On why massless particles move at the speed of light

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Discussion Overview

The discussion centers around the question of why massless particles must move at the speed of light, specifically within the framework of special relativity (SR). Participants explore various derivations, definitions, and implications related to the properties of massless particles, including their energy and momentum characteristics.

Discussion Character

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

Main Points Raised

  • One participant presents a derivation suggesting that as the rest energy (E0) approaches zero, the velocity (v) of a particle must equal the speed of light (c).
  • Another participant emphasizes that the rest mass of a particle is defined by the norm of its momentum 4-vector, arguing that massless particles must either travel at the speed of light or have no energy and momentum.
  • A different viewpoint proposes that the momentum vector can be defined in a way that shows massless particles must travel at the speed of light, without needing to clarify the definition of the momentum 4-vector.
  • One participant challenges the assumption of invariant mass, stating that the relationship P^2 = m^2 should be seen as a consequence rather than an assumption, and questions the implications for Lagrangian and Hamiltonian formulations when mass is zero.
  • Another participant raises concerns about how to justify the relationship between energy and momentum for massless particles without leading to contradictions, particularly when considering the implications of zero mass.

Areas of Agreement / Disagreement

Participants express differing views on the definitions and implications of massless particles and their relationship to the speed of light. There is no consensus on the best approach to derive or justify these properties, and multiple competing perspectives remain throughout the discussion.

Contextual Notes

Some participants note limitations in their arguments, such as the need for clearer definitions of the momentum 4-vector and the potential for contradictions when discussing zero mass. The discussion also reflects a variety of assumptions and interpretations regarding the underlying physics.

PAllen
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On "why massless particles move at the speed of light"

It has come up a few times whether you can derive that massless particles must go the speed of light, strictly using SR. Bcrowell proposed a way that some argued against. I have a different tack for consideration.

I recently derived that, for any particle with E0 (rest energy) > 0, the following is true:

(1 - v^2/c^2) = 1 - KE / (KE + E0)

From this you can say:

1) limit as E0 -> 0 leads to v=c
2) If there is to be such a thing as a particle with E0=0 and nonzero KE, and if it should be consistent with the SR, then this relation directly requires that v=c.
 
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PAllen said:
It has come up a few times whether you can derive that massless particles must go the speed of light, strictly using SR. Bcrowell proposed a way that some argued against. I have a different tack for consideration.

I recently derived that, for any particle with E0 (rest energy) > 0, the following is true:

(1 - v^2/c^2) = 1 - KE / (KE + E0)

From this you can say:

1) limit as E0 -> 0 leads to v=c
2) If there is to be such a thing as a particle with E0=0 and nonzero KE, and if it should be consistent with the SR, then this relation directly requires that v=c.

That should be:

sqrt(1 - v^2/c^2) = 1 - KE / (KE + E0)
 


The rest mass of a particle is defined to be the norm of its momentum 4-vector. There are only two kinds of vectors that have zero norm: null vectors and the zero vector. So a particle which is massless either travels at the speed of light or carries no energy and momentum at all.
 


Bill_K said:
The rest mass of a particle is defined to be the norm of its momentum 4-vector. [...]

How would you unambiguously define the <momentum 4-vector> ?
 


How would you unambiguously define the <momentum 4-vector> ?
It doesn't have to be unambiguous! The momentum vector for a particle is P = (α, αv) for some α, I don't care what. But so long as the norm is zero, P·P = 0, then v = c for any α, which is all we wanted to show. You guys are making this way too hard.
 


dextercioby said:
How would you unambiguously define the <momentum 4-vector> ?

Let's start with one spatial dimension. Then

given the Lagrangian L(x, v) where v = dx/dt

define

<br /> p = \frac{\partial L}{\partial v}<br />

This serves as an adequate definition of momentum.

A Lagrangian is defined as "good" if the equations of motion

<br /> \frac{dp}{dt} = \frac{\partial L}{\partial x}<br />

are correct, i.e. match observation. And E would be given by

E = p*v - L (more generally the sum over i of p_i *v_i - L when you have more than one dimension)
 


The point I was trying to make is that postulating the existence of rest/invariant mass, assuming it nonzero and the form of the Lagrangian of a free particle of rest mass m_0 leads to P^2 = m^2. Point: P^2 = m^2 is a consequence, not an assumption/definition/axiom.

Assume it in reverse, then what are the Lagrangian & Hamiltonian formulations of the theory with P^2 =0, thus with invariant mass = 0 ?
 


Bill_K said:
The rest mass of a particle is defined to be the norm of its momentum 4-vector. There are only two kinds of vectors that have zero norm: null vectors and the zero vector. So a particle which is massless either travels at the speed of light or carries no energy and momentum at all.

The aim is was to justify this with the fewest assumptions and without apparent division by zero that could be criticized by a skeptical newbie. Playing skeptical newbie, all you've got from this is:

E^2=P^2 c^2

So now newbie asks, isn't P = m gamma v = 0 if m=0? Contradiction (since E assumed nonzero)?
So now the problem has been transposed to showing why P=E/c implies speed is c.

[Edit: Of course, one way to do this is to write the general:

P = Ev/c^2 ; then the requirement that P = E/c implies v=c. But with this addition I don't see much superiority to this approach. ]
 
Last edited:

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