NVAMediumJEE 2023Electric Field & Field Lines

JEE Physics 2023 Question with Solution

An electron revolves around an infinite cylindrical wire having uniform linear charge density 2×108C/m12 \times 10^{-8} \, C/m^{-1} in a circular path under the influence of an attractive electrostatic field as shown in the figure. The velocity of the electron with which it is revolving is _____ ×106m/s1\times 10^6 \, m/s^{-1}. Given mass of the electron =9×1031kg= 9 \times 10^{-31} \, kg

A vertical infinitely long positively charged cylindrical wire with plus signs, and an electron moving in a circular orbit around the wire with radius r.

Answer

Correct answer:8

Step-by-step solution

Standard Method

Given: Linear charge density λ=2×108C/m\lambda = 2 \times 10^{-8} \, \text{C/m}, mass of electron m=9×1031kgm = 9 \times 10^{-31} \, \text{kg}, charge of electron e=1.6×1019Ce = 1.6 \times 10^{-19} \, \text{C}.

Find: The value of velocity in the form v=(__)×106m/sv = (\_\_) \times 10^6 \, \text{m/s}.

For an infinite line charge, the electric field at distance rr is

E=λ2πϵ0rE = \frac{\lambda}{2\pi \epsilon_0 r}

The electrostatic force on the electron is

F=eE=eλ2πϵ0rF = eE = \frac{e\lambda}{2\pi \epsilon_0 r}

This force provides the centripetal force for circular motion:

mv2r=eλ2πϵ0r\frac{mv^2}{r} = \frac{e\lambda}{2\pi \epsilon_0 r}

Cancelling rr from both sides,

v2=eλ2πϵ0mv^2 = \frac{e\lambda}{2\pi \epsilon_0 m}

Therefore,

v=eλ2πϵ0mv = \sqrt{\frac{e\lambda}{2\pi \epsilon_0 m}}

Substituting the given values,

v=(1.6×1019)(2×108)2π(8.85×1012)(9×1031)v = \sqrt{\frac{(1.6 \times 10^{-19})(2 \times 10^{-8})}{2\pi(8.85 \times 10^{-12})(9 \times 10^{-31})}} v=3.2×10275.0×1041v = \sqrt{\frac{3.2 \times 10^{-27}}{5.0 \times 10^{-41}}} v=6.4×1013v = \sqrt{6.4 \times 10^{13}} v8×106m/sv \approx 8 \times 10^6 \, \text{m/s}

Therefore, the required numerical value is 8.

Radius Cancellation Insight

Given: The electron moves in a circular path around an infinite line charge.

Find: Why the speed can be found without knowing the radius.

The electric field of an infinite line charge varies as 1/r1/r, so the electrostatic force on the electron also varies as 1/r1/r. The centripetal force requirement is

mv2r\frac{mv^2}{r}

which also contains the same 1/r1/r dependence after equating forces. Hence the radius cancels immediately:

mv2r=eλ2πϵ0r\frac{mv^2}{r} = \frac{e\lambda}{2\pi \epsilon_0 r} v2=eλ2πϵ0mv^2 = \frac{e\lambda}{2\pi \epsilon_0 m}

So the speed depends only on ee, λ\lambda, ϵ0\epsilon_0 and mm, not on the orbit radius. Substituting values gives v8×106m/sv \approx 8 \times 10^6 \, \text{m/s}. Therefore, the required numerical value is 8.

Common mistakes

  • Using the electric field formula of a point charge instead of that of an infinite line charge is incorrect because the symmetry is cylindrical, not spherical. Use E=λ2πϵ0rE = \frac{\lambda}{2\pi\epsilon_0 r} for an infinite wire.

  • Keeping the electron charge as negative while computing the magnitude of force can create sign confusion. For centripetal force, equate magnitudes and use the negative sign only to indicate that the force is attractive toward the wire.

  • Forgetting that rr cancels on both sides leads to unnecessary dependence on orbit radius. Since both electrostatic force and centripetal requirement contain 1/r1/r, the speed is independent of rr here.

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