Why is √(gμνdxμdxν) the Lagrangian for Geodesic Eq?

In summary, the term √(gμνdxμdxν) is taken as the Lagrangian because it maximizes the interval between points in space time.
  • #1
Apashanka
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15
From the invariance of space time interval the metric dΓ2=dt2-dx2-dy2-dz2
2=gμνdxμdxν
dΓ=√(gμνvμvμ)dt
dΓ=proper time.
Can someone please help me in sort out why the term √(gμνdxμdxν) is taken as the Lagrangian,as geodesic equation is solved by taking this to be the Lagrangian.
 
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  • #3
Think of it like this:

√(dt2 - dx2) = √(1 - v2)dt

so -m√(dt2 - dx2) = -m√(1 - v2) dt

L = -m√(1 - v2)
 
  • #4
Apashanka said:
From the invariance of space time interval the metric dΓ2=dt2-dx2-dy2-dz2
dΓ2=gμνdxμdxν
dΓ=√(gμνvμvμ)dt
dΓ=proper time.
Can someone please help me in sort out why the term √(gμνdxμdxν) is taken as the Lagrangian,as geodesic equation is solved by taking this to be the Lagrangian.
For light like interval dΓ is the maximum interval between two points in space time,
that means this choice of Lagranian actually maximises the interval between points in space time??
 
  • #5
expand out the square root in L = -m√(1 - v2)

You will find a term 1/2 mv2 which is the kinetic energy T.

Then try to connect this to L = T - U
 
  • #6
Apashanka said:
this choice of Lagranian actually maximises the interval between points in space time??
Yes. The requirement is that the action be extremised, not necessarily minimised.
 
  • #7
Apashanka said:
For light like interval dΓ is the maximum interval between two points in space time,
that means this choice of Lagranian actually maximises the interval between points in space time??
You mean time-like. Also, it is the action that is stationary, not the Lagrangian.
 
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  • #8
Orodruin said:
You mean time-like.
yes it is time like ,interval (dΓ)maximised
 
  • #9
Orodruin said:
Also, it is the action that is stationary, not the Lagrangian.
Will you please explain this statement.
Will stationary mean here extremum.e.g either maximum or minimum??
 
  • #10
Apashanka said:
Will you please explain this statement.
Will stationary mean here extremum.e.g either maximum or minimum??
Stationary means that ##\delta S = 0##, this does not necessarily imply max or min.
 
  • #11
Apashanka said:
From the invariance of space time interval the metric dΓ2=dt2-dx2-dy2-dz2
dΓ2=gμνdxμdxν
dΓ=√(gμνvμvμ)dt
dΓ=proper time.
Can someone please help me in sort out why the term √(gμνdxμdxν) is taken as the Lagrangian,as geodesic equation is solved by taking this to be the Lagrangian.
Is this lagrangian obtained from another frame of reference (e.g other than the frame in which interval is dΓ)??
 
  • #12
Apashanka said:
(e.g other than the frame in which interval is dΓ)
Interval is invariant. It's the same for all coordinate systems.
 
  • #13
Ibix said:
Interval is invariant. It's the same for all coordinate systems.
Why I try to say is that other than the frame in which spatial separation between events is 0
 

1. What is the Lagrangian for Geodesic Equations?

The Lagrangian for Geodesic Equations is the mathematical expression √(gμνdxμdxν), where gμν represents the metric tensor and dxμdxν represents the infinitesimal displacement in spacetime. It is used to describe the motion of particles in curved spacetime.

2. Why is the Lagrangian for Geodesic Equations important?

The Lagrangian for Geodesic Equations is important because it is a fundamental concept in Einstein's theory of General Relativity. It helps us understand how particles move in the presence of gravitational fields and how spacetime is curved.

3. How is the Lagrangian for Geodesic Equations derived?

The Lagrangian for Geodesic Equations is derived from the principle of least action, which states that the path a particle takes between two points is the one that minimizes the action. By applying this principle to the motion of particles in curved spacetime, we can derive the Lagrangian for Geodesic Equations.

4. What do the symbols in the Lagrangian for Geodesic Equations represent?

The symbol √(gμνdxμdxν) represents the proper time, which is the time experienced by an observer traveling along the geodesic. The gμν represents the components of the metric tensor, which describe the curvature of spacetime. The dxμdxν represents the infinitesimal displacement in spacetime.

5. Can the Lagrangian for Geodesic Equations be applied to other theories besides General Relativity?

Yes, the Lagrangian for Geodesic Equations can be applied to other theories besides General Relativity. It is a general concept in physics that can be used to describe the motion of particles in any curved space, not just spacetime. It has also been applied in other fields such as classical mechanics and quantum mechanics.

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