How can you create a geodesic path using the metric and initial velocity?

Click For Summary
To create a geodesic path for an object approaching Earth, one must utilize the given metric, initial velocity, and the equations of motion. The metric provided is a Minkowski space metric, indicating no external gravitational forces are present. The initial velocity vector can be applied to the metric to compute incremental steps along the geodesic. A numerical solution approach, such as using Scilab for the Schwarzschild metric, has been explored, although technical issues with file compression have hindered sharing results. The discussion highlights the need for clarity in the mathematical formulation and encourages collaboration for further exploration.
Jack3145
Messages
14
Reaction score
0
Let's say there is a small object heading towards Earth (it will burn up). It is first observed at:
x^{\\mu}=[x^{1},x^{2},x^{2},x^{4}]=[x_{0},y_{0},z_{0},t_{0}]
with a velocity:
V_{v}=[v_{1},v_{2},v_{3},v_{4}]

The metric is:
ds^{2} = dx^{2} + dy^{2} + dz^{2} -c^{2}*dt^{2}
g_{\\mu\\v} = \\left(\\begin{array}{cccc}<BR>1 & 0 & 0 & 0\\\\<BR>0 & 1 & 0 & 0\\\\<Br>0 & 0 & 1 & 0\\\\<BR>\\\\<BR>0 & 0 & 0 & 1<BR>\\end{array})\\right

Affinity is:
\\Gamma^{\\rho}{\\mu\\v} = 0

Riemann Curvature tensor is:
R^{\\rho}{\\mu\\v\\sigma} = 0

Ricci Tensor is:
R{\\mu\\sigma} = 0

My Question is how do you make a geodesic path from the metric and initial velocity?

V_{v} = x^{\\mu}*g_{\\mu\\v} and make incremental steps?
 
Last edited:
Physics news on Phys.org
Sorry for the abomination. I know that Minkowski Space has no external gravitational forces acting on it.
 
You can still edit post #1. Looks like you need to remove a lot of \ symbols.
 
You indicated an interest in a numerical solution. I did a Scilab solution for the Schwarzschild metric. Unfortunately I compressed the file using bz2 on Linux and my present (vista) decoder has a problem. If you are interested I will have my Linux machine back up in two weeks or perhaps somebody else will separate out the parts; the mash-up is probably my fault.
I never checked the compression or enhanced the program since nobody ever responded to my scilab post.
Some orbits are shown in the eps file at:
http://www.plaidheron.com/ray/temp/
drdth_f-example.eps
Ray
 
Last edited by a moderator:
MOVING CLOCKS In this section, we show that clocks moving at high speeds run slowly. We construct a clock, called a light clock, using a stick of proper lenght ##L_0##, and two mirrors. The two mirrors face each other, and a pulse of light bounces back and forth betweem them. Each time the light pulse strikes one of the mirrors, say the lower mirror, the clock is said to tick. Between successive ticks the light pulse travels a distance ##2L_0## in the proper reference of frame of the clock...

Similar threads

  • · Replies 4 ·
Replies
4
Views
1K
  • · Replies 24 ·
Replies
24
Views
2K
  • · Replies 62 ·
3
Replies
62
Views
6K
  • · Replies 3 ·
Replies
3
Views
819
  • · Replies 5 ·
Replies
5
Views
1K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 15 ·
Replies
15
Views
3K
Replies
82
Views
5K
  • · Replies 7 ·
Replies
7
Views
2K