Special Relativity 4-vector problem - Doing my head in

In summary, the problem is to find the energy of a photon when it is observed by two different observers.
  • #1
Astrofiend
37
0

Homework Statement



OK - the problem is thus:

In an inertial frame two observers (called a & b) travel along the positive x-axis with velocities Va and Vb. They encounter a photon traveling in the opposite x-direction. Without using the Lorentz transformations, show that the ratio of the energies of the photon observed by observers a & b is given by:

[tex]

\frac{E_a}{E_b} = \sqrt{\frac{1+V_a}{1+V_b}.\frac{1-V_b}{1-V_a}}

[/tex]

Homework Equations



[tex]

E_o = -p_o.u_o

[/tex]

where E_o is the observed energy of a photon with 4-momentum p_0, by a given observer moving with 4-velocity u_o.

I set up the 4-velocities of observers a & b as:

[tex]

u^\alpha_a = (\gamma_a,\gamma__a V_a ,0,0)

[/tex]
[tex]

u^\alpha_b = (\gamma_b,\gamma__b V_b ,0,0)

[/tex]

and the 4-momentum of the photon as:

[tex]

p^\alpha = (p^t,p^x, 0,0)

[/tex]

The Attempt at a Solution



With these 4-vectors set up, the energies of the photon for each observer should just be the dot product of each 4-velocity with the negative of the 4-momentum of the photon - i.e:

[tex]

E_o = -p_\alpha .u^\alpha = - \eta_\alpha_\beta p^\alpha .u^\alpha
[/tex]

where [tex] \eta_\alpha_\beta [/tex] is the metric.

so

[tex]
E_a = \gamma_a p_t + \gamma_a V_a p_x \\
[/tex]

[tex]
E_b = \gamma_b p_t + \gamma_b V_b p_x
[/tex]

Then, I used the fact that for a photon,

[tex]
p^\alpha.p^\alpha = 0 \\
[/tex]

[tex]
i.e. -p_t^2+ p_x^2 = 0 \\
[/tex]

so

[tex]
p_t = p_x
[/tex]

and we get:

[tex]E_a = \gamma_a p_t + \gamma_a V_a p_t = \gamma_a p_t (1+V_a) \\
[/tex]

[tex]
E_b = \gamma_b p_t + \gamma_b V_b p_t = \gamma_b p_t (1+V_b) \\
[/tex]

so

[tex]
\frac{E_a}{E_b} = \frac{\sqrt{1-V_b^2}(1+V_a)}{\sqrt{1-V_a^2}(1+V_b)}
[/tex]

...which is where I'm falling down. As I said before, I'm after the relation

[tex]

\frac{E_a}{E_b} = \sqrt{\frac{1+V_a}{1+V_b}.\frac{1-V_b}{1-V_a}}

[/tex]

Can anyone see what I'm doing wrong? Have I made a mistake somewhere, or is there some mathematical trick to take me further from where I am to the required answer? I've stared at this for a while now and can't work out why it's falling down.

Any help would be greatly appreciated.
 
Last edited:
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  • #2
Actually, I think I botched the dot product earlier between the 4-vels and the 4-mom. I think it should give me:

[tex]
E_a = \gamma_a p_t - \gamma_a V_a p_t = \gamma_a p_t (1-V_a) \\
[/tex]

[tex]
E_b = \gamma_b p_t - \gamma_b V_b p_t = \gamma_b p_t (1-V_b) \\
[/tex]

as opposed to:

[tex]
E_a = \gamma_a p_t + \gamma_a V_a p_t = \gamma_a p_t (1+V_a) \\
[/tex]

[tex]
E_b = \gamma_b p_t + \gamma_b V_b p_t = \gamma_b p_t (1+V_b) \\
[/tex]

i.e. with minus signs, not the plusses I have before. But this seems to take me even further away from where I want to be. Arrg!

Help!
 
  • #3
Astrofiend said:
[tex]
\frac{E_a}{E_b} = \frac{\sqrt{1-V_b^2}(1+V_a)}{\sqrt{1-V_a^2}(1+V_b)}
[/tex]

...which is where I'm falling down. As I said before, I'm after the relation

[tex]

\frac{E_a}{E_b} = \sqrt{\frac{1+V_a}{1+V_b}.\frac{1-V_b}{1-V_a}}

[/tex]

Can anyone see what I'm doing wrong?

Nothing is wrong. These two expressions are equal. It's easier to see this by squaring each expression, then using [itex]1-V^2 = (1-V)(1+V)[/itex].
 
  • #4
Ah - thanks heaps. I'll work through it!

Cheers.
 

FAQ: Special Relativity 4-vector problem - Doing my head in

What is a 4-vector in special relativity?

A 4-vector in special relativity is a mathematical object that consists of four components: three components for space and one component for time. It is used to represent physical quantities in spacetime, which is a four-dimensional space that combines space and time into a single entity.

How is a 4-vector used to solve problems in special relativity?

A 4-vector is used in special relativity to solve problems involving the behavior of objects moving at high speeds or in strong gravitational fields. By representing physical quantities as 4-vectors, it allows for the application of the principles of special relativity, such as time dilation and length contraction, to accurately describe the behavior of these objects.

What is the difference between a contravariant and a covariant 4-vector?

In special relativity, a contravariant 4-vector has components that transform in the opposite direction of the coordinate system, while a covariant 4-vector has components that transform in the same direction as the coordinate system. This distinction is important in solving problems in special relativity, as the transformation of 4-vectors is dependent on their type.

How do you calculate the magnitude of a 4-vector in special relativity?

The magnitude of a 4-vector in special relativity is calculated using the Minkowski metric, which takes into account both the time and space components of the vector. This metric is used to calculate the spacetime interval, which is the invariant quantity that remains the same for all observers in special relativity.

What are some common applications of 4-vectors in special relativity?

4-vectors are commonly used in special relativity to describe physical quantities such as position, velocity, momentum, and energy. They are also used in the formulation of the Einstein field equations, which describe the behavior of gravity in the context of special relativity. 4-vectors are also crucial in the development of many modern technologies, such as GPS navigation systems and particle accelerators.

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