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Simple Harmonic Motion question

2006 · Shift 0 · Q125
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  5. /2006 · Shift 0 · Q125

Simple Harmonic Motion question

2006 · Shift 0 · Q125

JEE MainPhysicsSimple Harmonic MotionMCQ+4 / −1
A coin is placed on a horizontal platform which undergoes vertical simple harmonic motoin of angular frequency ω.\omega .ω. The amplitude of oscillation is gradually increased. The coin will leave contact with the platform for the first time
  1. A
    at the mean position of the platform
  2. B
    for an amplitude of gω2{g \over {{\omega ^2}}}ω2g​
  3. C
    For an amplitude of g2ω2{{{g^2}} \over {{\omega ^2}}}ω2g2​
  4. D
    at the height position of the platform
View written solutionFree

Correct answer: B

  1. Condition for losing contact

A coin placed on a vertically oscillating platform remains in contact as long as the normal reaction N≥0N \ge 0N≥0.

Taking upward as positive, for the coin while in contact: N−mg=maN - mg = maN−mg=ma So, N=m(g+a)N = m(g+a)N=m(g+a)

The coin will leave the platform when contact just breaks, i.e. N=0N=0N=0 Hence, g+a=0⇒a=−gg+a=0 \Rightarrow a=-gg+a=0⇒a=−g

So the coin loses contact when the downward acceleration of the platform becomes equal to ggg.


  1. Acceleration in SHM

If the platform executes SHM with amplitude AAA and angular frequency ω\omegaω, then a=−ω2ya=-\omega^2 ya=−ω2y where yyy is displacement from mean position.

Maximum downward acceleration occurs at the topmost position: amin⁡=−ω2Aa_{\min}=-\omega^2 Aamin​=−ω2A

For the coin to leave contact for the first time, this maximum downward acceleration must just equal −g-g−g: −ω2A=−g-\omega^2 A=-g−ω2A=−g ω2A=g\omega^2 A=gω2A=g A=gω2A=\frac{g}{\omega^2}A=ω2g​


  1. Check the instant/position

At the threshold amplitude A=gω2A=\dfrac{g}{\omega^2}A=ω2g​, contact is first lost when the platform is at the highest position, because that is where downward acceleration is maximum.

So:

  • Option A: false
  • Option B: true
  • Option C: false
  • Option D: false

  1. Final answer

The coin leaves contact for the first time when the amplitude reaches gω2\boxed{\frac{g}{\omega^2}}ω2g​​ which corresponds to Option B.

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