A solid spherical ball of radius 5m is projected to the right from a rough ground with a velocity 10 m/s at an angle θ with the horizontal. Also at the same time it is given an angular velocity of 3 rad/s clockwise such that axis of rotation is perpendicular to plane of projectile .
Let horizontal distance travelled by the ball from the point of projection to the point where it made it's second bounce be D . Given that maximum value of D occurs at θ = arccos c ( a − b ) where a , b , c are integers, a is square free, b , c are co-prime then find a + b + c .
Assumptions and details
Co-efficient of friction of ground with the ball is 3 1
Mass of the ball = 5 kg
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Please comment if you believe the solution to be wrong and please upvote it if you believe it to be right
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You should have informed if ball is going right or left, because the ball's rotation can be help or disturb the ball's movement.
But thanks for more this question, I'll keep it in my favorite set!
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I believed that the convention is assumed to be right. Anyway I will put up a diagram to the question
Same but I use angular momentum conservation about bottom most point.
( 1 0 cos θ ) r + 5 2 m r 2 ω o = V x " r + 5 2 m r 2 ω " .
Nice question @Ronak agarwal ! But the most important part of this question is that to think that sphere Can Rolls purely .
And I think You should state in question that there is sufficient friction instead of giving coefficient of friction to remove ambiguity in question
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You are missing one thing @Deepanshu Gupta here, first thing there is no ambiguity in the question, in fact you have to check whether the case of maximum range there is sufficient friction or not, I have checked it while making this question and it came out to be sufficient. Don't underappriciate this part of the question.
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Oh Okay I got it ! Amazing !!
. Really This is beautiful part of this question! Thanks for notifying me for this.
@Ronak Agarwal
Could you please help me out? This is how I proceeded. After finding out that the angular velocity will make the friction point in the right direction during the first bounce, we also see that the angular momentum decreases.
L e t N b e t h e v e r t i c a l f o r c e t h a t a c t s o n t h e b a l l o n t h e f i r s t b o u n c e . N = d t d P = Δ t Δ P W e k n o w , V f v = 2 V i v ( v f o r v e r t i c a l ) Δ P = 2 3 m v sin θ ( t a k i n g s i g n s i n t o c o n s i d e r a t i o n ) N Δ t = 2 3 m v sin θ N o w , f r i c t i o n a l f o r c e = 3 N τ = 3 N r = Δ t Δ L = Δ t I ( w f − w i ) o r Δ t I ( w i − w f ) ( S i n c e w i > w f ) N Δ t = 3 × 5 2 m r × ( 3 − w f ) W e g e t , 2 3 m v sin θ = 5 6 m r ( 3 − w f ) W h i c h g i v e s u s , w f = 3 − 2 5 sin θ T h e n w e u s e c o n s e r v a t i o n o f a n g u l a r m o m e n t u m a b o u t t h e p o i n t o f c o n t a c t t o f i n d h o r i z o n t a l c o m p o n e n t o f V f
I didn't understand how one can assume the sphere would go into rolling motion right after its first bounce.
Those who have the doubt how I have assumed friction to be sufficient,you can derive the expression for fricional impulse and check it is less than the maximum possible friction.
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can u do it plz
wat if slipping took place during contact with ground??\
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That is what I wanted to say.If the frictional impulse required
for no slipling is more than the maximum frictional impulse,than sliping would take place with the ground.
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@Ronak Agarwal – But it can also be that the friction is not sufficient to start pure rolling.?
Ronak u have a great problem solving capability, keep it up. What is your daily routine ,how long u study.
I'm not very good at rotational motion - how does one arrive at the momentum-impulse equations? Thanks!
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One should approach those when they see that collision is taking place
Silly me... got correct at the 3rd attempt
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Hi Bro. See my profile. There 3rd or 4th question from the top is your related to collision and spring. There the friction required for pure rolling is coming out to be less than the maximum. But I am getting answer when I take the maximum value of frictional impulse. Please check.
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Distance travelled by particle before first bounce R 1 = g v 2 s i n ( 2 θ ) = 1 0 s i n ( 2 θ )
As the ball bounces for the first time it is easy to note that the point of contact of the ball is tending to go backward hence friction will be forward direction.
v y ( i n i t i a l ) = − 1 0 sin θ j
Since coefficient of restitution is 0 . 5 hence v y ( f i n a l ) = 5 sin θ j
We say let impulse due to friction be f
If we assume friction to be sufficient then :
ω f i n a l R = v x ( f i n a l ) ) (i)
Writing momentum-impulse equations:
f = m ( v x ( f i n a l ) − 1 0 c o s θ ) (ii)
f R = 5 2 m R 2 ( 3 − ω f i n a l ) (iii)
Solving v x ( f i n a l ) = ( 5 0 cos θ + 6 R ) / 7
Since R = 5 , v x ( f i n a l ) = ( 5 0 cos θ + 3 0 ) / 7
Finally distance between point of first bounce to second bounce is :
R 2 = g 2 v y ( f i n a l ) v x ( f i n a l ) = g 1 0 s i n θ ( 7 5 0 c o s θ + 3 0 ) = ( 2 5 s i n 2 θ + 3 0 s i n θ ) / 7
Hence D = R 1 + R 2 = 1 0 s i n 2 θ + 7 2 5 s i n 2 θ + 3 0 s i n θ = 7 9 5 s i n 2 θ + 3 0 s i n θ .
Now to maximise this we differentiate D w.r.t θ and equate it to 0
⟹ 1 9 0 c o s 2 θ + 3 0 c o s θ = 0
⇒ 3 8 c o s 2 θ + 3 c o s θ − 1 9 = 0
S o l v i n g c o s θ = 7 6 ( 2 8 9 7 − 3 )
Hence a = 2 8 9 7 , b = 3 , c = 7 6
We get a + b + c = 2 9 7 6
Sorry for this very long solution guys!