In Figure above, a
3
0
k
g
child stands on the edge of a stationary merry-go-round of radius
2
.
0
m
. The rotational inertia of the merry-go-round about its rotation axis is
1
5
0
k
g
m
2
• The child catches a ball of mass
1
.
0
k
g
thrown by a friend. Just before the ball is caught, it has a horizontal velocity
v
of magnitude
1
2
m
/
s
, at angle
ϕ
=
3
7
°
with. a line tangent to the outer edge of the merry-go-round, as shown. What is the angular speed (in rad/sec) of the merry-go-round just after the ball is caught?
Liked it try some more
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In case of collisions it is better to talk in terms of angular impulse rather than torque.
How come it's a level 5 problem!!!!
Yes L = I ω = c o n s t a n t we have L i n i t i a l = ( m b a l l ) ( v c o s t h e t a ) ( R ) note v sin theta is irrelevant as it is along radius.And expression for I is I t o t a l = ( m b a l l + m c h i l d ) R 2 + I m e r r y g o r o u n d .There now we have all the information.just substitute to get ω .
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AS NET TORQUE ABOUT THE CENTER OF MERRY GO ROUND IS ZERO WE CAN CONSERVE ANGULAR MOMENTUM ABOUT IT. m=mass of ball.
M=mass of child
r=radius of merry go round
L i = L f
m v r s i n ( 9 0 − ϕ ) = I ω
I = 1 5 0 + m r 2 + M r 2 = 2 7 4 k g − m 2
m v r sin ( 9 0 − ϕ ) = 1 × 1 2 × 2 s i n 5 3 = 1 9 . 2
19.2=274 ω
ω =0.070