GRAVITATION by MTW: p.49, lambda or tau?

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Discussion Overview

The discussion revolves around the parameterization of a worldline in the context of general relativity, specifically addressing the use of parameters lambda and tau in the equation for a straight line tangent to the worldline as presented in MTW (Misner, Thorne, and Wheeler). Participants explore the implications of using different parameters in the vector equation and the relationship between the worldline and the tangent vector.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant questions the use of lambda in the equation, suggesting that since the worldline is parameterized by tau, the equation should use tau instead of lambda.
  • Another participant argues that the equation is appropriate as it represents a tangent vector to the worldline, and the parameter k (which could be lambda) does not need to be directly related to time.
  • A participant reiterates the initial concern about the parameterization, emphasizing the need for clarity on why tau should be used in the vector equation for the tangent line.
  • Further discussion highlights that differentiating the straight line equation with respect to tau yields the tangent at tau=0, suggesting that the relationship between lambda and tau is not straightforward.
  • Another participant points out that the distinction between vector quantities and constants at a specific point in the worldline is crucial for understanding the differentiation process involved.

Areas of Agreement / Disagreement

Participants express differing views on the appropriateness of using lambda versus tau in the tangent vector equation. There is no consensus on which parameter should be used, and the discussion remains unresolved regarding the implications of each choice.

Contextual Notes

The discussion highlights the complexity of parameterization in the context of worldlines and tangent vectors, with participants noting that the differentiation process and the nature of the quantities involved may influence the choice of parameter. There are unresolved assumptions regarding the relationship between lambda and tau.

Living_Dog
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At the very bottom of the page they have that the straight line, using the definition of a vector as the derivative of the worldline is given as:

[tex]P(0) + \lambda(\frac{dP}{d\tau})_o[/tex]

But since the worldline, [tex]P(\tau)[/tex] is paramtrized by [tex]\tau[/tex] and not [tex]\lambda[/tex], then shouldn't the equation be:

[tex]P(0) + \tau(\frac{dP}{d\tau})_o[/tex]

?

Thanks in advance.
 
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I'm not sure what you think the trouble is. It seems fine to me. At that point, the world line isn't straight, and they just seem to be looking for the vector equation of the straight line which is tangent to that point. The equation is just the vector pointing to the point, plus k x tangent vector, with k an arbitrary real. There's no reason why this k should be intimately connected with t is there
 
Living_Dog said:
At the very bottom of the page they have that the straight line, using the definition of a vector as the derivative of the worldline is given as:

[tex]P(0) + \lambda(\frac{dP}{d\tau})_o[/tex]

But since the worldline, [tex]P(\tau)[/tex] is paramtrized by [tex]\tau[/tex] and not [tex]\lambda[/tex], then shouldn't the equation be:

[tex]P(0) + \tau(\frac{dP}{d\tau})_o[/tex]

?

Thanks in advance.

Just a little typo. Your correction is completely apposite.

AB
 
Altabeth

if you get a chance, could you explain that to me. For the equation of the straight line that is a tangent to the curve, why does tau have to appear as the parameter in the vector equation? I can't see any connection.
 
yossell said:
Altabeth

if you get a chance, could you explain that to me. For the equation of the straight line that is a tangent to the curve, why does tau have to appear as the parameter in the vector equation? I can't see any connection.

The parameter of curve is apparently [tex]\tau[/tex] and when you differentiate the straight line [tex]P(0) + \tau(\frac{dP}{d\tau})_o[/tex] with respect to [tex]\tau[/tex] then you get the tangent to curve at [tex]\tau=0[/tex] which is [tex](dP(\tau)/d\tau)_0.[/tex] I f we take [tex]\lambda[/tex] to be related to [tex]\tau[/tex] linearly, [tex]\lamda=a\tau+b[/tex] with both [tex]a,b[/tex] being constants (a=/=0) then it doesn't let the differentiation produce the tangent through including an extra factor [tex]a[/tex] multiplied by the true tangent above.

P.s. when you talk of straight line you're no longer allowed to asign a "vector equation" to this line. "tau" is just a parameter of curve and has the same role as [tex]t[/tex] in the Newtonian equation [tex]x=vt+x_0.[/tex]

AB
 
Last edited:
Thanks Altabeth,

But in MTW they only say `the straight line' of the four velocity. For this, I'm struggling to see a connection between the parameter used on the curve and the parameter on the new straight line. It's surely irrelevant what it is, and provided to differentiate the function with respect the variable, whether it's tau or lambda, you get the right result.

And from MTW
One must first form dP/d\tau and only thereafter draw the staight line P(0) + \lambda(dP/d\tau)

P(0) and dP/d\tau are vectors, this is a vector equation, and they're calling it a straight line.
 
yossell said:
Thanks Altabeth,

But in MTW they only say `the straight line' of the four velocity. For this, I'm struggling to see a connection between the parameter used on the curve and the parameter on the new straight line. It's surely irrelevant what it is, and provided to differentiate the function with respect the variable, whether it's tau or lambda, you get the right result.

And from MTW


P(0) and dP/d\tau are vectors, this is a vector equation, and they're calling it a straight line.

Gotta be more careful here: They are saying that [tex]P(0)+\lambda (dP/d\tau)_0[/tex] is a straight line. You think incorrectly that [tex]P(0)[/tex] and [tex]dP/d\tau[/tex] are vectors whereas [tex]P(\tau)[/tex] and [tex]dP/d\tau[/tex] are respectively the straight world line of a free particle (a non-vector quantity) and the tangent on this world line so that both of [tex]P(0)[/tex] and [tex]dP/d\tau[/tex] due to being computed at some point ([tex]\tau=0[/tex]) are to be considered as constants only. This means when taking the derivative of[tex]P(0)+\lambda (dP/d\tau)_0[/tex] with respect to the variable of world line, i.e. [tex]\tau[/tex], you get

[tex]\frac{d\lambda}{d\tau} (\frac{dP}{d\tau})_0[/tex]

which was expected to be the tangent to the world line,

[tex](\frac{dP}{d\tau})_0[/tex]

thus leading to

[tex]\frac{d\lambda}{d\tau} =1[/tex]

or

[tex]\lambda=\tau.[/tex]

I hope this helps.

AB
 

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