Linear and angular momentum problem: Ball hitting a rod

AI Thread Summary
The discussion centers on a physics problem involving a ball colliding with a pivoting rod, focusing on the conservation of linear and angular momentum. Participants express confusion about how to combine linear and angular momentum equations, especially when the rod is free to both rotate and translate. It is clarified that both types of momentum can be treated separately, and equations for each can be combined mathematically. The importance of specifying the point of reference for angular momentum calculations is emphasized, as it affects the results. Ultimately, the conversation leads to the realization that specific relationships between the masses and the collision dynamics are crucial for solving the problem accurately.
barryj
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Homework Statement
Ball of mass mb and velocity vb hits rod of length L , Rod pivots about the center. What is the angular momentum aafter impact?
Relevant Equations
I = 1/12 (mR^2)
I = mR^2
Homework Statement:: Ball of mass mb and velocity vb hits rod of length L , Rod pivots about the center. What is the angular momentum aafter impact?
Homework Equations:: I = 1/12 (mR^2)
I = mR^2

See the attached figure. I understand the concept of linear and angular momentum separately but I am confused as to how to use both at the same time. In the attached diagram ball B hits a rod that pivots in the center. In this case we have a classic case of conservation of angular momentum. However, if the rod is free to move, i.e. not connected at the center to the pivot, then the rod would move horizontally as well as rotating. I am having trouble finding an explanation as to how to add the linear momentum to the equation. Are they handled separately or can I have one equation for the angular part and another for the linear part?

I know that initially I would have a linear momentum of the ball being Mb X Vb. Would this be equal to the Mr X Vr where Vr is the linear velocity of the center of mass?
 

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barryj said:
Homework Statement:: Ball of mass mb and velocity vb hits rod of length L , Rod pivots about the center. What is the angular momentum aafter impact?
Homework Equations:: I = 1/12 (mR^2)
I = mR^2

Homework Statement:: Ball of mass mb and velocity vb hits rod of length L , Rod pivots about the center. What is the angular momentum aafter impact?
Homework Equations:: I = 1/12 (mR^2)
I = mR^2

See the attached figure. I understand the concept of linear and angular momentum separately but I am confused as to how to use both at the same time. In the attached diagram ball B hits a rod that pivots in the center. In this case we have a classic case of conservation of angular momentum. However, if the rod is free to move, i.e. not connected at the center to the pivot, then the rod would move horizontally as well as rotating. I am having trouble finding an explanation as to how to add the linear momentum to the equation. Are they handled separately or can I have one equation for the angular part and another for the linear part?

I know that initially I would have a linear momentum of the ball being Mb X Vb. Would this be equal to the Mr X Vr where Vr is the linear velocity of the center of mass?

Both linear and angular momentum are conserved. Equations are equations and if they include common variables they can be combined in any way that is mathematically valid.

PS remember that angular momentum is defined relative to a given point. So, you are also free to choose the point about which you measure angular momentum of the system.
 
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barryj said:
Homework Statement:: Ball of mass mb and velocity vb hits rod of length L , Rod pivots about the center. What is the angular momentum aafter impact?
Homework Equations:: I = 1/12 (mR^2)
I = mR^2

I don't understand your equation (1). Can you explain that? Why are those two quantities equal?
 
@PeroK has answered your main question, but in solving the actual problem you seem to have forgotten about what happens to the ball afterwards. More information is needed, e.g. it sticks to the rod, or bounces elastically, or happens to come to rest, etc.
 
Referring to my attached sketch, if the ball strikes the free rod at the center of mass, then there would be no rotation only a linear translation then I could say that mb X vb = mr X vr. Would this be a good equation if the ball stikes the rod off center?

I just realized that the initial angular momentum is incorrect because the center of toation was taken from the end of the rod not the center.
 
Oh, I forgot. this is an elastic collision and the ball remains stationary after the collision.
 
barryj said:
Oh, I forgot. this is an elastic collision and the ball remains stationary after the collision.
Ok. But if you take the same set up (rod length, masses) and just compare with and without pivot then the ball will not end up stationary in both. (I think.)
 
I think that whether or not the ball remains stationary might depend on the initial velocity. But my biggest confusion is how to work with both linear and angular momentum when the rod is free to rotate and translate.
 
barryj said:
I think that whether or not the ball remains stationary might depend on the initial velocity. But my biggest confusion is how to work with both linear and angular momentum when the rod is free to rotate and translate.

It can't depend on the initial velocity. It could depend on ##D##. But, that's not really relevant.

You are okay with one equation at a time, but not with two? What do you do when both linear momentum and linear KE are conserved? Those are two different equations.

PS how do you find the total linear momentum of a rigid body?
 
  • #10
My understanding is that in an elastic collision, both KE and Momentum are conserved. I don't see how this answers my basic question above. I start with a ball of mass mb moving at a velocity of vb that hits a free rod. The rod then starts rotating and translating. How are these two effects put together?
 
  • #11
barryj said:
I start with a ball of mass mb moving at a velocity of vb that hits a free rod. The rod then starts rotating and translating. How are these two effects put together?
Just write down the conservation equations independently, as you did.
 
  • #12
Could I say...

KE of ball before impact = (linear)KE of the center of mass of the rod + the rotational KE of the rod?

You could also think of the ball as having rotational momentum, or could you, about what axis? so could you think of the ball as initially having some rotational KE? You can see why I am confused.
 
  • #13
barryj said:
Could I say...

KE of ball before impact = (linear)KE of the center of mass of the rod + the rotational KE of the rod?

That's correct.

barryj said:
You could also think of the ball as having rotational momentum, or could you, about what axis? so could you think of the ball as initially having some rotational KE? You can see why I am confused.

The ball has no rotational KE.
 
  • #14
barryj said:
Could I say...

KE of ball before impact = (linear)KE of the center of mass of the rod + the rotational KE of the rod?

You could also think of the ball as having rotational momentum, or could you, about what axis? so could you think of the ball as initially having some rotational KE? You can see why I am confused.
The ball has some initial KE. The equations do not care whether it is "rotational", "linear" or something else. The ball likely has some initial angular momentum. How much will depend on what axis of rotation you choose.

"Rotational kinetic energy" as such need not enter in.
 
  • #15
OK, the ball has initial KE of 1/2 Mb*Vb^2
After impact there is both rotational and linear KE, yes/no?
So could I write one equation equating the initial KE of the ball = Rotational KE of the rod plus the Linear KE of the rod? something like..(1/2)Mb*Vb^2 = (1/2) Ib*wb^2 + (1/2)Mrod*Vrod^2
 
  • #16
barryj said:
OK, the ball has initial KE of 1/2 Mb*Vb^2
After impact there is both rotational and linear KE, yes/no?
So could I write one equation equating the initial KE of the ball = Rotational KE of the rod plus the Linear KE of the rod? something like..(1/2)Mb*Vb^2 = (1/2) Ib*wb^2 + (1/2)Mrod*Vrod^2

That's definitely your first equation. There are two more needed. One for linear momentum; and one for angular momentum about a point of your choice.
 
  • #17
Then for linear momentum I would say that
Mball*Velocityball = Massrod * Velocityrod since mass1 is stationary after impact
take center of rod as axis of rotation then
mD^2 * Velocityball/D = (1/12)Massrod * D^2 *Omegarod

Maybe I should learn LaText or post a new set of equations.
 
  • #18
barryj said:
Then for linear momentum I would say that
Mball*Velocityball = Massrod * Velocityrod since mass1 is stationary after impact
take center of rod as axis of rotation then
mD^2 * Velocityball/D = (1/12)Massrod * D^2 *Omegarod

Maybe I should learn LaText or post a new set of equations.

The linear equation looks right.

The AM equation is not right. You seem to be taking the AM of the ball and the rod about different points: the ball relative to the top of the rod and the rod about its COM. Those are different points.

To be clear: you must specify the point about which you are measuring the AM of the system.
 
  • #19
Yes, the AM of the ball around the COM should be m(D/2)^2 * Vball/(D/2)
So, I am going to have three equations to work with, yes?

I think I will take a break, get my thoughts together and get back in a bit.
 
  • #20
barryj said:
Yes, the AM of the ball around the COM should be m(D/2)^2 * Vball/(D/2)
So, I am going to have three equations to work with, yes?

I think I will take a break, get my thoughts together and get back in a bit.

I don't understand ##D/2##. It would be simpler to introduce, ##d = D - L/2##, which is the offset from the COM.

I also don't understand the square term. The AM of a point mass is simply ##mvd## in this context.
 
  • #21
I of the ball is mR^2 AM = I*Omega

You are correct. I have the d confused. I need to take a break and redraw my diagram and get my equations correct. Don't forget me as I shall return
 
  • #22
I have attached an updated diagram with equations.
I think these equations agree with what we have been discussing.
I will now have to manipulate them to get the results I want.
At this point, I have forgotten what I am looking for :-)
 

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  • #23
Just for fun I assigned some values to see what I would get.
Mr = 1 kg, Mb = .1 kg, L = 1m, D = 0.4m
Vb = 10 m/sec

I calculagte Ib == mr^2 = (.1)(.4)^2 = 0.016
I calculatge Ir = (1/12)mL2 = (1/12)(1)(1)^2 = .0833

Using eq 2 I get Vr = 1
Using Eq 3 I get omega(r) = 4.8

If I put these into the KE equation, #1, I get 0.7 not close to 5 as I expected since (1/2)(.1)(10)^2 = 5.

Hmmmmmmm...
 
  • #24
barryj said:
I have attached an updated diagram with equations.
I think these equations agree with what we have been discussing.
I will now have to manipulate them to get the results I want.
At this point, I have forgotten what I am looking for :-)
A couple of errors in there, but later fixed up, so maybe transcription errors.
In the second KE equation you start with 1/12 when you mean 1/2.
In the first angular momentum equation you have the angular velocities squared.
 
  • #25
You are totally correct on both accounts.
 
  • #26
barryj said:
You are totally correct on both accounts.
Does it change your results in post #23?
 
  • #27
No it didn"t
 
  • #28
barryj said:
No it didn"t
You have chosen that it is an elastic collision and the ball comes to rest. That will only happen with the right relationship between the masses, but you have plugged in arbitrary masses.
Let the ball's mass be unknown. With the resulting movement of the rod, that gives you three unknowns in total. Conservation of energy, linear momentum and angular momentum gives you three equations. Solve.
 
  • #29
barryj said:
Just for fun I assigned some values to see what I would get.
Mr = 1 kg, Mb = .1 kg, L = 1m, D = 0.4m
Vb = 10 m/sec

I calculagte Ib == mr^2 = (.1)(.4)^2 = 0.016
I calculatge Ir = (1/12)mL2 = (1/12)(1)(1)^2 = .0833

Using eq 2 I get Vr = 1
Using Eq 3 I get omega(r) = 4.8

If I put these into the KE equation, #1, I get 0.7 not close to 5 as I expected since (1/2)(.1)(10)^2 = 5.

Hmmmmmmm...

It turns out that one constraint for a solution to this problem is that ##M_b \le M_r \le 4 M_b##.

Also, depending on the ratio ##M_r/M_b##, the ball must hit the rod at a specific offset ##d##. For example, if ##M_b = M_r##, then ##d = 0## and you have the (hopefully familiar) case of an equal mass elastic collision.

There can't be a solution for all variables. In fact, the ball can only stop when there is a strict relationship between ##M_b, M_r, d## and ##L##.

The one truly independent variable is the impact velocity ##v_b##.
 
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  • #30
Given that my assumed variables will not result in a stationary ball after inmpact I assume we can still solve this problem for Vr and Or after the collision. I am using O for (omega)

Using the linear momentum equation I get (0.1)(10 = (a)(Vr) so Vr = 1

Using the angular momentum equation (0.16)(10/0.4) = (.0833)Or so Or = 4.8

If we calculate the KE after the equation it is (.5))(1)(1)^2 + (.5)(.0833)(4.8)^2 = 1.45J
The KE of the ball before the collision is (.5)(.1)(10)^2 = 5J

Clearly thee is still some KE in the ball after the collision so I assume that with these variables, the ball does not come to rest after the collision. Is this correct? If so, then we can assume that the equations are correct and that the initial assumption that the ball comes to rest is wrong. I am learning a lot from this exchange.
 
  • #31
"It turns out that one constraint for a solution to this problem is that Mb≤Mr≤4Mb. "
I don't understand why this is so at this time but I will continue to study this problem.
 
  • #32
barryj said:
Given that my assumed variables will not result in a stationary ball after inmpact I assume we can still solve this problem for Vr and Or after the collision. I am using O for (omega)

Using the linear momentum equation I get (0.1)(10 = (a)(Vr) so Vr = 1

Using the angular momentum equation (0.16)(10/0.4) = (.0833)Or so Or = 4.8

If we calculate the KE after the equation it is (.5))(1)(1)^2 + (.5)(.0833)(4.8)^2 = 1.45J
The KE of the ball before the collision is (.5)(.1)(10)^2 = 5J

Clearly thee is still some KE in the ball after the collision so I assume that with these variables, the ball does not come to rest after the collision. Is this correct? If so, then we can assume that the equations are correct and that the initial assumption that the ball comes to rest is wrong. I am learning a lot from this exchange.
Not quite. The problem is that, given the assumptions, you must find the angular velocity of the rod. In solving the problem you may find constraints between the various quantities.

Like the one I found for the masses.

You have to work algebraically I'm afraid!
 
  • #33
Well, given the initial masses and velocities it seems to me that I can use the conservation of angular momentum and conservation of linear momentum to fine Vr and Or. Isn't Or = 4.8?

I did some algebra and if the equations are correct why are my results of Vr and Or not correct?
 
  • #34
barryj said:
Well, given the initial masses and velocities it seems to me that I can use the conservation of angular momentum and conservation of linear momentum to fine Vr and Or. Isn't Or = 4.8?

I did some algebra and if the equations are correct why are my results of Vr and Or not correct?
What result? You're supposed to get am expression for ##\omega## in terms of the other variables.
 
  • #35
I am getting confused.

Assuming that the parameters I selected are OK and that my equation for angular momentum is correct then..

IbOb = IrOr (I am using O for Omega)
I calculated that...
Ib = Mb*Db^2 = (.1)(.4)^2 = 0.016
Ob = Vb/Db = 10/.4 = 25
Ir = (1/12)MrL^2 = (1/12)(1)(1)=.08333
so
Or = IbOb/Ir = (0.016)(25)/(0.08333) = 4.8

Recall at this time I am using the parameters I established, i.e.
Mb = .1 , Vb = 10, Mr = 1, and Db = .4
 
  • #36
barryj said:
I am getting confused.

Assuming that the parameters I selected are OK and that my equation for angular momentum is correct then..

IbOb = IrOr (I am using O for Omega)
I calculated that...
Ib = Mb*Db^2 = (.1)(.4)^2 = 0.016
Ob = Vb/Db = 10/.4 = 25
Ir = (1/12)MrL^2 = (1/12)(1)(1)=.08333
so
Or = IbOb/Ir = (0.016)(25)/(0.08333) = 4.8

Recall at this time I am using the parameters I established, i.e.
Mb = .1 , Vb = 10, Mr = 1, and Db = .4

##KE_i = \frac 1 2 M_b v_b^2 = 5J##

##KE_f = \frac 1 2 I_r w^2 = 9.6J##

Your methods are unsound!

You need to do this properly or not at all.
 
  • #37
I am trying to do this properly. I am not understanding the basic concept here. Let's forget about my initial statement that the ball is stationary after the collision, OK?

Now, are my equations correct, if not then they must be fixed.

I agree that "KEi=12Mbv2b=5J "
I don't see where you get "KEf=12Irw2=9.6J"

However, I am not considering KE at this point, just conservation of linear and angular momentum.

I think my parameters are realistic so I should be able to calculate the Or after the collision with the equations, if they are correct.Yes?
 
  • #38
barryj said:
I am trying to do this properly. I am not understanding the basic concept here. Let's forget about my initial statement that the ball is stationary after the collision, OK?

Now, are my equations correct, if not then they must be fixed.

I agree that "KEi=12Mbv2b=5J "
I don't see where you get "KEf=12Irw2=9.6J"

However, I am not considering KE at this point, just conservation of linear and angular momentum.

I think my parameters are realistic so I should be able to calculate the Or after the collision with the equations, if they are correct.Yes?

I'm not sure what you've understood and what you haven't. We've told you that you can't just plug in any old masses here and get a consistent solution.

Your parameters are not valid for this problem, because they don't support the ball having zero velocity after the collision. A ball that light would rebound. I must have told you that several times already.

I don't understand why you are plugging numbers in rather than solving the problem properly - using the algebraic variables. It's not that hard, surely.

A few posts back you seemed to be getting close to having all the equations, but you've drifted off into a numerical approach that leads nowhere.

Your lack of Latex makes things hard to read as well, it must be said.
 
  • #39
barryj said:
IbOb = IrOr (I am using O for Omega)
Let us attack just this equation for the moment. It asserts that ##I_b## (the moment of inertia of the ball just prior to impact) times ##\omega_b## (the initial angular velocity of the ball just prior to impact) is equal to ##I_r## (the moment of inertia of the rod) times ##\omega_r## (the angular velocity of the rod just after impact).$$I_b \omega_b = I_r \omega_r$$
That would follow from conservation of angular momentum but only on the assumption that the ball stops dead after the impact. I thought that we were solving three simultaneous equations and discovering whether the ball would or would not stop based on the results obtained.

I am not entirely comfortable describing the angular momentum of the ball as ##I_b \omega_b## since it is not an object rotating rigidly about the reference axis. Instead, I would use ##\vec{r_b} \times \vec{p_b}## where ##\vec{r_b}## is the displacement of the ball from the reference axis, and ##\vec{p_b}## is its momentum and ##\times## denotes the vector cross product.

The concern with using ##I_b## to denote the moment of inertia of the ball is that it is not constant.
 
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  • #40
Ah Ha, I see some light. As briggs said, my angular momentum equation is valid only if the ball stops and I keep saying let's not have this condition and this makes my equation wrong. I must learn LaTex also!
 
  • #41
barryj said:
Ah Ha, I see some light. As briggs said, my angular momentum equation is valid only if the ball stops and I keep saying let's not have this condition and this makes my equation wrong. I must learn LaTex also!
You can also use the clicky thing that looks like ##\sqrt{x}## above the editting panel. That will give you to access to symbols such as "ω".

I cannot find superscripts and subscripts there. But you can insert those using bbcode tags such as ω[sub]b[/sub]. Which renders as ωb
 
  • #42
barryj said:
Ah Ha, I see some light. As briggs said, my angular momentum equation is valid only if the ball stops and I keep saying let's not have this condition and this makes my equation wrong. I must learn LaTex also!

You need to decide whether the ball has a known velocity of zero after the collision; or a to-be-determined velocity.

Having a zero velocity simplifies the equation, but puts constraints on the variables.

It's your problem, so which is it?
 
  • #43
PeroK said:
Having a zero velocity simplifies the equation, but puts constraints on the variables.
If I understand correctly, the constraint on the variables can be seen as arising from the idea that the collision should not result in a net increase in kinetic energy. One can erase that constraint by placing a tiny blasting cap of exactly the right size on the rod at the point of collision.
 
  • #44
Lets start out with zero just so I can get something that is correct.
If the ball stops then the linear KE of the rod + angular KE of the rod must be 5.
This would give a relationship between ωr and Vr yes?
 
  • #45
barryj said:
Lets start out with zero just so I can get something that is correct.
If the ball stops then the linear KE of the rod + angular KE of the rod must be 5.
This would give a relationship between ωr and Vr yes?
If the ball stops and you still insist on conserving kinetic energy, that gives you too many equations. They will likely be inconsistent. The obvious suggestion is to drop the requirement that kinetic energy be conserved and go with conservation of linear and angular momentum only.
 
  • #46
If we don't insist on conserving KE then we can eliminate equation 1, yes and only use the conservation of linear momentuim and conservation of angular momentum equations, yes?
 
  • #47
jbriggs444 said:
If the ball stops and you still insist on conserving kinetic energy, that gives you too many equations. They will likely be inconsistent. The obvious suggestion is to drop the requirement that kinetic energy be conserved and go with conservation of linear and angular momentum only.

The problem as originally stated was quite nice I thought. You just have to assume that the ball hit the rod at just the right spot.
 
  • #48
barryj said:
If we don't insist on conserving KE then we can eliminate equation 1, yes and only use the conservation of linear momentuim and conservation of angular momentum equations, yes?
Yes. The angular momentum equation I'd suggested above would be$$\vec{r_b} \times \vec{p_b} = I_r\omega_r$$ Can you produce for us the linear momentum equation in a similar format before proceeding to solve? [It is easier to follow algebra than numeric computations]
 
  • #49
mbvb = mrvr
 
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  • #50
Does the "thumbs up" mean I am correct? If so then we can solve for vr given the other inputs, yes?
 
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