Derivation of the momentum-energy relation

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In deriving the relation [tex]E^2=(pc)^2+(mc^2)^2[/tex], I have used the relations [tex]p=\gamma mu[/tex] and [tex]E=\gamma m_0c^2[/tex]. I am currently stuck until a certain step and would appreciate it if someone could show its derivation, thanks a lot...

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Okay,here goes:

[tex]p^{2}=\gamma^{2}m^{2}v^{2}=\frac{c^{2}m^{2}v^{2}}{c^{2}-v^{2}}[/tex]

Add what u need,but only after multiplying by [itex]c^{2}[/itex]:

[tex]p^{2}c^{2}+m^{2}c^{4}=m^{2}c^{4}(\frac{v^{2}}{c^{2}-v^{2}}+1)=<br /> m^{2}c^{4}\frac{c^{2}}{c^{2}-v^{2}}=(\gamma m c^{2})^{2}=E^{2}[/tex]

,where i made use of Einstein's formula...

Daniel.



[tex]p[/tex]
 
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Just to encourage more use of the rapidity [tex]\theta[/tex] (and one's trigonometric intuition):

[tex]u=c\tanh\theta[/tex] and [tex]\gamma=\cosh\theta[/tex] (So, [tex]\gamma u=c\sinh\theta[/tex])

So, start with [tex]p=m_0c\sinh\theta[/tex] and [tex]E=m_0c^2\cosh\theta[/tex].

Since [tex] \begin{align*}<br /> \cosh^2\theta - \sinh^2\theta&\equiv1\\<br /> \left(\frac{E}{m_0 c^2}\right)^2 - \left( \frac{p}{m_0c}\right)^2&=1\\<br /> E^2 - (pc)^2&=(m_0c^2)^2\\<br /> \end{align*}[/tex]
 
dextercioby said:
Though not taught in HS

IMHO, there is no reason why hyperbolic trig functions should not be taught in HS trig (in 1950 we got them in "College Math" which I took Junior year in HS). Nor is there that rapidity should not be taught in intro to relativity for math-enabled students.
 
hey, thanks for the help ! and i'll definitely check out that trig derivation once I've started on hyperbolic functions though...

: )
 
Umm, not to bother you guys but, how does
[tex]p^{2}=\gamma^{2}m^{2}v^{2}=\frac{c^{2}m^{2}v^{2}}{ c^{2}-v^{2}}[/tex]?
What I get is:

[tex](\frac{1}{\sqrt{1-v^2/c^2}})^2=\frac{1}{1-v^2/c^2} *m^2v^2[/tex]

[tex]\frac{m^2v^2}{1-v^2/c^2}[/tex]

Now I'm stuck...
 
oo, you now I got it, thanks. Is that what Dexter meant when he said:
"Add what u need,but only after multiplying by [itex]c^2[/itex]:"?