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JEE Main 2018 · Physics · Electrostatics · hard

A proton moving at 2×10^5 m s^-1 enters, perpendicular to its boundary, a region of uniform magnetic field 0.5 T directed perpendicular to the…

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A proton moving at 2×105 m s−12\times10^5\ \mathrm{m\,s^{-1}} enters, perpendicular to its boundary, a region of uniform magnetic field 0.5 T0.5\ \mathrm{T} directed perpendicular to the velocity. The region has width 2 mm2\ \mathrm{mm}. Take the proton mass as 1.6×10−27 kg1.6\times10^{-27}\ \mathrm{kg} and charge 1.6×10−19 C1.6\times10^{-19}\ \mathrm{C}. The time the proton spends inside the field is nearly
  1. A. 62.8 ns62.8\ \mathrm{ns}
  2. B. 10.5 ns10.5\ \mathrm{ns}
  3. C. 21.0 ns21.0\ \mathrm{ns}
  4. D. 31.4 ns31.4\ \mathrm{ns}
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Answer: (B) 10.5 ns10.5\ \mathrm{ns}

Radius of the path: r=mvqB=1.6×10−27×2×1051.6×10−19×0.5=4 mmr=\dfrac{mv}{qB}=\dfrac{1.6\times10^{-27}\times2\times10^5}{1.6\times10^{-19}\times0.5}=4\ \mathrm{mm}. Entering normally to the boundary, the proton has turned through angle θ\theta when it has advanced rsin⁡θr\sin\theta into the region; it leaves the far side when rsin⁡θ=2 mmr\sin\theta=2\ \mathrm{mm}, so sin⁡θ=12\sin\theta=\tfrac12 and θ=30∘=π/6\theta=30^\circ=\pi/6. The angular speed is ω=qBm=5×107 rad s−1\omega=\dfrac{qB}{m}=5\times10^7\ \mathrm{rad\,s^{-1}}, so t=θω=π/65×107=1.05×10−8 s≈10.5 nst=\dfrac{\theta}{\omega}=\dfrac{\pi/6}{5\times10^7}=1.05\times10^{-8}\ \mathrm{s}\approx10.5\ \mathrm{ns}.
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