A particle of mass m and charge q is placed in an electric field e which varies with time as equal to
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Equation of motion of the particle is
mdvdt=qE0sin(ωt) mdvdt=qE0sin(ωt)
which upon integrating gives,
m∫dv=qE0∫sin(ωt)dtv=−qE0mωcos(ωt) +C1 m∫dv=qE0∫sin(ωt)dtv=-qE0mωcos(ωt) +C1
where C1 is the constant of integration.
so ,
dxdt=−qE0mωcos(ωt) +C1 dxdt=-qE0mωcos(ωt) +C1
which , upon integration again , gives
∫dx=−qE0mω∫(cos(ωt) +C1)dtx=−qE0mω2sin(ωt) +C1t+C2∫dx=−qE0mω∫(cos(ωt) +C1)dtx=-qE0mω2sin(ωt) +C1t+C2
The first term on the right hand provides the simple harmonic part ,
So, the amplitude of the simple harmonic part of the solution is
qE0mω2
Explanation:
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