Solve 4-velocity Problem with 3-velocity \underline{v}

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SUMMARY

The discussion focuses on the relationship between 4-velocity \overline{U} and 3-velocity \underline{v} in the context of special relativity. It establishes that the spatial components of 4-velocity can be expressed as U^{\alpha} = \gamma(v)v^{\alpha}, where \gamma(v) = \frac{1}{\sqrt{1-v^2}}. The participants clarify that \alpha represents the spatial components, which take values 1, 2, and 3, and emphasize the importance of expressing \gamma(v) in terms of the components of v, specifically using the hint |\vec{v}|^2 = v_{\alpha}v^{\alpha}.

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Homework Statement



4-velocity [tex]\overline{U} = (U^0, U^1, U^2, U^3)[/tex] is related to 3-velocity [tex]\underline{v}[/tex] by [tex]\overline{U} = \gamma(v) (1,\underline{v})[/tex]

Express [tex]U^{\alpha}[/tex] in terms of [tex]\underline{v}[/tex], where [tex]\alpha[/tex] represents the spatial components and takes values 1,2,3.

Homework Equations



[tex]\gamma(v) = \frac{1}{\sqrt{1-v^2}}[/tex].I can't see how this is possible.

[tex]U^{\alpha} = \frac{dx^{\alpha}}{d \tau}[/tex]

[tex]v^{\alpha} = \frac{1}{\gamma (v)} \frac{dx^{\alpha}}{d \tau}[/tex]

How can you do it for just v..?!?
 
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Deadstar said:
I can't see how this is possible.

[tex]U^{\alpha} = \frac{dx^{\alpha}}{d \tau}[/tex]

[tex]v^{\alpha} = \frac{1}{\gamma (v)} \frac{dx^{\alpha}}{d \tau}[/tex]

How can you do it for just v..?!?

Combining the two equations, you should immediately see that [itex]U^{\alpha}=\gamma(v)v^{\alpha}[/itex] (Remember, [itex]\alpha[/itex] varies from one to 3 only, for the spatial components of 4-velocity)

Now you need only express [itex]\gamma(v)[/itex] in terms of the components of [itex]v[/itex]...

hint: [itex]|\vec{v}|^2=v_{\alpha}v^{\alpha}[/itex]
 


gabbagabbahey said:
Combining the two equations, you should immediately see that [itex]U^{\alpha}=\gamma(v)v^{\alpha}[/itex] (Remember, [itex]\alpha[/itex] varies from one to 3 only, for the spatial components of 4-velocity)

Now you need only express [itex]\gamma(v)[/itex] in terms of the components of [itex]v[/itex]...

hint: [itex]|\vec{v}|^2=v_{\alpha}v^{\alpha}[/itex]

Thanks for the reply. I had already got the first part. Just a bit odd notation that threw me off at first.
 

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