Apparent paradox with angular and linear motion

In summary: The amount of impulse is proportional to the mass of the object and the distance between the objects. If the objects are at an offset, the impulse is larger.
  • #1
cybie
6
0
A friend raised an observation which I thought would be easy to explain. But it seem I have a gap in my physics knowledge...

An object (rigidbody) is stationary in zero gravity empty space. In the first situation we apply an impulse to its COG and its linear momentum changes, and no angular momentum change. Correct?

In the second situation, same initial condition, but the same impulse is apply off center, inducing a change in angular velocity, as well as the same change in linear momentum as in the first situation.

In the first situation, the impulse resulted in the object having an linear kinetic energy. In the second situation, the impulse caused the object to have the same linear kinetic energy, but also an additional rotational kinetic energy.

Why aren't the total kinetic energy after the impulse the same in both situation?

Thanks for answering.
 
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  • #2
Energy must be conserved, so the energy from the impulse is divided between linear and angular kinetic energy. The ratio of the division depends on the magnitude of the components of the impulse along the directions parallel and perpendicular to the direction from the point of impact to the body's centre of mass, and also the mass and moment of inertia about the axis of induced rotation.
 
  • #3
One way to understand this is to realize that the work performed by this impulse is proportional to the distance moved by the point of application of the force.

If you apply the impulse at the center of mass, the only resulting motion is linear.

If you apply the impulse off-center, there is both linear motion and rotational motion. The point at which the force is applied moves further under application of the same force.

So even though the force * time might be the same for the two situations, force * distance can be different.
 
  • #4
>So even though the force * time might be the same for the two situations, force * distance can be different.

I want narrow to just impulse and not force (I am assuming it is theoretically possible), because I don't want to deal with how the application position of the force change over time.

In all the text I read about change in momentum, I didn't find one which change in linear momentum is a function of 'offset' from the center where the impulse is apply. That why I assume the change in momentum is just a function of mass and the magnitude of the impulse.

If that's the case, then by offsetting the impulse, I will get same change in linear momentum plus an addition angular momentum, resulting in a bigger total kinetic energy. So that doesn't sound right.

What did I miss?
 
  • #5
cybie said:
In all the text I read about change in momentum, I didn't find one which change in linear momentum is a function of 'offset' from the center where the impulse is apply. That why I assume the change in momentum is just a function of mass and the magnitude of the impulse.
That is correct.

cybie said:
If that's the case, then by offsetting the impulse, I will get same change in linear momentum plus an addition angular momentum, resulting in a bigger total kinetic energy.
That is also correct.

cybie said:
So that doesn't sound right.

What did I miss?
You missed that impulse ≠ energy. The center and offset impulses have the same impulse but different energies. You cannot match both except in special cases (like both on center, or both offcenter by same amount).
 
  • #6
In the second situation, same initial condition, but the same impulse is apply off center, inducing a change in angular velocity, as well as the same change in linear momentum as in the first situation.

The second part of that statement is untrue.
While a body rotaing and moving linerally at the same time can be analyzed for the velocities of certain points by suposition of translation and rotation, the same cannot be said for an inpulse applied off centre to the centre of gravity - ie you do not calculate first the angular momentum as if the impulse was applied off some distance to the CG and then calculate a linear momentum as if the same impulse was at the CG.

If you do think about what you have stated is that
1. Apply impulse off from the CG so that the rigid body acquires an angular momentum.
2. At an oportune moment, apply the same impulse at the CG so that the body acquires a linear momentum.

I will explain it in terms of collisions in regards to conservation of momentum. Note that when two bodies do collide they are acting upon each other with impulse.

You should look up coefficient of restitution, e.
If e = 0 , a collision is non elastic
If e = 1 , a collision is elastic and energy is conserved
For e=0 to e<1, energy is not conserved.

For a linear collision, two bodies with collinear velocities of the CG V1a and V1b with the point of contact will collide and separate with CG velocities V2a and V2b. And one can calculate the coeficient of restitution from the values of velocity.

You may find this surprising, but rigid bodies have the same coeficient of restitution whether the contact is colliner with the CG or off centre. What that means is that the point(s) of contact of the bodies respectively having velocities V1a and V1b before contact will have velocites V2a and V2b after contact. Other parts of the rigid bodies will have different velocities. ( The velocities mentioned here are vectors ).

Note that it follows that the CG of the rigid body(s) when hit off centre cannot have the same V1b or V2b as the point of contact or there would not be any rotaion.
 
  • #7
Thanks for all the replies.

I am still not clear about this.

the same cannot be said for an inpulse applied off centre to the centre of gravity - ie you do not calculate first the angular momentum as if the impulse was applied off some distance to the CG and then calculate a linear momentum as if the same impulse was at the CG.

Then how do you calculate the change in linear and angular momentum due to an off-center impulse?
 
  • #8
I don't think it is very helpful to bring collisions and coefficients of restitution into this. Applying a known impulse to a body doesn't necessarily have anything to do with collisions. It is equally relevant to analysing "steady state" situations like rockets or jet engines.

Dalespam has it right: The kinetic energy is different in the two situations because impulse ≠ energy - they are measured in different units, so they can't be "the same thing".
 
  • #9
cybie said:
I am still not clear about this.
Then how do you calculate the change in linear and angular momentum due to an off-center impulse?

You seem to have done the right things in your OP, but the problem was you didn't believe the answer.

Impulse = change of linear momentum.
Moment of the impulse about the CG = change of angular momentum.
 
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  • #10
Noting that energy does not equal impulse.

But the difficulty I think I am having is the that 1st situation (on center) and 2nd situation (off center), both with the same impulse, give different total kinetic energy. How do I explain that the 2nd case have higher total kinetic energy.

[Adding real life example]
Let me elaborate: Let's say the situation we are talking about is coin flipping. Assuming my thumb is asserting an impulse on the coin. In situation 1 is my thumb impact the coin on-center. 2nd situation my thumb impact the coin off-center. Assuming I use the same amount of energy to flick my thumb, how come the 2nd case resulted in higher total kinetic energy?
 
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  • #11
256bits said:
The second part of that statement is untrue.
This is incorrect, the statement was true. An off-center impulse imparts the same linear momentum as an on-center impulse.
 
  • #12
cybie said:
But the difficulty I think I am having is the that 1st situation (on center) and 2nd situation (off center), both with the same impulse, give different total kinetic energy. How do I explain that the 2nd case have higher total kinetic energy.
You can work it out mathematically by the process jbriggs444 suggested above. Then, if you want to go to an instantaneous impulse you can simply fix the impulse and take the limit as the time goes to 0. You will see that the work done is not the same, and so therefore by the work energy theorem the KE is not the same either.
 
  • #13
Thanks for continuing to answer to help me get my head around this.

I stated that the same amount of energy was use to flick my thumb to impact the coin. It must follow that the kinetic energy of the coin be the same whether I hit it on or off center. If I hit it on center, the linear velocity should be less than the linear velocity if I hit it off center (because now it also has angular momentum). But that seem to contradict the statement that the change in linear momentum does not take into account of where the impulse was apply.
 
  • #14
An on center force and an off center force may have the same impulse, or they may do the same work, not both. If you state as a fact that the work is the same then the off-center impulse must be less.
 
  • #15
Maybe it would help to know that in order to generate the same impulse off center, the point of application of that force will be accelerating faster, resulting in the force being applied at a faster speed over time. Since power = force x speed, a greater amount of power is involved when the same impulse is applied off center.
 
  • #16
cybie said:
In all the text I read about change in momentum, I didn't find one which change in linear momentum is a function of 'offset' from the center where the impulse is apply. That why I assume the change in momentum is just a function of mass and the magnitude of the impulse.

If that's the case, then by offsetting the impulse, I will get same change in linear momentum plus an addition angular momentum, resulting in a bigger total kinetic energy. So that doesn't sound right.

What did I miss?
"So that doesn't sound right."
What you missed is that "sounding right" is not a law of physics.

Law of physics: The impulse is equal to the total change in linear momentum of the system. This is a law of physics.
Statement that sounds right:The impulse determines the total change of kinetic energy of the system.

The "law of physics" is correct. The "statement that sounds right" is incorrect.

The impulse is equal to the change in linear momentum of the system. Therefore,
F_Ext Δt=M_Total ΔV_CM
where "F_Ext" is the average force over the time interval "Δt", "M"_Total is the total mass of the system and "ΔV_CM" is the change in velocity of the center of mass of the system. I couldn't write the vector the vector caps on the force or velocity, but they are there,
You can't determine the total kinetic energy of the system from "F_Ext Δt". As you pointed out, there are other degrees of freedom that are not "linear". The system has angular degrees of freedom, too.
 
  • #17
cybie said:
[Adding real life example]
Let me elaborate: Let's say the situation we are talking about is coin flipping. Assuming my thumb is asserting an impulse on the coin. In situation 1 is my thumb impact the coin on-center. 2nd situation my thumb impact the coin off-center. Assuming I use the same amount of energy to flick my thumb, how come the 2nd case resulted in higher total kinetic energy?

Not a very accurate experiment -- much energy is lost and little measurement is done in that scenario.

If you were able to look very closely, you would see that in order to apply the same impulse in an off-center impact as in an on-center impact, the thumb has to hit harder.

That's because in an off-center impact, the coin rebounds more quickly. This means that the duration of the impact is reduced. And since impulse is the product of force * duration, that means that the force has to be increased in order to impart the same impulse.
 
  • #18
rcgldr said:
Maybe it would help to know that in order to generate the same impulse off center, the point of application of that force will be accelerating faster, resulting in the force being applied at a faster speed over time. Since power = force x speed, a greater amount of power is involved when the same impulse is applied off center.

Thanks rcgldr! I think this is what I am looking. In order to explain the off-center case resulting in greater total kinetic energy, the energy it take to produce the impulse is greater than the on-center case, even though magnitude of both impulse are the same. Hence conservation of energy is not violated. Right?

Thanks
 
  • #19
Try thinking about it this way:

In both cases, the impulse is the same. We agree on this.

But, for the ON CENTER case, your force (or the energy you supply) is only "fighting" linear inertia (that is, the mass).
In the OFF CENTER case, your force (or the energy you supply) is "fighting" both the linear inertia (mass) and the angular inertia (its moment of inertia about the CoG). So, in order for you to supply the same impulse to both cases, you MUST use more energy in the off-center case, since you're "fighting" more inertia, and using more energy is exactly what allows the total KE at the end to be greater because it is rotating.

Thus, impulse= same in both cases, but KE=different.
 
  • #20
rcgldr said:
... in order to generate the same impulse off center, the point of application of that force will be accelerating faster, resulting in the force being applied at a faster speed over time. Since power = force x speed, a greater amount of power is involved when the same impulse is applied off center.

cybie said:
In order to explain the off-center case resulting in greater total kinetic energy ... even though magnitude of both impulse are the same.
You can think of the energy added as power x time or as force x distance, in the first case, the power is greater because of the greater speed, in the second case, the distance is greater because of the greater speed (while the force and time remain the same).

In the off center case, there's less resistance to the force, because the object is free to rotate as well as translate (move linearly), so in order to generate the same force, the acceleration needs to be greater.
 
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  • #21
Just as I said, but thinking in terms of inertia is often easier.
 
  • #22
DaleSpam said:
An on center force and an off center force may have the same impulse, or they may do the same work, not both. If you state as a fact that the work is the same then the off-center impulse must be less.

That was what I was trying to say, but I see you ( and others ) have explained it more distinctly.
 

FAQ: Apparent paradox with angular and linear motion

What is the apparent paradox with angular and linear motion?

The apparent paradox with angular and linear motion is the fact that two objects can have the same linear velocity but different angular velocities, or vice versa. This seems contradictory because we often associate speed and distance with motion, but angular motion is measured in terms of angle and time.

How can two objects have the same linear velocity but different angular velocities?

This is possible because linear velocity is defined as the rate of change of an object's position in a straight line, while angular velocity is defined as the rate of change of an object's angular position. So, two objects can have the same linear velocity if they are moving at the same speed in a straight line, but if one is moving in a circular path, it will also have an angular velocity.

What is the relationship between angular and linear velocity?

The relationship between angular and linear velocity is that they are proportional to each other. This means that if the linear velocity of an object increases, its angular velocity will also increase, and vice versa. This relationship is described by the equation v = rω, where v is linear velocity, r is the radius of the object's circular path, and ω is angular velocity.

How does the direction of motion affect the apparent paradox with angular and linear motion?

The direction of motion does not affect the apparent paradox. Whether an object is moving in a straight line or a circular path, the relationship between angular and linear velocity remains the same. However, the direction of motion can affect other factors such as centrifugal and centripetal forces, which play a role in circular motion.

Can the apparent paradox with angular and linear motion be resolved?

Yes, the apparent paradox can be resolved by understanding the different ways in which we measure and define motion. Linear and angular motion are two distinct types of motion, and they can coexist without contradicting each other. By understanding the relationship between angular and linear velocity, we can resolve the apparent paradox and better understand the complexities of motion.

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