Understanding E=mc² and Other Equations of Relativity

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Discussion Overview

The discussion revolves around the equations of relativity, specifically E=mc² and E²=m²c⁴+p²c². Participants explore the implications of these equations, the concept of relativistic mass, and the role of the Lorentz factor (γ) in different contexts, including total energy and momentum. The scope includes theoretical aspects and mathematical reasoning related to special relativity.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • Some participants express confusion about the relationship between E²=m²c⁴+p²c² and E=mγc², questioning how they can be equivalent.
  • Others clarify that E²=m²c⁴+p²c² uses rest mass (m) and that substituting for momentum leads to E=mγc².
  • There is a discussion about whether the Lorentz factor (γ) should be applied to both terms in the equation when considering relativistic mass.
  • Some participants argue that the longer form of the equation is also useful for massless particles, while others suggest that defining "relativistic mass" complicates the understanding of force and acceleration.
  • Participants provide algebraic steps to show how the two equations can yield the same results, though some express difficulty in following the algebraic manipulations.
  • One participant emphasizes the importance of understanding the definition of γ and its derivation from the context of Minkowski space-time.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the utility of the concept of relativistic mass, with some advocating for its use while others argue against it. There is also ongoing uncertainty about the equivalence of the two equations and the appropriate application of the Lorentz factor.

Contextual Notes

Some participants mention the need for algebraic proficiency to navigate the mathematical aspects of the discussion. There are unresolved steps in the algebraic derivations presented, and the discussion reflects varying levels of understanding among participants.

Who May Find This Useful

This discussion may be useful for individuals interested in the mathematical foundations of special relativity, the interpretation of relativistic equations, and the conceptual challenges surrounding relativistic mass and energy.

Antuanne
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I've just saw this other equation E2=m2c4+p2c2 but what's going on with that? I thought E=mγc2 was the equation including relativistic mass. What is going on?
 
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Just algebra. If you substitute the expression for relativistic 3-momentum (p=γmv) into E2=m2c4+p2c2, you'll end up at E=γmc2.
 
I get it now, but, if you we're traveling near the speed of light and needed the Lorentz factor, would you make it E2=(mγ)2c4+(mvγ)c2 since you need to put in for relativistic mass in both places?
 
Antuanne said:
I get it now, but, if you we're traveling near the speed of light and needed the Lorentz factor, would you make it E2=(mγ)2c4+(mvγ)c2 since you need to put in for relativistic mass in both places?

No, in the formula E2=m^2c^4+p^2c^2, m is rest mass (or invariant mass). In substituting for momentum, it is better to just treat p=γmv as a definition of momentum, not as 'relativistic mass' times velocity.
 
Antuanne said:
I get it now, but, if you we're traveling near the speed of light and needed the Lorentz factor, would you make it E2=(mγ)2c4+(mvγ)c2 since you need to put in for relativistic mass in both places?

No. The m in E2=(mc2)2 + p2c2 is the rest mass.

One of the advantages of this formulation is that it works for photons and other massless particles as well.
 
That makes sense, but in the simplified thing E=mγc2, where does the γ come from then?
 
Antuanne said:
That makes sense, but in the simplified thing E=mγc2, where does the γ come from then?

mc^2 is rest energy. mγc^2 is total energy, including kinetic energy. Not quite sure what you are asking. In Newtonian mechanics, do you ask: where does the 1/2 come from in:

KE = (1/2) mv^2 ?
 
What I'm asking is what is the equation E2=m2c4+p2c2 used for if E=mγc2 is used for total energy? And is the γ in the just there for relativistic mass or what is that there for?
 
Antuanne said:
That makes sense, but in the simplified thing E=mγc2, where does the γ come from then?
It is always there. But if you are at rest, the gamma factor is 1 and it reduces to the famous form. If you are traveling at lightspeed then gamma is infinite, but m is zero and you need to use the other form and a different definition of momentum - p=2pi hk.
 
  • #10
Ibix said:
It is always there. But if you are at rest, the gamma factor is 1 and it reduces to the famous form. If you are traveling at lightspeed then gamma is infinite, but m is zero and you need to use the other form and a different definition of momentum - p=2pi hk.

Normally, for massless particles traveling at c, you simply use p=E/c.
 
  • #11
Antuanne said:
What I'm asking is what is the equation E2=m2c4+p2c2 used for if E=mγc2 is used for total energy? And is the γ in the just there for relativistic mass or what is that there for?

The two equations are equivalent for particles with non-zero rest mass. Use whichever you like the look of better. However, the longer form is also useful for massless particles, albeit with a different expression for momentum.

The gamma isn't "for" anything. Some people do like to define a "relativistic mass" and make the relativistic equations look like the Newtonian ones. Consensus around here is that this is not helpful - for example you need two different relativistic masses to deal with force, and the acceleration is not parallel to the force (in general) anyway. Better to acknowledge that from the beginning.

The gamma is a consequence of being in a universe with a Minkowski space-time. It is not a modification to Newton. If you wish to recover the low velocity limit, do a binomial expansion of gamma and neglect terms of order v4 and higher. But you can't get from Newton to Einstein that way.

Does that make some kind of sense?
 
  • #12
Do E2=m2c4+p2c2 and E=mγc2 give you the same answer, because, it doesn't seem like they do?
 
  • #13
Antuanne said:
Do E2=m2c4+p2c2 and E=mγc2 give you the same answer, because, it doesn't seem like they do?

Of course they do. Just plug p=mγv in and you get E=mγc2 after algebra.
 
  • #14
Antuanne said:
Do E2=m2c4+p2c2 and E=mγc2 give you the same answer, because, it doesn't seem like they do?

They do. For p2, just substitute m2v2γ2 = m2c4(v/c)2γ2
 
  • #15
But E2=m2c4-p2c2 has v velocity in p so where does that go?
 
Last edited:
  • #16
Did you try the algebra?

Here are a few stages along the way. Try to fill in the gaps.

E^2 = (mc^2)^2 + m^2γ^2v^2c^2

= (mc^2)^2 ( 1 + v^2/(c^2 - v^2) )

= (mc^2)^2 (c^2 / (c^2 - v^2) )

then E = mγc^2
 
  • #17
I still can't figure out how to factor or whatever your doing to get to that!
 
  • #18
Antuanne said:
I still can't figure out how to factor or whatever your doing to get to that!

Don't take this wrong, but while SR needs no higher math, it needs basic facility with algebra. It would be much better for you to review algebra and work it out for yourself than for me fill in one or two more steps between each posted intermediate result.
 
  • #19
Antuanne, don't forget that\gamma = \frac{1}{\sqrt{1 - \frac{v^2}{c^2}}}You will need to use that at some point.
 
  • #20
The OP won't be coming back.
 

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