NVAMediumJEE 2025Force on Current-Carrying Conductor

JEE Physics 2025 Question with Solution

A tightly wound long solenoid carries a current of 1.5A1.5 \, \text{A}. An electron is executing uniform circular motion inside the solenoid with a time period of 75×109s75 \times 10^{-9} \, \text{s}. The number of turns per meter in the solenoid is _____.

Answer

Correct answer:250

Step-by-step solution

Standard Method

Given: current in the solenoid is I=1.5AI = 1.5 \, \text{A} and the time period of the electron is T=75×109sT = 75 \times 10^{-9} \, \text{s}.

Find: the number of turns per meter nn in the solenoid.

Inside a long solenoid, the magnetic field is

B=μ0nIB = \mu_0 n I

For the electron in uniform circular motion, magnetic force provides the centripetal force:

evB=mv2re v B = \frac{m v^2}{r}

Using

T=2πrvT = \frac{2\pi r}{v}

we get

v=2πrTv = \frac{2\pi r}{T}

Substituting in the force relation,

B=mver=mer2πrT=2πmeTB = \frac{m v}{e r} = \frac{m}{e r}\cdot \frac{2\pi r}{T} = \frac{2\pi m}{eT}

Now substitute m=9.11×1031kgm = 9.11 \times 10^{-31} \, \text{kg}, e=1.6×1019Ce = 1.6 \times 10^{-19} \, \text{C} and T=75×109sT = 75 \times 10^{-9} \, \text{s}:

B=2π×9.11×10311.6×1019×75×109=1.58×103TB = \frac{2\pi \times 9.11 \times 10^{-31}}{1.6 \times 10^{-19} \times 75 \times 10^{-9}} = 1.58 \times 10^{-3} \, \text{T}

Using

B=μ0nIB = \mu_0 n I

with μ0=4π×107T m/A\mu_0 = 4\pi \times 10^{-7} \, \text{T m/A} and I=1.5AI = 1.5 \, \text{A},

1.58×103=(4π×107)n×1.51.58 \times 10^{-3} = (4\pi \times 10^{-7}) n \times 1.5

So,

n=1.58×103(4π×107)×1.5=250n = \frac{1.58 \times 10^{-3}}{(4\pi \times 10^{-7}) \times 1.5} = 250

Therefore, the number of turns per meter in the solenoid is 250250.

Direct Cyclotron-Period Relation

Given: I=1.5AI = 1.5 \, \text{A} and T=75×109sT = 75 \times 10^{-9} \, \text{s}.

Find: nn.

For a charged particle moving perpendicular to a uniform magnetic field, the time period is directly

T=2πmeBT = \frac{2\pi m}{eB}

Hence,

B=2πmeTB = \frac{2\pi m}{eT}

For a long solenoid,

B=μ0nIB = \mu_0 n I

Therefore,

n=2πmμ0eTIn = \frac{2\pi m}{\mu_0 e T I}

Substituting the values,

n=2π×9.11×1031(4π×107)(1.6×1019)(75×109)(1.5)250n = \frac{2\pi \times 9.11 \times 10^{-31}}{(4\pi \times 10^{-7})(1.6 \times 10^{-19})(75 \times 10^{-9})(1.5)} \approx 250

This shortcut works because the orbital time period in a magnetic field is independent of the radius and speed. Therefore, the required number of turns per meter is 250250.

Common mistakes

  • Using B=mv2erB = \frac{mv^2}{er} without then relating vv and rr through the time period is incomplete. The correct approach is to use T=2πrvT = \frac{2\pi r}{v} so that rr cancels out.

  • Substituting 75ns75 \, \text{ns} as 75×109s75 \times 10^{9} \, \text{s} or as 75s75 \, \text{s} gives a wildly incorrect field. Convert nanoseconds correctly as 75×109s75 \times 10^{-9} \, \text{s}.

  • Forgetting that the magnetic field inside a long solenoid is B=μ0nIB = \mu_0 n I, not just proportional to nn alone, leads to a missing factor of current. Always substitute the given current 1.5A1.5 \, \text{A}.

Practice more Force on Current-Carrying Conductor questions

Get unlimited AI-adaptive practice, mastery tracking, and an AI tutor that explains every step — free to start.

Related questions