Gallilean v/s Lorentz transformation

In summary, the Galilean transformation and the Lorentz transformation are mathematical frameworks used to relate the coordinates of events in different inertial frames of reference. The Galilean transformation, applicable at low speeds relative to the speed of light, assumes time is absolute and does not change between frames, leading to simple additive relationships for position and velocity. In contrast, the Lorentz transformation arises from the principles of special relativity and accounts for the effects of time dilation and length contraction at high speeds, particularly as objects approach the speed of light. This results in a more complex relationship that maintains the constancy of the speed of light across all inertial frames.
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PhysicsEnjoyer31415
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Why do we still use gallilean transformation if Lorentz transformation works for all velocities equal to and approaching 'c' . Also by using Gallilean transformations it is possible to get values of relative velocity more than 'c' which is not possible ....So is this because it is practically the same for v<c or just because it is a prerequisite to lorentz transformation?
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You can ask the same question about why we still use Newtonian gravitation when we have general relativity. The answer is that it is much simpler to apply and for most applications the predictions are indistinguishable. Obviously, when we enter realms where there is a relevant difference, such as objects moving at high relative velocities, then Lorentz transformations must be applied to get a result compatible with experiments.

Newtonian physics is also much easier to understand as so much more of it appears "intuitive" to more people. Most engineers will never need relativity and so they can make do with the conceptually easier Newtonian physics. (Of course, if you work enough with relativity, it also becomes "intuitive", which in essence is just our brains telling us that we are familiar enough with something that we can discern the main results without going into much detail.) Who do you prefer building your bridge: An engineer using Newtonian physics or an engineer using relativistic physics, but taking three times as long and possibly getting it wrong because it became conceptually difficult?
 
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Newtonian physics is conceptually and mathematically much easier than relativity, and for most applications in every day life the answers will be the same to the precision you can measure.

If I drive at 60mph for an hour and return home, this is a twin paradox scenario and I will have aged less than my twin who stayed at home. 60mph is about 30m/s, which equates to a ##\gamma## of about ##1+5\times 10^{-15}##, which means I'm about 20 picoseconds younger after my hour journey. That's indistinguishable from "I'm the same age as my twin", so why pay the price of the additional maths?
 
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Oh .....now that makes so much more sense.
 
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We call this idea the correspondence principle: different theories are used in different regions. No theory is "the ultimate theory"; some theories just happen to be broader applicable. The correspondence principe guarantees you that for v<<c Einstein's theory of special relativity effectively becomes Newton's theory of motion (both on the level of equations of motion and underlying symmetries).

Try to use Einstein's theory of General Relativity to describe the free fall motion of a rock here on Earth and you'll understand why we turn to Newton.
 
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haushofer said:
Try to use Einstein's theory of General Relativity to describe the free fall motion of a rock here on Earth and you'll understand why we turn to Newton.
I mean ... That particular piece of phenomenology is not that hard in GR ...
 
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haushofer said:
We call this idea the correspondence principle: different theories are used in different regions. No theory is "the ultimate theory"; some theories just happen to be broader applicable. The correspondence principe guarantees you that for v<<c Einstein's theory of special relativity effectively becomes Newton's theory of motion (both on the level of equations of motion and underlying symmetries).

Try to use Einstein's theory of General Relativity to describe the free fall motion of a rock here on Earth and you'll understand why we turn to Newton.
Oh ok 👍just another question that do we have anything better than einstein's SR and GR as of now ?
 
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Orodruin said:
I mean ... That particular piece of phenomenology is not that hard in GR ...
Relatively speaking.
 
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PhysicsEnjoyer31415 said:
Oh ok 👍just another question that do we have anything better than einstein's SR and GR as of now ?
No. Not for gravitational phenomena or non-quantum dynamics like classical electromagnetism, that is.
 
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Ibix said:
If I drive at 60mph for an hour and return home, this is a twin paradox scenario and I will have aged less than my twin who stayed at home. 60mph is about 30m/s, which equates to a ##\gamma## of about ##1+5\times 10^{-15}##, which means I'm about 20 picoseconds younger after my hour journey. That's indistinguishable from "I'm the same age as my twin", so why pay the price of the additional maths?
Just to be sure: the fact that you aged less than your twin who stayed at home, is invariant since both you and your twin's timelike worldlines share the same start and return events respectively.

However the above is not symmetric (from your point of you is your twin moving), since you and not your "at home twin" undergo proper acceleration at some point/event along your timelike worldline.
 
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FAQ: Gallilean v/s Lorentz transformation

What is the main difference between Galilean and Lorentz transformations?

The main difference lies in how they account for the effects of relative motion on time and space. Galilean transformations assume that time is absolute and the same for all observers, leading to the classical mechanics framework. In contrast, Lorentz transformations, derived from Einstein's theory of special relativity, incorporate the effects of time dilation and length contraction, indicating that measurements of time and space can differ for observers in relative motion, particularly at speeds approaching the speed of light.

When are Galilean transformations applicable?

Galilean transformations are applicable in classical mechanics, particularly when dealing with objects moving at speeds much less than the speed of light. They are used in everyday situations where relativistic effects are negligible, such as the motion of cars, projectiles, and other objects in our daily experience.

What are the key equations for Galilean and Lorentz transformations?

The key equations for Galilean transformations are: 1. x' = x - vt (for position)2. t' = t (for time). For Lorentz transformations, the equations are: 1. x' = γ(x - vt) (for position), 2. t' = γ(t - (vx/c²)) (for time), where γ (gamma) is the Lorentz factor defined as γ = 1 / √(1 - v²/c²), with v being the relative velocity and c the speed of light.

How do Galilean and Lorentz transformations affect the concept of simultaneity?

In Galilean transformations, simultaneity is absolute; events that are simultaneous in one inertial frame are simultaneous in all frames. However, in Lorentz transformations, simultaneity is relative; events that are simultaneous in one frame may not be simultaneous in another frame moving relative to the first, due to the finite speed of light and the effects of time dilation.

Why are Lorentz transformations important in modern physics?

Lorentz transformations are crucial because they provide the mathematical framework for understanding phenomena in special relativity, which has been experimentally validated in numerous scenarios involving high-speed particles and electromagnetic radiation. They help explain behaviors that cannot be accounted for by classical mechanics, such as time dilation, length contraction, and the invariance of the speed of light, fundamentally altering our understanding of space, time, and the nature of the universe.

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