Relative velocity and conservation of linear momentum

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Homework Help Overview

The problem involves a rocket's last stage, which consists of a rocket case and a payload capsule that separate after the release of a clamp. The initial speed of the rocket is given, along with the masses of the two components and their relative speed after separation. The task is to determine the final speeds of both the rocket case and the payload capsule after separation, using principles of conservation of momentum and relative velocity.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the use of conservation of momentum and relative velocity to set up equations for the problem. Some suggest using the center of momentum frame for analysis, while others explore the implications of different assumptions about the direction of velocities.

Discussion Status

There is an ongoing exploration of different approaches to the problem, with some participants providing guidance on how to set up the equations correctly. Multiple interpretations of the problem setup are being examined, particularly regarding the direction of the velocities involved.

Contextual Notes

Participants note the importance of correctly applying the conservation of momentum and the potential impact of sign changes in their calculations. There is a recognition of the need to clarify assumptions about the direction of motion for the components after separation.

Lord Anoobis
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Homework Statement


The last stage of a rocket, which is traveling at a speed of 7600m/s, consists of two parts that are clamped together: a rocket case with a mass of 290.0 kg and a payload capsule with a mass of 150.0kg. When the clamp is released, a compressed spring causes the two parts to separate with a relative speed of 910.0m/s. What are the speeds of
(a) the rocket case and
(b) the payload after they have separated? Assume that all velocities are along the same line.


Homework Equations



m1V1i + m2V2i = m1V1f + m2V2f

Vac = Vpc + Vap
Subscripts being ac=case velocity according to A, pc=relative velocity between case and payload, ap=velocity of payload according to A

The Attempt at a Solution


Howdy folks, I hope I haven't botched the equation writing part, being a newcomer here.

I took the perspective of an observer, A, and used the Galilean transformation for velocity which resulted in

Vac = 910 + Vap

Then with the conservation of momentum:

150Vap + 290Vac = 440(7600), 440kg being the total mass.

Solving for the case's velocity gave an answer of 7910m/s with the correct answer being 8200m/s. I noticed that dividing the relative speed of 910m/s in the same ratio as the masses gives the correct answer. Two attempts at the problem without success so far.
 
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Those simultaneous equations look correct to me. Can you show your work solving them?
 
An important method for dealing with this sort of problem is to treat the interaction in the centre of momentum (COM) frame. Then when you have that figured out, transform the whole thing back to the lab frame.

In the lab frame here, the whole system starts as one "lump" moving at 7600 m/s. The COM frame starts with the whole system as a lump at rest. You should be able to very easily figure out what happens to this system if it starts as one lump at rest and splits as described. Then just add the 7600 m/s back on to get what happens in the lab frame.
 
jbriggs444 said:
Those simultaneous equations look correct to me. Can you show your work solving them?

150VAP + 290VAC = 440(7600)

VAP = (440(7600) - 290VAC)/150

Substituting yields VAC = 910 + (440(7600) - 290VAC)/150

150VAC = 910(150) + 440(7600) - 290VAC

VAC = (910(150) + 440(7600))/440

VAC = 7910m/s
 
Lord Anoobis said:
I took the perspective of an observer, A, and used the Galilean transformation for velocity which resulted in

Vac = 910 + Vap
Try assuming that the payload goes forward and the capsule goes backwards (relatively).
 
DEvens said:
An important method for dealing with this sort of problem is to treat the interaction in the centre of momentum (COM) frame. Then when you have that figured out, transform the whole thing back to the lab frame.

In the lab frame here, the whole system starts as one "lump" moving at 7600 m/s. The COM frame starts with the whole system as a lump at rest. You should be able to very easily figure out what happens to this system if it starts as one lump at rest and splits as described. Then just add the 7600 m/s back on to get what happens in the lab frame.

With this in mind and the fact that the total momentum after the spring action must be zero, I get

290VC = 150VP, ignoring signs for now. This then means that the velocity the spring imparts to each must be 910m/s divided into an opposite ratio, so to speak. Obviously one or the other must then be a negative quantity and adding the 7600m/s yields the correct answer. Am I correct in thinking about it this way?
 
Lord Anoobis said:
With this in mind and the fact that the total momentum after the spring action must be zero, I get

290VC = 150VP, ignoring signs for now. This then means that the velocity the spring imparts to each must be 910m/s divided into an opposite ratio, so to speak. Obviously one or the other must then be a negative quantity and adding the 7600m/s yields the correct answer. Am I correct in thinking about it this way?
That's fine and equivalent to my comment earlier.

Your analysis was fine as well. But you assumed that the capsule went forward and payload backward. Reverse that assumption and you'll get the answers you need. (Don't give up on your original analysis!)
 
Doc Al said:
That's fine and equivalent to my comment earlier.

Your analysis was fine as well. But you assumed that the capsule went forward and payload backward. Reverse that assumption and you'll get the answers you need. (Don't give up on your original analysis!)

I see what you mean and the correct answers have indeed appeared. I actually thought the entire calculation was a complete balls-up but a single sign change makes all the difference. Many thanks.
 

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