Collision, angular momentum and energy

In summary: Yes, but in this case it is rather surprising that they reversed the sign convention for vf. Which way the ball goes after collision depends on how its mass compares with M/4, so it would have been far more natural to have kept the positive direction the same.
  • #1
LCSphysicist
646
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Homework Statement
A plank of length 2l and mass M lies on a frictionless plane.
A ball of mass m a nd speed Vo strikes its end as shown. Find the final
velocity of the ball, vf, assuming that mechanical energy is conserved
and that vf is along the original line of motion
Relevant Equations
All below.
IS my solution right? Comparing with the other solutions, the answer just exchange the signals, i don't know why,
1592419362789.png
THats what ifound.

And here is the three equations:
{i use the point which occurs the collision}
Lo = Lf >>

0 = Iw + M*Vcm(block)

Eg = ct>

mvo² = mvf² + MVcm² + Iw²

I = ml²/3

P = cte

mvo = mvf + MVcm

I just assumed that xyz dextrogira, i thought that putting by this way, the math would implies the correct values, that is, we would find w<0, and the others values. Apparently i am wrong in something, where?
 
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  • #3
wrobel said:
a picture would be good
1592426809272.png
 
  • #4
LCSphysicist said:
Apparently i am wrong in something, where?
I get the same answer you do.
Please post the book answer exactly as given.
 
  • #5
haruspex said:
I get the same answer you do.
Please post the book answer exactly as given.
1592428685088.png

As you can see, in our answer the numerator has signals exchanged.
 
  • #6
LCSphysicist said:
As you can see, in our answer the numerator has signals exchanged.
You have a different sign convention for ##v_0## and ##v_f##. What's up with that? If you are trying to explain a sign error in the answer, the very first place to look is at the sign conventions.
 
  • #7
jbriggs444 said:
You have a different sign convention for ##v_0## and ##v_f##. What's up with that? If you are trying to explain a sign error in the answer, the very first place to look is at the sign conventions.
Yes, but in this case it is rather surprising that they reversed the sign convention for vf. Which way the ball goes after collision depends on how its mass compares with M/4, so it would have been far more natural to have kept the positive direction the same.
 
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  • #8
Sorry for offtop, perhaps somebody will be interested.
I remember a much funny problem of the same type. A plank of mass ##m## and of length ##2l## lies on a smooth horizontal table as it is shown at the picture. Here ##S## is the center of mass. A bullet punches through the plank (dotted arrow) and loses linear momentum ##p##. Find the angular velocity of the plank right after the punch. It is not so trivial as it looks from the first glance.

Screenshot from 2020-06-18 10-16-48.png
 
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  • #9
wrobel said:
Sorry for offtop, perhaps somebody will be interested.
I remember a much funny problem of the same type. A plank of mass ##m## and of length ##2l## lies on a smooth horizontal table as it is shown at the picture. Here ##S## is the center of mass. A bullet punches through the plank (dotted arrow) and loses linear momentum ##p##. Find the angular velocity of the plank right after the punch. It is not so trivial as it looks from the first glance.

View attachment 264805
Depends whether b>l/3, right?
 
  • #10
haruspex said:
Depends whether b>l/3, right?
yes :)
 
  • #11
haruspex said:
Yes, but in this case it is rather surprising that they reversed the sign convention for vf. Which way the ball goes after collision depends on how its mass compares with M/4, so it would have been far more natural to have kept the positive direction the same.
1. Why do they reverse the sign convention for vf when it is a velocity with a direction.
2. Doesn't it say that " assuming that mechanical energy is conserved
and that vf is along the original line of motion "?
3. Are vector arrows meant to be drawn on vector quantities?
4. If we just draw vector arrows on the equation that OP supplies, is there any need for changing the sign now?
 
  • #12
wrobel said:
Sorry for offtop, perhaps somebody will be interested.
I remember a much funny problem of the same type. A plank of mass ##m## and of length ##2l## lies on a smooth horizontal table as it is shown at the picture. Here ##S## is the center of mass. A bullet punches through the plank (dotted arrow) and loses linear momentum ##p##. Find the angular velocity of the plank right after the punch. It is not so trivial as it looks from the first glance.

View attachment 264805

Help, I want a solution.

haruspex said:
Depends whether b>l/3, right?

?
 
  • #13
aspodkfpo said:
Why do they reverse the sign convention for vf when it is a velocity with a direction.
I assume whoever wrote that solution considered rebound as the expected behaviour, but there is no good reason.
aspodkfpo said:
Doesn't it say that " assuming that mechanical energy is conserved
and that vf is along the original line of motion "?
Yes, but being along the same line is not quite the same as in the same direction.
aspodkfpo said:
Are vector arrows meant to be drawn on vector quantities?
Yes, but since the velocities are all in the same line there's no problem working with the scalar coefficient of the velocity in the chosen unit vector direction.
aspodkfpo said:
If we just draw vector arrows on the equation that OP supplies, is there any need for changing the sign now?
Not sure what you are asking.
If you mean ##\vec {v_f}=\frac{1-\frac{4m}M}{1+\frac{4m}M}\vec{v_0}##, that would simply be wrong.
 
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  • #14
aspodkfpo said:
1. Why do they reverse the sign convention for vf when it is a velocity with a direction.
You are asking us to guess about a decision made by someone else. I do not agree with that decision, but I can try to defend it anyway.

Often, one will try to choose a sign convention so that all of the numbers in the problem will be positive. So if one expects the initial velocity to be toward the right and the final velocity toward the left then one might want to choose a sign convention so that positive values of ##v_0## are rightward while positive values of ##v_f## are leftward.

Of course, this means that when those values are combined in an equation, the difference in sign must be accounted for. So instead of writing down a conservation of linear momentum equation like$$mv_0 + Mv_0 = mv_f + MV_f$$we have to write$$mv_0 + MV_0 = -mv_f + MV_f$$.

If we do not know, when initially approaching the problem, what direction the final velocity is going to have, it is more sensible to use the same sign convention (or, more generally, the same coordinate axes) for everything. If that means that the numeric velocity comes out negative, so be it.
2. Doesn't it say that " assuming that mechanical energy is conserved
and that vf is along the original line of motion "?
Yes. But lines extend in two directions. That statement leaves the sign convention one will use to report the final velocity undefined.
3. Are vector arrows meant to be drawn on vector quantities?
Arrows. Or boldface. When working in one dimension, it can be somewhat pointless.
4. If we just draw vector arrows on the equation that OP supplies, is there any need for changing the sign now?
One still has to pay attention to sign conventions. Sticking a graphic enhancement on the equations does not change that.

When dealing with vectors, the sign convention amounts to a choice of a set of basis vectors for the vector space. Those fancy words mean picking a direction for your coordinate axes. If you have vector ##\vec{v_0}## expressed using a coordinate system where positive x points rightward and vector ##\vec{v_f}## using a coordinate system where positive x points leftward then you will have to include a minus sign in your equations when referring to x-coordinates using the other coordinate system. That minus sign amounts to a coordinate system transformation so that all of the coordinate values in an equation are using the same system.
 
Last edited:
  • #15
aspodkfpo said:
Help, I want a solution.
?
Don't worry about wrobel's post. It is an entirely different, but quite interesting, question.
 
  • #16
haruspex said:
I assume whoever wrote that solution considered rebound as the expected behaviour, but there is no good reason.

Yes, but being along the same line is not quite the same as in the same direction.

Yes, but since the velocities are all in the same line there's no problem working with the scalar coefficient of the velocity in the chosen unit vector direction.

Not sure what you are asking.
If you mean ##\vec {v_f}=\frac{1-\frac{4m}M}{1+\frac{4m}M}\vec{v_0}##, that would simply be wrong.
jbriggs444 said:
You are asking us to guess about a decision made by someone else. I do not agree with that decision, but I can try to defend it anyway.

Often, one will try to choose a sign convention so that all of the numbers in the problem will be positive. So if one expects the initial velocity to be toward the right and the final velocity toward the left then one might want to choose a sign convention so that positive values of ##v_0## are rightward while positive values of ##v_f## are leftward.

Of course, this means that when those values are combined in an equation, the difference in sign must be accounted for. So instead of writing down a conservation of linear momentum equation like$$mv_0 + Mv_0 = mv_f + MV_f$$we have to write$$mv_0 + MV_0 = -mv_f + MV_f$$.

If we do not know, when initially approaching the problem, what direction the final velocity is going to have, it is more sensible to use the same sign convention (or, more generally, the same coordinate axes) for everything. If that means that the numeric velocity comes out negative, so be it.

Yes. But lines extend in two directions. That statement leaves the sign convention one will use to report the final velocity undefined.

Arrows. Or boldface. When working in one dimension, it can be somewhat pointless.

One still has to pay attention to sign conventions. Sticking a graphic enhancement on the equations does not change that.

When dealing with vectors, the sign convention amounts to a choice of a set of basis vectors for the vector space. Those fancy words mean picking a direction for your coordinate axes. If you have vector ##\vec{v_0}## expressed using a coordinate system where positive x points rightward and vector ##\vec{v_f}## using a coordinate system where positive x points leftward then you will have to include a minus sign in your equations when referring to x-coordinates using the other coordinate system. That minus sign amounts to a coordinate system transformation so that all of the coordinate values in an equation are using the same system.

For Question 4, what I mean is doesn't V with an arrow on top indicate both magnitude and direction along the defined axis. So from the start when we do V0 and Vf, we simply ignore all signs and write all of them as positive, rather than using the scalar coefficient?

haruspex said:
Don't worry about wrobel's post. It is an entirely different, but quite interesting, question.

Don't care if it's different, please show solution.
 
  • #17
aspodkfpo said:
Don't care if it's different, please show solution.
The trick in the question is you have to consider two possibilities. If the impact is sufficiently close to the rod's mass centre, the rod will rotate relatively slowly, so the end that was on the table will rise off the table. If the impact is sufficiently far from the rod's mass centre, the rod's rotation could be so fast that the end at A would move down into the table; to prevent that there must be a normal impulse at A.
 
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  • #18
aspodkfpo said:
For Question 4, what I mean is doesn't V with an arrow on top indicate both magnitude and direction along the defined axis. So from the start when we do V0 and Vf, we simply ignore all signs and write all of them as positive, rather than using the scalar coefficient?
Yes, hence my answer in post #13.
 
  • #19
haruspex said:
Yes, hence my answer in post #13.
You say that would be simply wrong? Why would it be wrong?
 
  • #20
aspodkfpo said:
You say that would be simply wrong? Why would it be wrong?
When working in vectors, unless otherwise stated, they should all be in the same coordinate system.
Consider e.g. m tends to zero. That vector equation has ##\vec {v_f}## tending to ##\vec{v_0}## instead of to ##-\vec{v_0}##. When m is very small it should just rebound, hardly disturbing M.
 
  • #21
haruspex said:
When working in vectors, unless otherwise stated, they should all be in the same coordinate system.
Consider e.g. m tends to zero. That vector equation has ##\vec {v_f}## tending to ##\vec{v_0}## instead of to ##-\vec{v_0}##. When m is very small it should just rebound, hardly disturbing M.

?
Vectors are along the same line. Arrow drawn on top indicates that the direction is included.

I am saying that at the very start of working out, we do not take a -vf and a v0 but just take a vf and v0 with an arrow on top.
Then we end with the original answer OP got which was vf (arrow) = (-1+4m/M)/(1+4m/M) v0 (arrow).
We never bother with what happens, but this would be correct since v0 would be in the different direction from vf, and we end with vf = (1-4m/M)/(1+4m/M) v0 if we bother to make it into scalar form.
 
  • #22
aspodkfpo said:
?
Vectors are along the same line. Arrow drawn on top indicates that the direction is included.

I am saying that at the very start of working out, we do not take a -vf and a v0 but just take a vf and v0 with an arrow on top.
Then we end with the original answer OP got which was vf (arrow) = (-1+4m/M)/(1+4m/M) v0 (arrow).
We never bother with what happens, but this would be correct since v0 would be in the different direction from vf, and we end with vf = (1-4m/M)/(1+4m/M) v0 if we bother to make it into scalar form.
We seem to be at cross purposes.
In post #13 I wrote that ##\vec {v_f}=\frac{1-\frac{4m}M}{1+\frac{4m}M}\vec{v_0}## would be wrong.
##\vec {v_f}=\frac{-1+\frac{4m}M}{1+\frac{4m}M}\vec{v_0}## would be correct.
 
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Related to Collision, angular momentum and energy

1. What is a collision in physics?

A collision in physics refers to the interaction between two or more objects where they come into contact with each other and exchange energy and momentum. This can be either an elastic collision, where there is no loss of energy, or an inelastic collision, where some energy is lost in the form of heat or sound.

2. How is angular momentum defined?

Angular momentum is a measure of an object's resistance to changes in its rotational motion. It is defined as the product of an object's moment of inertia and its angular velocity. In simpler terms, it is the amount of rotational motion an object has.

3. What is the conservation of angular momentum?

The conservation of angular momentum states that in the absence of external torques, the total angular momentum of a system remains constant. This means that the total amount of rotational motion in a system will not change unless acted upon by an external force.

4. How does energy play a role in collisions?

In a collision, energy is transferred between objects. In an elastic collision, the total kinetic energy of the system remains constant before and after the collision. In an inelastic collision, some of the kinetic energy is converted into other forms, such as heat or sound.

5. What is the relationship between energy and momentum in collisions?

In a collision, the total momentum of the system is conserved, meaning that the sum of the momenta of all objects before the collision is equal to the sum of the momenta after the collision. The total energy of the system, however, may change depending on the type of collision. In an elastic collision, both momentum and kinetic energy are conserved, while in an inelastic collision, only momentum is conserved.

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