(gamma)ma=F-[F.(beta)]beta How derive this?

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The discussion centers on the derivation of the equation (gamma)ma=F-[F.(beta)]beta, which involves key concepts from relativistic physics. Participants clarify that "gamma" represents the Lorentz factor, "m" denotes mass, "a" signifies acceleration, "F" stands for force, and "beta" is defined as v/c. Lev Okun's derivation utilizes the equations E=ymc^2 and p=ymv, leading to the expression a=[F-(F.beta)beta]/ym. The conversation emphasizes the importance of understanding the context and components of force vectors in relativistic mechanics.

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  • Understanding of Lorentz transformations and the Lorentz factor (gamma).
  • Familiarity with Newton's laws of motion and force equations.
  • Knowledge of relativistic momentum and energy equations.
  • Basic grasp of vector components in physics.
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(gamma)ma=F-[F.(beta)]beta
How derive this?
 
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Would you mind explaining what it is? Until you explain what "gamma", "m", "a", "F", and "beta" mean, it's just a string of symbols.
 


gamma is the lorentz factor, m is mass, a acceleration, F force; beta is v/c
Lev Okun, in his "concepts of mass" has derived it as follows:
E=ymc^2
p=ymv
dp/dt=F
and next he writes
a=[F-(F.beta)beta]/ym
 
Last edited:


HallsofIvy said:
Would you mind explaining what it is? Until you explain what "gamma", "m", "a", "F", and "beta" mean, it's just a string of symbols.

This is how I feel every time I try to read anything written by a physicist :rolleyes:



But Halls is right. What is the context of the problem you're working on?

The left hand side, F-[F.(beta)]beta, looks a lot like you're trying to remove a component from the force vector (it's very close to the force perpendicular to the direction of motion... is this what you're going for?)
 


I think the equation you are looking for is
{\bf F}=\frac{d{\bf p}}{dt}
\frac{d}{dt}\frac{m{\bf v}}{\sqrt{1-v^2}}
=m{\bf a}\gamma+m{\bf v}({\bf v}\cdot{\bf a})\gamma^3.
This is the usual form.
To get your form, use the above equation to show
{\bf v}\cdot{\bf F}=m\gamma^3{\bf v}\cdot{\bf a}
in a few steps.
I use units with c=1.
I couldn't find my latex errors. I hope you can read it as is.
 
Last edited by a moderator:


clem said:
I couldn't find my latex errors. I hope you can read it as is.
Just add tex tags.

clem said:
I think the equation you are looking for is
{\bf F}=\frac{d{\bf p}}{dt}
\frac{d}{dt}\frac{m{\bf v}}{\sqrt{1-v^2}}<br /> =m{\bf a}\gamma+m{\bf v}({\bf v}\cdot{\bf a})\gamma^3.
This is the usual form.
To get your form, use the above equation to show
{\bf v}\cdot{\bf F}=m\gamma^3{\bf v}\cdot{\bf a}
in a few steps.
I use units with c=1.
 


Thank you. I did use ..., but it kept showing errors.
I guess it can read your handwriting.
 


I got it thanks but using the equation gives F=y^3ma when parallel and F=yma when transverse why is dt so?
 
Last edited:


You can't argue with algebra. There is no "why" in algebra.
 
  • #10


Usually it is "y" times mass but here it increases to y^3 times as we move from transverse to longitudinal
 

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