Jump to content

Gravitational force between 2 bodies at relativistic speeds


Guest blaze

Recommended Posts

Hi all,

 

Newton's law of gravitation states the force between 2 masses M1 and M2 is equal to F = G M1 M2/ d^2

 

My question is simple:

 

Case 1:

 

If both masses are both travelling at relativistic speeds (referred to observer), next to each other, on parallel paths, what would the force be.

 

Case 2:

 

If both masses are travelling at relativistic speeds (referred to observer), on the same path, one behind the other, what would the force be.

 

Thanks

Blaze.

Link to comment
Share on other sites

if they are travelling at relativistic speeds, but stationary with respect to one another (as in case 2, and mostl likely case 1) then there is no difference on the force between them as observed from their own inertial frame. However there will be a difference between the force you observe on them, and the force they observe, and yu can find this by replacing d with the lorentz contraction.

Link to comment
Share on other sites

Let me see if I got it right (assume both masses are equal):

 

From the moving mass reference frame, the force between the masses will not change.

 

From the stationary reference frame,

 

F= y^2 (GMM/d^2) ..... y=Lorentz factor

 

or alternatively we can say that in such a case:

 

F= G (yM)(yM)/d^2

 

So if the stationary observer wants to hold the masses at a fixed distance from each other, he would exert the same force as he normally needs with 2 masses having mass ym each.

 

Right?

Link to comment
Share on other sites

Create an account or sign in to comment

You need to be a member in order to leave a comment

Create an account

Sign up for a new account in our community. It's easy!

Register a new account

Sign in

Already have an account? Sign in here.

Sign In Now
×
×
  • Create New...

Important Information

We have placed cookies on your device to help make this website better. You can adjust your cookie settings, otherwise we'll assume you're okay to continue.