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IIT-JEE 2010 - Career Point

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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

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