NVAMediumJEE 2026Self & Mutual Inductance

JEE Physics 2026 Question with Solution

Inductance of a coil with 10410^4 turns is 10mH10 \, \text{mH} and it is connected to a DC source of 10V10 \, \text{V} with internal resistance 10Ω10 \, \Omega. The energy density in the inductor when the current reaches (1e)\left(\frac{1}{e}\right) of its maximum value is απ×1e2J m3\alpha \pi \times \frac{1}{e^2} \, \text{J m}^{-3}. The value of α\alpha is _____. (μ0=4π×107T m A1)\left(\mu_0 = 4\pi \times 10^{-7} \, \text{T m A}^{-1}\right)

Answer

Correct answer:500

Step-by-step solution

Standard Method

Given: Inductance L=10mHL = 10 \, \text{mH}, source voltage V=10VV = 10 \, \text{V}, internal resistance R=10ΩR = 10 \, \Omega, and the current is 1e\frac{1}{e} times its maximum value.

Find: The value of α\alpha in the energy density expression.

From the solution working,

Imax=VR=1010=1AI_{\max} = \frac{V}{R} = \frac{10}{10} = 1 \, \text{A}

So at the given instant,

I=1eImax=1eI = \frac{1}{e} I_{\max} = \frac{1}{e}

Magnetic energy density is

u=B22μ0u = \frac{B^2}{2\mu_0}

For a solenoid,

B=μ0nIB = \mu_0 n I

Hence,

ν=(μ0nI)22μ0=μ0n2I22\nu = \frac{(\mu_0 n I)^2}{2\mu_0} = \frac{\mu_0 n^2 I^2}{2}

Using

L=μ0n2AlL = \mu_0 n^2 A l

we get

ν=12LI2Al\nu = \frac{1}{2} \frac{L I^2}{A l}

Substituting the given values as in the provided solution,

ν=500π×1e2J m3\nu = 500\pi \times \frac{1}{e^2} \, \text{J m}^{-3}

Comparing with απ×1e2J m3\alpha \pi \times \frac{1}{e^2} \, \text{J m}^{-3}, we obtain α=500\alpha = 500.

Therefore, the value of α\alpha is 500500.

Solution Working

Given: The coil is connected to a DC source, so the maximum current is set by resistance, and the required current is 1e\frac{1}{e} of that value.

Find: The coefficient α\alpha.

  1. Find the maximum current:
Imax=VR=1010=1AI_{\max} = \frac{V}{R} = \frac{10}{10} = 1 \, \text{A}
  1. Current at the specified instant:
I=1eImax=1eI = \frac{1}{e} I_{\max} = \frac{1}{e}
  1. Use magnetic energy density:
ν=B22μ0\nu = \frac{B^2}{2\mu_0}
  1. For a solenoid:
B=μ0nI,n=NlB = \mu_0 n I, \qquad n = \frac{N}{l}
  1. Substitute for BB:
ν=(μ0nI)22μ0=μ0n2I22\nu = \frac{(\mu_0 n I)^2}{2\mu_0} = \frac{\mu_0 n^2 I^2}{2}
  1. Use the inductance relation:
L=μ0n2AlL = \mu_0 n^2 A l

So,

ν=12LI2Al\nu = \frac{1}{2} \frac{L I^2}{A l}
  1. The provided solution concludes:
ν=500π×1e2J m3\nu = 500\pi \times \frac{1}{e^2} \, \text{J m}^{-3}

Hence,

α=500\alpha = 500

Therefore, the final answer is 500500.

Common mistakes

  • Using the instantaneous current as I=11eI = 1 - \frac{1}{e} instead of I=1eImaxI = \frac{1}{e} I_{\max} is incorrect because the question directly states the current has reached 1e\frac{1}{e} of its maximum value. Use the stated fraction of maximum current.

  • Using magnetic energy U=12LI2U = \frac{1}{2} L I^2 directly as energy density is incorrect because energy density is energy per unit volume. Convert total energy to density by dividing by the volume of the inductor region.

  • Confusing total resistance with inductive reactance is incorrect because the source is DC. The maximum current is determined by Imax=VRI_{\max} = \frac{V}{R} using the internal resistance given.

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