'Expansion' of fluid world lines

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Discussion Overview

The discussion revolves around the concept of the expansion of fluid world lines in the context of general relativity, specifically referencing exercise 22.6 from MTW. Participants explore the mathematical expressions and physical interpretations related to the divergence of fluid 4-velocity and its implications for fluid dynamics in a relativistic framework.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Homework-related

Main Points Raised

  • One participant questions why the expression ∇·u is termed the expansion of fluid world lines, suggesting a connection to the commutator and the closure of quadrilaterals formed by vectors.
  • Another participant states that the expansion θ = ∇·u describes the rate of increase of the volume of a fluid element, referencing exercise 22.1 for clarification.
  • It is proposed that the expression ∇_a u^a can be shown to represent the rate of change of an infinitesimal space-time volume along the worldline of a fluid element.
  • One participant mentions deriving a solution based on the continuity equation and assumptions about the divergence of density.
  • References to additional resources, such as a previous thread and a book by Wheeler and Ciufolini, are made to provide further context and geometric descriptions of hydrodynamical quantities in general relativity.

Areas of Agreement / Disagreement

Participants appear to share some understanding of the mathematical expressions involved, but there is no explicit consensus on the interpretation of the expansion of fluid world lines or the implications of the divergence of the fluid 4-velocity.

Contextual Notes

Some participants reference specific exercises and concepts from MTW, indicating that the discussion is grounded in particular mathematical frameworks and assumptions that may not be universally accepted or understood.

zn5252
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hello
In MTW exercise 22.6, given a fluid 4-velocity u, why the expression :
∇.u is called an expansion of the fluid world lines ?

Is the following reasoning correct ?

We know that the commutator : ∇BA - ∇AB is (see MTW box 9.2) is the failure of the quadrilateral formed by the vectors A and B to close.

Now If we apply this to the expression of the fluid world lines I would get :

eσu - ∇ue = ∇eσu since a freely falling observer Fermi-Walker transports its own spatial basis (see MTW page 218) thus one can conclude that the quadrilateral formed by the time segment and the velocity segment does not close which means that the fluid expands 'or contracts'.

Regards,
 
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zn5252 said:
In MTW exercise 22.6, given a fluid 4-velocity u, why the expression : ∇·u is called an expansion of the fluid world lines ?
This quote from Ex. 22.6 explains why:

Exercise 22.1 showed that the expansion θ = ∇·u describes the rate of increase of the volume of a fluid element.
 
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One can show that ##\nabla_a u^a = \frac{1}{V}u^a \nabla_a V## where ##V## is an infinitesimal space-time volume carried along the worldline of some fluid element. So ##\nabla_a u^a## represents the rate of change of said volume per unit volume along the worldline of some fluid element.
 
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Bill_K said:
This quote from Ex. 22.6 explains why:

Oh I see Bill. I did not get to part b) yet .
 
WannabeNewton said:
One can show that ##\nabla_a u^a = \frac{1}{V}u^a \nabla_a V## where ##V## is an infinitesimal space-time volume carried along the worldline of some fluid element. So ##\nabla_a u^a## represents the rate of change of said volume per unit volume along the worldline of some fluid element.

Indeed this is what part b) mentions. Thanks !
 
Cool! Have fun with the exercise :) MTW has the solution to 22.1 right below, if you're interested as to why the above is true.
 
WannabeNewton said:
Cool! Have fun with the exercise :) MTW has the solution to 22.1 right below, if you're interested as to why the above is true.

Indeed I saw it and also attempted to derive my own which yielded the correct result based on the continuity equation and on the assumption that the divergence of the density is negligible...
 
WannabeNewton said:
Nice! We had a similar thread a while back that you might be interested in, where everything was done in a coordinate-free manner: https://www.physicsforums.com/showthread.php?t=702266&highlight=physical+description+concepts

Also, if you have access to Wheeler and Ciufolini's "Gravitation and Inertia", they give a very nice geometric description of hydrodynamical quantities in GR starting in section 4.5 (p.234).

Great . Thanks ! I have Wheeler and Ciufolini's "Gravitation and Inertia". I will check that out. Thanks for mentioning that.
 
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Anytime broski! :)
 

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