no virag .......dont think ur right abt the mag.
A man pushes a cylinder of mass m1 with the help of a plank m2 as shown in the figure. there is no slipping at any contact.
the horizontal component of the force applied by the man is F.
a ) Find the acceleration of plank and the center of mass of the cylinder
b) the magnitudes of direction of frictional forces at contact points...
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5 Answers
(a) Let the plank move by distance x, then the center of mass of cylinder moves by x/2.
Hence, by work energy principle
Fx=\dfrac{1}{2}m_2v_2^2+\dfrac{1}{2}m_1v_1^2 + \dfrac{1}{2}\cdot \dfrac{1}{2}m_1R^2\omega^2
Here, v1 and v2 are, respectively, the speeds of c.m of cylinder and the plank, and ω is the angular speed of the cylinder. Since
v_2=2v_1, \qquad \textrm{and}\quad \omega = \dfrac{v_1}{R}=\dfrac{v_2}{2R}
we get
Fx=\dfrac{1}{2}m_2v_2^2 + \dfrac{1}{2}m_1\dfrac{v_2^2}{4}+ \dfrac{1}{2}m_1\dfrac{v_2^2}{8}
i.e.
Fx=\dfrac{1}{2}v_2^2\left(m_2+\dfrac{3}{8}m_1\right)
Hence,
v_2=\sqrt{\dfrac{2Fx}{m_2+\frac{3}{8}m_1}}
Comparison with v=√2as gives the acceleration a2 of the plank as
a_2=\dfrac{F}{m_2+\frac{3}{8}m_1}=\dfrac{8F}{8m_2+3m_1}
Hence, the acceleration of the center of mass of the cylinder
a_1=\dfrac{a_2}{2}=\dfrac{4F}{8m_2+3m_1}
(b) Let f_2 be the force of friction between the plank and the cylinder, then
F-f_2=m_2a_2, which give
f_2=F-m_2a_2=F-\dfrac{8m_2F}{8m_2+3m_1}=\dfrac{3m_1F}{8m_2+3m_1}
Let f1 be the friction force between the cylinder and the ground, then f1 must act forward. Hence, we get
f1+f2 = m1a1
from where we get
f_1=m_1a_1-f_2=\dfrac{4m_1F}{8m_2+3m_1}-\dfrac{3m_1F}{8m_2+3m_1}=\dfrac{m_1F}{8m_2+3m_1}
ajet tesla Why ç.m moves by X/2 distance
Upvote·0· Reply ·2018-11-29 09:07:39ajet tesla And I can't understand w=V2/2r =v1r
ajet tesla Means how V1= 2 v2 it comes
F - f = m2a2 ...(1)
(f-f2)R = Iα .........(2)
f + f2 = m1a1 ........(3)
a1 = Rα .........................(4)
a1 + a2 + Rα= 0 ...................(5)
PLS CHECK IF EQXNS ARE RITE SIR
ive taken alpha in anti clock dir and a1 and a2 rightward............
Magnitude and direction of friction
Friction at the top of the ball
The direction is opposite to the force applied.
Force of friction = Ï
1m2g providing anti-clockwise motion
Friction at the bottom
The direction is to provide clockwise rotation.
Force of friction =Ï
2(m1+m2)g