Morin's Rocket Example: Chapter 12, Page 606

Click For Summary
SUMMARY

The forum discussion centers on Morin's relativistic rocket example from Chapter 12 of his classical mechanics book. The original equation for rocket motion is established as (dm/m) + (dv/(1-v²)) = 0, where dm is a negative quantity representing the mass loss of the rocket. The user attempted to derive the same result using a positive dm, leading to an incorrect equation: (dm/m) - (dv/(1-v²)) = 0. The confusion arises from the interpretation of infinitesimal changes in mass and the limits of integration, which must be handled carefully to arrive at the correct solution.

PREREQUISITES
  • Understanding of relativistic dynamics as outlined in Morin's classical mechanics.
  • Familiarity with differential equations and integration techniques.
  • Knowledge of the concepts of mass-energy equivalence and momentum in physics.
  • Experience with the notation and terminology used in calculus, particularly regarding infinitesimals.
NEXT STEPS
  • Study the derivation of the relativistic rocket equation in Morin's classical mechanics, focusing on Chapter 12.
  • Learn about the implications of mass-energy equivalence in relativistic physics.
  • Explore the concept of infinitesimals in calculus and their application in physics.
  • Investigate the relationship between momentum and energy in relativistic contexts.
USEFUL FOR

Students of physics, particularly those studying classical mechanics and relativistic dynamics, as well as educators seeking to clarify concepts related to mass loss in rocket propulsion.

almarpa
Messages
94
Reaction score
3
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.
 
Physics news on Phys.org
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##.
 
  • Like
Likes   Reactions: jim mcnamara
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.
 

Similar threads

  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 17 ·
Replies
17
Views
2K
  • · Replies 15 ·
Replies
15
Views
4K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 30 ·
2
Replies
30
Views
3K
  • · Replies 4 ·
Replies
4
Views
3K
Replies
3
Views
2K
  • · Replies 10 ·
Replies
10
Views
2K
  • · Replies 47 ·
2
Replies
47
Views
4K