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JEE Main 20253 AprilMorning Shift
Exam
JEE Main
Year
2025
Date
3 April
Shift
Morning Shift
Subject
Physics
Chapter
Oscillations

JEE Main 2025 · 3 April · Morning Shift · Physics · Oscillations

Two blocks of masses m and M,(M m) , are placed on a frictionless...

Two blocks of masses mm and M,(M>m)M,(M \gt m), are placed on a frictionless table as shown in figure. A massless spring with spring constant k is attached with the lower block. If the system is slightly displaced and released then
(μ=\mu= coefficient of friction between the two blocks)
Two blocks of masses m and M,(M m) , are placed on a frictionless table as shown in figure. A massless spring with
(A) The time period of small oscillation of the two blocks is T=2π( m+M)k\mathrm{T}=2 \pi \sqrt{\frac{(\mathrm{~m}+\mathrm{M})}{\mathrm{k}}}
(B) The acceleration of the blocks is a=kxM+m\mathrm{a}=\frac{\mathrm{kx}}{\mathrm{M}+\mathrm{m}} (x=\mathrm{x}= displacement of the blocks from the mean position)
(C) The magnitude of the frictional force on the upper block is mμ∣x∣M+m\frac{m \mu|x|}{M+m}
(D) The maximum amplitude of the upper block, if it does not slip, is μ(M+m)gk\frac{\mu(M+m) g}{k}
(E) Maximum frictional force can be μ(M+m)g\mu(\mathrm{M}+\mathrm{m}) \mathrm{g}.
Choose the correct answer from the options given below:

Options

  1. AA, B, D Only
  2. BB, C, D Only
  3. CC, D, E Only
  4. DA, B, C Only

Correct answer

A. A, B, D Only

Step-by-step solution

(A) As both blocks moving together so Time period =2π m K;=2 \pi \sqrt{\frac{\mathrm{~m}}{\mathrm{~K}}} ; where m=M+m\mathrm{m}=\mathrm{M}+\mathrm{m}
T=2πM+m K\mathrm{T}=2 \pi \sqrt{\frac{\mathrm{M}+\mathrm{m}}{\mathrm{~K}}}
(B) Let block is displaced by x in (+ve)(+\mathrm{ve}) direction so force on block will be in(-ve) direction
<br/>F=−Kx(M+m)a=−Kxa=−Kx(M+m)<br/>\begin{aligned}<br/>& \mathrm{F}=-\mathrm{Kx} \\ & (\mathrm{M}+\mathrm{m}) \mathrm{a}=-\mathrm{Kx} \\ & \mathrm{a}=-\frac{\mathrm{Kx}}{(\mathrm{M}+\mathrm{m})}<br/>\end{aligned}
(C) As upper block is moving due to friction thus
f=ma=mKx(M+m)\mathrm{f}=\mathrm{ma}=\frac{\mathrm{mKx}}{(\mathrm{M}+\mathrm{m})}
(D) This option is like two block problem in friction for maximum amplitude, force on block is also maximum, for which both blocks are moving together.
Two blocks of masses m and M,(M m) , are placed on a frictionless table as shown in figure. A massless spring with
<br/>KA=(M+m)aa=KA(M+m)f=ma=mKA(M+m)fmax⁡=fL=μmgf=μmgmKA(M+m)=μmgA=μ(M+m)gK<br/>\begin{aligned}<br/>& K A=(M+m) a \\ & a=\frac{K A}{(M+m)} \\ & f=m a=\frac{m K A}{(M+m)} \\ & f_{\max }=f_L=\mu \mathrm{mg} \\ & f=\mu m g \\ & \frac{m K A}{(M+m)}=\mu m g \\ & A=\frac{\mu(M+m) g}{K}<br/>\end{aligned}
(E) Maximum friction can be μmg\mu \mathrm{mg} as force is acting between blocks \& normal force here is mg.
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