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PHYSICS<br />
Students' Forum<br />
Expert’s Solution for Question asked by <strong>IIT</strong>-<strong>JEE</strong> Aspirants<br />
1. A homogeneous sphere of radius r rolls without<br />
slipping with constant angular speed ω' over bigger<br />
sphere, of radius R, which is in pure rotation with<br />
constant angular speed ω about its centre O. (Fig.)<br />
Find the time taken.<br />
ω<br />
R<br />
O<br />
ω′<br />
r<br />
C<br />
(i) for the centre C of the rolling sphere to return to its<br />
initial position (with respect to O), and<br />
(ii) for the point of contact of the rolling sphere to make<br />
one full revolution over the bigger rotating sphere.<br />
(b)(i) Determine the acceleration of the contact point of the<br />
rolling sphere, and<br />
(ii) the point of greatest acceleration of the rolling sphere<br />
(both w.r.t. the centre O)<br />
Sol. Suppose that at t = 0, the contact points of lie along<br />
the fixed line (reference line) OX. Let at time t the<br />
line OC makes the angle θ with OX (Fig.)<br />
ω<br />
O<br />
^<br />
t<br />
C<br />
P<br />
θ P′<br />
It is better to express the velocity and acceleration of<br />
any point including contact point P (say) at an<br />
arbitrary instant of time t as,<br />
v po = v co and a po = a co = a pc + a pc + a co (1)<br />
We know that in the case of pure rolling the velocity<br />
of contact point of the rolling body has zero velocity<br />
and zero tangential acceleration relative to the contact<br />
point of the surface on which it rolls. So if P′ be the<br />
contact point of rotating sphere at time t, then<br />
v p′o = v po<br />
So, v p'o = v pc + v co (2)<br />
ω′<br />
X<br />
(a) If t is the direction of common tangent, then from<br />
eqn. (2)<br />
v p'o (t) = v pc (t) + v co (t)<br />
⎛ dθ<br />
⎞<br />
ωR = – ω′R + ⎜ ⎟ (R + r)<br />
⎝ dt ⎠<br />
dθ ωR<br />
+ ω'r<br />
or,<br />
=<br />
(3)<br />
dt R + r<br />
R + r<br />
so, dt =<br />
dθ (4)<br />
( ωR<br />
+ ω'r)<br />
(ii) It is simple to observer if rotating sphere were at rest,<br />
the CM of rolling sphere C will turn by the angle 2 π,<br />
⎛ dθ<br />
⎞<br />
with angular speed ⎜ ⎟ – ω to satisfy the condition<br />
⎝ dt ⎠<br />
of the problem.<br />
dθ<br />
dt<br />
ω<br />
Hence the sought time t′ (say) is given by<br />
2π<br />
2π(R<br />
+ r)<br />
t′ = = [using Eq. (4)]<br />
⎛ dθ<br />
⎞ r( ω−ω ' )<br />
⎜ ⎟ − ω<br />
⎝ dt ⎠<br />
(b) From a po = a pc + a co = a pc (tangential) + a pc (normal) + a co<br />
In our case a pc (tangential) = 0, because ω′ = constant<br />
Hence, a po = a pc (normal) + a co (5)<br />
⎡<br />
2<br />
⎤<br />
2 ⎛ dθ<br />
⎞<br />
a po = ⎢− ω'<br />
r + ⎜ ⎟ (R + r)<br />
⎥<br />
⎢⎣<br />
⎝ dt ⎠ ⎥⎦<br />
dθ ωR<br />
+ ω'r<br />
(using = from equation (3) or part (a))<br />
dt R + r<br />
(ii) From eqn. (5) it is obvious that the maximum value<br />
|apo | ma x = |a pc (normal) | + | a co |<br />
2<br />
= – ω′ 2 ⎛ dθ<br />
⎞<br />
r + ⎜ ⎟⎠ (R + r)<br />
⎝ dt<br />
dθ<br />
where will be substituted from Eqn. (3).<br />
dt<br />
XtraEdge for <strong>IIT</strong>-<strong>JEE</strong> 22 DECEMBER 2009