Morin's Rocket Example: Chapter 12, Page 606

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Discussion Overview

The discussion revolves around a relativistic rocket example from Morin's classical mechanics book, specifically addressing the treatment of mass changes in the context of relativistic dynamics. Participants explore the implications of defining the change in mass (dm) as either positive or negative and how this affects the resulting equations of motion.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant notes a discrepancy in the rocket motion equation when treating dm as positive versus negative, leading to different results.
  • Another participant suggests that if dm is treated consistently as either positive or negative, the equations should yield the same result.
  • A participant proposes that the confusion may stem from the interpretation of "infinitesimal change in mass" versus "increment of the mass variable" used in integration.
  • It is mentioned that reversing the limits of integration could reconcile the differing results.
  • Further clarification is provided regarding the definitions of variables, particularly how the change in mass (dm) relates to the instantaneous mass of the rocket and the implications for the equations derived.

Areas of Agreement / Disagreement

Participants express differing views on the treatment of the change in mass and its sign, leading to unresolved discrepancies in the resulting equations. There is no consensus on the correct approach or interpretation.

Contextual Notes

Participants highlight the importance of careful variable definitions and the potential for confusion in the treatment of mass changes in relativistic contexts. The discussion remains focused on the mathematical formulation without resolving the underlying conceptual issues.

almarpa
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Hello all.

In Morin's classical mechanics book, chapter 12 (relativistic dynamics), in the axample about the relativistic rocket, we have a rocket that propels itself converting mass into photons and firing them back. Here Morin takes dm as a negative quantity, so the instantaneous mass of the rocket goes from m to m+dm.

I have tried to solve the same example taking dm as a positive quantity, and assuming that the instantaneous mass goes from m to m-dm, but I do not get the same answer. The correct rocket motion equation should be:

(dm/m)+(dv/(1-v2))=0

, but instead I get:

(dm/m)-(dv/(1-v2))=0

As you see, the solution is the same, except for one minus sign.
What could be the problem? Any ideas?

Thank you so much.
 
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If dm is a positive quantity in one equation and a negative quantity in the other then it is the same equation.
 
Yes, that is what I thought.

Nevertheless, in Morin example he integrates this equiation from M to m and from 0 to v to get:

m=M[(1-v)/(1+v)]1/2

But if I integrate my equation in the same terms (from M to m and from 0 to v ), what I get is:

m=M[(1+v)/(1-v)]1/2

As you see, the signs are exchanged in the quotient, so the result is nor the same.

What is the problem?
 
This sounds like it might be a confusion between
the use and/or interpretation of an "infinitesimal change in mass" [whose sign depends on whether one adds or subtracts]
and as an "increment of the mass variable m" (used in doing an integral) [which is always positive].

I think it might analogous to this [my reply in an old thread]
Dot product in the Gravitational Potential Energy formula
 
Ah, then per robphy's point if the OP reverses the limits of integration, they will get the same answer as the other method.
 
Or is that, when ##dm## changes sign (in the attempted change of variables)
then ##v## (or ##dv##) changes sign?
 
Confusing, isn't it?
 
almarpa said:
Confusing, isn't it?
It could be, if one isn't careful.

I took a closer look.
Let's clarify variable names.
m is the instantaneous rocket-mass function (which varies with time).
dm is the incremental change in that rocket-mass function (following what Morin is doing)
so that m+dm represents the new mass (which is smaller than the old mass since the increment is a negative amount).
M is the original mass.

Now if you wish change variables
so that you can (better?) display the fact that the rocket-mass decreases,
let ##(d\mu)=-dm##;
this ##d\mu## is positive (which could be interpreted as the positive photon-energy ejected in the rocket-frame).

Following Morin,
the spatial-momentum of the rocket in the ground frame is
##(m\gamma v)_{new}=(m\gamma v)_{old}-\gamma(1-v)dm##
Using ##(d\mu)##,
##(m\gamma v)_{new}=(m\gamma v)_{old}-\gamma(1-v)(-d\mu)##,
which could be written as
##d(m\gamma v)= -\gamma(1-v)(-d\mu)##.
When expanding out the left-hand side, you have ##dm##, but you have ##d\mu## on the right-hand-side.
If you expand then try to combine terms (in favor of ##d\mu##) to get the diff eq, you get
##\frac{-d\mu}{m}+\frac{dv}{1-v^2}=0##.
However, you can't continue to solve for m unless you use ##d\mu=-dm##.

So, you are forced to same differential equation for ##m##.
 
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All right, I see.

I will take a deeper look to it, to check if I really get it.

Thank you so much, I spent a lot of time thinking about it.
 

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