Galilean Transformations and Postulates

In summary, a Galilean transformation on the point (t,x) is a constant velocity transform, a translation transform, and a rotation transformation. It is based on the postulates that two observers observe the same time between events and measure the same distance for simultaneous events. However, it can be modified to preserve time and distance by using an arbitrary velocity function v(t). In classical mechanics, this is allowed according to Arnold, but in relativity, boosts cannot be a function of spacetime.
  • #1
RedX
970
3
I read that the form of a galilean transformation on the point (t,x) is the following:

constant velocity transform by velocity v: (t,x) ---> (t,x+vt)
translation transform by (t0,x0): (t,x)--->(t+t0,x+x0)
rotation transformation by rotation matrix R: (t,x)--->(t,Rx)

and that it is based on the following postulates: two observers observe the same time between events, and two observers measure the same distance for simultaneous events.

My question is, based on those two postulates, couldn't you modify the first transform to

(t,x)--->(t,x+vf(t))

This transformation preserves the time between events (it doesn't change time at all). It also preserves simultaneous distance:

|(x1+vf(t))-(x2+vf(t))|=|x1-x2|
 
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  • #2
Yeah, doesn't that just correspond to moving with an arbitrary velocity v(t)=vf(t)?
 
  • #3
darkSun said:
Yeah, doesn't that just correspond to moving with an arbitrary velocity v(t)=vf(t)?

Yeah, but unfortunately the book I'm using (Mathematical Methods of Classical Mechanics, V. Arnold) emphasizes that v is uniform.

If you take the simplest case of a uniformily accelerated reference frame, then the transformation would look like:

(t,x)--->(t,x+.5*g*t2)

This transformation preserves the time between two events, and the distance between simultaneous events. So two observers, one uniformily accelerating with respect to the other, observe the same time between events and the same distance between simultaneous events.

So according to Arnold, such a transformation is a gallilean transformation.

Bringing in relativity, things are much different. Instead of preserving time between events and distance between simultaneous events separately, you consider transformations that preserve:

(ct)^2-(x)^2

Here you can show that the Poincare group (as opposed to the gallilean group) is a 10-parameter group consisting of uniform boosts, rotations, and translations. The boosts have to be uniform and can't be a function of spacetime.

But it seems in classical mechanics, according to Arnold, you can have boosts that depend on time (so reference frames can be accelerated), although not space.
 

1. What are Galilean Transformations?

Galilean Transformations are mathematical equations that describe the relationship between space and time in different reference frames, specifically in non-accelerating frames of reference. They were developed by Galileo Galilei in the 17th century and are still used today in classical mechanics.

2. What are the two postulates of Galilean Transformations?

The first postulate states that the laws of physics are the same in all inertial frames of reference, meaning that the laws of physics do not change regardless of the observer's position or velocity. The second postulate is the principle of relativity, which states that there is no preferred inertial frame of reference and all inertial frames are equally valid.

3. How do Galilean Transformations differ from Einstein's theory of relativity?

Galilean Transformations are based on Newton's laws of motion and assume that time and space are absolute, while Einstein's theory of relativity takes into account the constancy of the speed of light and the relativity of time and space. This means that in Einstein's theory, the laws of physics are the same in all frames of reference, even in accelerating ones.

4. Can Galilean Transformations be applied to objects moving at speeds close to the speed of light?

No, Galilean Transformations are only valid for objects moving at speeds much slower than the speed of light. At higher speeds, the equations break down and Einstein's theory of relativity must be used to accurately describe the behavior of objects.

5. How are Galilean Transformations used in everyday life?

Galilean Transformations are used in many practical applications, such as predicting the motion of objects in the sky or calculating the trajectory of a projectile. They are also used in the design of vehicles, buildings, and other structures to account for the effects of gravity and motion.

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