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ModPhy1/Unit1/SpecialRelativity/RelativeView/

8/21/04

 

1.      Galilean Velocities

2.      Lorentz Velocities

Velocity is Relative

 


 

The Galilean Velocity Transformation Equation

Velocity is a relative quantity in both classical and relativistic physics. But classical physics admits the possibility of an absolute rest frame. According to classical physics, Newton's laws of mechanics are velocity invariant (the same in all inertial reference frames independent of their velocities), but Maxwell’s electromagnetic field equations are not. They are valid only in one preferred reference frame. Therefore, classical physics sometimes treated velocity as being relative and at other times as being absolute.

 

The classical equations for transforming relative velocities from one inertial reference frame to another are called the Galilean velocity transformation equations. When reduced to linear form, they become:

 

vAB = velocity of A relative to B, etc.

vBA = -vAB

vAC = vAB + vBC

 

According to this equation, relative velocities simply add to one another. For this reason, velocity transformation equations are also called velocity addition equations.

 

As an illustration of the application of this equation, suppose two cosmic rays approach the earth from opposite directions at 0.9 c. Then v1E = 0.9 c, v2E = -0.9 c = - vE2 , and v12 = v1E + vE2  = 0.9 c + 0.9 c = 1.8 c. Therefore, according to classical physics, the velocity of one cosmic ray with respect to the other is greater than the speed of light.

 

 

The Lorentz Velocity Transformation Equation

Relativistic physics denies the existence of an absolute rest frame. Therefore, relativity always treats velocity as a relative quantity, never as an absolute quantity.

 

The relativistic velocity addition equations are called the Lorentz velocity transformation equations. When reduced to linear form, they become:

 

vAB = velocity of A relative to B, etc.

vBA = -vAB

 

As you can see, the relativistic velocity addition equation contains an additional factor in the denominator of the expression that prevents the sum of two velocities from ever exceeding the speed of light.

 

For example, consider the same two cosmic rays treated classically above and substitute their relative velocities into the Lorentz velocity transformation equation. Then, v12 = (0.9c+0.9c)/(1+(0.9c)(0.9c)/c2) = (1.8c)/(1.81) = 0.9945 c. Therefore, according to relativity, the velocity of the first cosmic ray with respect to the second is close to, but still less than, the speed of light.

 


 

Questions:

Q1.      An object A is moving in the +y-direction with a speed of 0.8 c. Object B is moving in the -x-direction with a speed of 0.8 c. What is the speed of object A with respect to object B according to relativity.
0.933 c 5154

 

Problems:

P1.       Classical Boost Sequence

A large acceleration over a short period of time is called a “boost.” (a) Use the Galilean velocity addition equations to determine the speed of a spaceship boosted twice, each time to half the speed of light. (b) What is its speed after the third such boost? (c) After the fourth? (d) After the fifth? (e) After the n’th? (f) Will such a process of multiple boosts ever accelerate the spaceship faster than the speed of light?

 

P2.       Relativistic Boost Sequence

Use the Lorentz velocity addition equations to determine the speed of a spaceship twice boosted to half the speed of light. (b) What is its speed after the third such boost? (c) After the fourth? (d) After the fifth? (e) After the n’th? (f) Will such a process of multiple boosts ever accelerate the spaceship faster than the speed of light?

 

P3.       Correspondence Principle

Prove that the Lorentz velocity addition equation reduces to the Galilean velocity addition equation for small velocities.

 

P4.       Velocity of a Photon

A photon of speed c passes a spaceship of speed v moving in the same direction relative to the earth. (a) Use the relativistic velocity addition equation to show that the speed of the photon relative to the spaceship is also c. (a) Show that the same is true for a photon traveling in the opposite direction.

 

P4.       A Photon Approaching a Photon

(a) Use the velocity addition equation to determine the relative velocity of two photons traveling in opposite directions. (b) Use the velocity addition equation to determine the relative velocity of two photons traveling in the same direction.

 

 

  1. Galilean Velocities – The three-dimensional classical velocity addition equations.
  2. Lorentz Velocities– The three-dimensional relativistic velocity addition equations.

ModPhy1/Unit1/SpecialRelativity/RelativeView/