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Question: A proton goes round in a circular orbit of radius 0.01 m under a centripetal force of \( 4\times 10^...

A proton goes round in a circular orbit of radius 0.01 m under a centripetal force of 4×1034\times 10^{-3} N. What is the frequency of revolution of protons?
A. 2.5×10122.5\times 10^{12} Hz
B. 4×10134\times 10^{13} Hz
C. 8×10128 \times 10^{12} Hz
D. 16×101216\times 10^{12} Hz

Explanation

Solution

Consider m=1.67×1027m = 1.67\times 10^{-27} . Since angular velocity(ω) occurs due to circular path, so covert v=rωv = r\omega , and convert ω to frequency to get the final answer.
Formula: For Centripetal force (Fc)=mω2R\left( {{F_c}} \right) = m{\omega ^2}R

Complete step by step solution:
It is important to understand that the centripetal force is not a fundamental force, but just a label given to the net force which causes an object to move in a circular path.
Given,
R(radius) = 0.01 m= 10210^{-2} m
Fc (centripetal force) = 4×1034\times 10^{-3} N
m=1.67×1027m = 1.67\times 10^{-27}
Using formula,
(Fc)=mω2R\left( {{F_c}} \right) = m{\omega ^2}R
4×103=(1.67×1027)×ω2×102 ω2=(4×103)(1.67×1027)×102   \Rightarrow 4\times {10^{ - 3}} = \left( {1.67\times {{10}^{ - 27}}} \right) \times {\omega ^2}\times{10^{ - 2}} \\\ \Rightarrow {\omega ^2} = \dfrac{{(4\times{{10}^{ - 3}})}}{{(1.67 \times {{10}^{ - 27}})\times{{10}^{ - 2}}}} \;
ω=1.55×1013\therefore \omega = 1.55 \times {10^{13}} (removing the squares)
Using formula,
ω=2πf f=ω2π=1.55×10132π=2.46×1012   \omega = 2\pi f \\\ \therefore f = \dfrac{\omega }{{2\pi }} = \dfrac{{1.55\times {{10}^{13}}}}{{2\pi }} = 2.46\times {10^{12}} \;
Thus, the required frequency is 2.5×10122.5\times 10^{12} Hz (approx.)
So, the correct answer is “Option A”.

Note: A centripetal force is a net force that acts on an object to keep it moving along a circular path.
Here we will see the one common example -: centripetal force is the case in which a body moves with uniform speed along a circular path. The centripetal force is directed at right angles to the motion and also along the radius towards the centre of the circular path.