 0.25 Ω\OmegaΩ D: 135 ±\pm± 0.23 Ω\OmegaΩ

    Our calculated value matches option C.

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