Exploring the Mass Increase of Accelerated Particles at the LHC

In summary, the conversation discusses the concept of mass in relation to the Large Hadron Collider (LHC). It is debated whether particles experience a mass increase when accelerated in the LHC and whether this is a result of the Special Theory of Relativity. It is clarified that the term "relativistic mass" is not commonly used in physics and that the correct concept is the invariant mass, which is a constant property of a particle. The conversation also discusses the relationship between mass and energy and the use of different notations.
  • #1
Force1
Is it proper to say that when the LHC accelerates particles, those particles experience a mass increase? What is the Special Relativity explanation of the mass increase, i.e. do the particles have increased mass when observed in the rest frame of the detector or do the particles have the same mass and greater kinetic energy in the frame of the detector?
 
Physics news on Phys.org
  • #2
Force1 said:
Is it proper to say that when the LHC accelerates particles, those particles experience a mass increase?

It depends on which definition of "mass" you use.

do the particles have increased mass when observed in the rest frame of the detector

This is a correct statement for the "relativistic mass" that most pop-science books and some introductory physics textbooks talk about, but relatively few physicists use.

or do the particles have the same mass and greater kinetic energy in the frame of the detector?

This is a correct statement for the "invariant mass" (usually called "rest mass" in pop-science books and some intro physics textbooks) that most physicists mean when they say simply "mass."
 
  • #3
jtbell said:
It depends on which definition of "mass" you use.
I should have said relativistic mass then and physicists would say what, apparent mass?
This is a correct statement for the "relativistic mass" that most pop-science books and some introductory physics textbooks talk about, but relatively few physicists use.

This is a correct statement for the "invariant mass" (usually called "rest mass" in pop-science books and some intro physics textbooks) that most physicists mean when they say simply "mass."
OK, so can we say that the relativistic or apparent mass (if that term is correct) of the particles in the detector is increased by the kinetic energy added by acceleration in separate frames, different from the frame of the detector, and when we view the particles in the frame of the detector the difference between rest mass and apparent mass is the kinetic energy?
 
  • #4
Force1 said:
I should have said relativistic mass then and physicists would say what, apparent mass?
The reason people eventually gave up on the concept of "relativistic mass" is precisely because it is not "apparent" ! There is nothing more than [itex]E^2=p^2c^2+m^2c^4[/itex] and Lorentz transformation of [itex](E,p)[/tex] leaving [itex]m[/itex] fixed. The "relativistic mass" is the result of multiplying the mass by the Lorentz dilatation factor [itex]\gamma=\frac{1}{\sqrt{1-\beta^2}}[/itex] "as if" the mass were a time-component, but in fact it is not, the energy is a time-component and it happens to be mass only when the mass is at rest. The "relativistic mass" is the equivalent mass an object at rest would have corresponding to the true total energy of the moving mass.

In fact, wikipedia reproduces an interesting historical comment by Einstein. I did not read the article in details.
 
  • #5
Force1 said:
I should have said relativistic mass then and physicists would say what, apparent mass?

Most physicists, I think, would say "energy." There is nothing massy about "relativistic mass."
 
  • #6
humanino said:
The reason people eventually gave up on the concept of "relativistic mass" is precisely because it is not "apparent" ! There is nothing more than [itex]E^2=p^2c^2+m^2c^4[/itex] and Lorentz transformation of [itex](E,p)[/tex] leaving [itex]m[/itex] fixed. The "relativistic mass" is the result of multiplying the mass by the Lorentz dilatation factor [itex]\gamma=\frac{1}{\sqrt{1-\beta^2}}[/itex] "as if" the mass were a time-component, but in fact it is not, the energy is a time-component and it happens to be mass only when the mass is at rest. The "relativistic mass" is the equivalent mass an object at rest would have corresponding to the true total energy of the moving mass.

In fact, wikipedia reproduces an interesting historical comment by Einstein. I did not read the article in details.
So for physicists at the LHC, the mass of the particles they view in the detector are total energy divided by the speed of light squared. The term relativistic is a point of contention in that relativistic mass is not a fundamental concept of the theory of GR spacetime, although mistakenly used that way by some. “There is disagreement over whether the concept is pedagogically useful”, but most or many physicists have stopped or rarely use the term “relativistic” in circumstances like with the LHC? Is that correct?
 
  • #7
Force1 said:
So for physicists at the LHC, the mass of the particles they view in the detector are total energy divided by the speed of light squared.
Certainly not, unless they did not evolve for 50 years. The mass is a constant, similar to the electric charge, caracteristic of a particle properties under space-time symmetry (Loretnz group representation). Please read https://www.worldscientific.com/phy_etextbook/6833/6833_02.pdf on the question, which you could have found for instance from wikipedia.
 
Last edited by a moderator:
  • #8
humanino said:
Certainly not, unless they did not evolve for 50 years. The mass is a constant, similar to the electric charge, caracteristic of a particle properties under space-time symmetry (Loretnz group representation). Please read https://www.worldscientific.com/phy_etextbook/6833/6833_02.pdf on the question, which you could have found for instance from wikipedia.
From the PDF:

E sub o=mc^2 (1)

E=mc^2 (2)

E^2-p^2c^2=m^2c^4 (5)

P=v E/c^2 (6)

“Thus we obtain in the nonrelativistic limit the well known Newtonian equations for momentum and kinetic energy. This means that m in equation 5 is the ordinary Newtonian mass. Hence, if I were to use m sub o instead of m, the relativistic and nonrelativistic notation would not match.”

“If the notation m sub o and the term ‘rest mass’ are bad, why then are the notation E sub o and the term ‘rest energy’ good? The answer is, because mass is a relativistic invariant and is the same in different reference systems, while energy is the fourth component of a four-vector (E,p) and is different in different reference systems. The index 0 in E sub o indicates the rest system of the body.”

“Let us look again at the equations 5 and 6, and consider them in the case when m=0, the extreme ‘anti-Newtonian’ case. We see that in this case the velocity of the body is equal to that of light: v=c in any reference system. There is no rest frame for such bodies. They have no rest energy; their total energy is purely kinetic."

So from that PDF, “equations 5 and 6 describe the kinematics of a free body for all velocities from 0 to c, and equation 1 follows from them directly. Every physicist who knows special relativity will agree on this.”

“On the other hand, every physicist and many nonphysicists are familiar with ‘the famous Einstein formula E=mc^2.’ But it is evident that equations 1 and 2, E sub o=mc^2 and E=mc^2, are absolutely different. According to equation 1, m is constant and the photon is massless. According to equation 2, m depends on energy (on velocity) and the photon has mass m=E/c^2.”

So (5) and (6) give us equation 1 which is one of Einstein’s great discoveries, energy is equal to rest mass times the speed of light when velocity and momentum are 0, i.e. Newtonian and nonrelativistic. But as Einstein said in a letter to Lincoln Barnett, 19 June 1948, “It is not good to introduce the concept of mass M=m/(1-v^2/c^2)^1/2 of a moving body for which no clear definition can be given. It is better to introduce no other mass concept than the ‘rest mass’ m. Instead of introducing M it is better to mention the expression for the momentum and energy of a body in motion.”

So can you say how the physicist at the LHC would describe the mass/energy of the accelerated particles? Is it simply that they would refer to the energy of the particles and not m, not M, but total energy?
 
Last edited by a moderator:
  • #9


BuddyPal said:
I watched a video on a large hadron collider (LHC), and it mentioned that the protons get much much heavier (relative to their initial weight) when they approach the speed of light. How does this happen? How does the energy create protons,
Who said energy creates protons?
BuddyPal said:
I thought matter cannot be created nor destroyed, only change form, but how does energy spawn matter?
In this case it doesn't, it just increases mass as they are both equivalent. But in general you can create matter+antimatter just from energy.
 
  • #10
Force1 said:
So can you say how the physicist at the LHC would describe the mass/energy of the accelerated particles? Is it simply that they would refer to the energy of the particles and not m, not M, but total energy?
Again, in the modern point of view there is one mass and it is constant. It is a caracteristic of the particle, it defines what we call a particle (from a representation of the Lorentz group). The total energy of the particle includes kinetic energy, and this energy can be arbitrarily high (at least without taking into account gravity, otherwise one may hit a stability limit and form a black-hole). When we accelerate a particle, we simply increase its kinetic energy.
 
  • #11
humanino said:
Again, in the modern point of view there is one mass and it is constant. It is a caracteristic of the particle, it defines what we call a particle (from a representation of the Lorentz group). The total energy of the particle includes kinetic energy, and this energy can be arbitrarily high (at least without taking into account gravity, otherwise one may hit a stability limit and form a black-hole). When we accelerate a particle, we simply increase its kinetic energy.
To test my understanding let me say it; The physicists at the LHC would say that a particle from the representation of the Lorentz group has one mass and that is the rest mass as in E sub o = rest mass times the speed of light squared, and the total energy of said particle would be the energy of the rest mass plus the kinetic energy added by accelerating said particle which could be extremely high at relativistic speeds. Is that correct?

If not I want to keep trying :). But if that is correct, then you mentioned "without taking into consideration gravity". How would gravity change things and can you mention something about the stability limit relative to a black hole forming :.
 
  • #12
Force1 said:
Is that correct?
I think so, yes.
Force1 said:
How would gravity change things and can you mention something about the stability limit relative to a black hole forming :.
That's a qualitative guess that I made mostly to illustrate that the "energy can increase without limit" is a "for all purpose" statement concerning protons at the LHC. Beyond experimental constraints, more serious care must be taken. A reasonable guess is that from the atom scale to the LHC scale is an increase which is (much) less than the necessary increase to go from LHC to conventional gravity scale scenario. However, it could also be, in more exotic scenarios, that the gravity scale occurs sooner. Since we do not know the correct quantum theory for gravity, there is room for improvisation. It is in any case fairly certain that if you keep increasing the particle's energy, gravity will come into the game at some point. The formation of a black-hole is a dramatic example. It can not occur merely from kinematics BTW. We would need our putative very very very energetic particle to interact with something around.
 
  • #13
humanino said:
I think so, yes.
That's a qualitative guess that I made mostly to illustrate that the "energy can increase without limit" is a "for all purpose" statement concerning protons at the LHC. Beyond experimental constraints, more serious care must be taken. A reasonable guess is that from the atom scale to the LHC scale is an increase which is (much) less than the necessary increase to go from LHC to conventional gravity scale scenario. However, it could also be, in more exotic scenarios, that the gravity scale occurs sooner. Since we do not know the correct quantum theory for gravity, there is room for improvisation. It is in any case fairly certain that if you keep increasing the particle's energy, gravity will come into the game at some point. The formation of a black-hole is a dramatic example. It can not occur merely from kinematics BTW. We would need our putative very very very energetic particle to interact with something around.
Does this qualitative guess relate to the conceivable presence of an amount of energy in a particle that reaches some as yet undefined energy limit beyond which there could be gravitational events that we don't yet understand?
 
  • #14
Force1 said:
conceivable presence of an amount of energy in a particle that reaches some as yet undefined energy limit beyond which there could be gravitational events that we don't yet understand?
Almost. I was trying to convey that this energy is not really intrinsic to the particle : it is in the velocity difference between the particle and us (or the lab).
 

1. What is the LHC?

The LHC (Large Hadron Collider) is a particle accelerator located at the European Organization for Nuclear Research (CERN) in Geneva, Switzerland. It is the world's largest and most powerful particle accelerator, used to study the fundamental building blocks of matter and the forces that govern them.

2. What is meant by "particle mass increase" at the LHC?

The LHC is able to accelerate particles to incredibly high speeds, close to the speed of light. As particles move at these high speeds, they gain energy. This energy can then be converted into mass, according to Einstein's famous equation E=mc². This is what is meant by "particle mass increase" at the LHC.

3. How does the LHC measure particle mass increase?

The LHC uses a variety of detectors, such as the ATLAS and CMS detectors, to measure the properties of particles produced during collisions. These detectors can measure the energy and momentum of particles, which can then be used to calculate their mass.

4. Why is the study of particle mass increase important?

The study of particle mass increase at the LHC helps us understand the fundamental properties of matter and the forces that govern the universe. It also allows us to test and refine our current theories and models of particle physics, such as the Standard Model. This knowledge can have implications for various fields, including technology, medicine, and our understanding of the universe.

5. What have been some significant findings related to particle mass increase at the LHC?

One of the most significant findings at the LHC related to particle mass increase was the discovery of the Higgs boson in 2012. This particle was predicted by the Standard Model and its discovery confirmed our understanding of how particles acquire mass. Additionally, the LHC has also provided evidence for the existence of other particles, such as the top quark and the W and Z bosons, which have increased our understanding of particle mass and interactions.

Similar threads

  • Special and General Relativity
Replies
11
Views
2K
  • Special and General Relativity
3
Replies
102
Views
3K
  • Special and General Relativity
5
Replies
167
Views
4K
  • Special and General Relativity
Replies
4
Views
1K
  • Special and General Relativity
Replies
16
Views
1K
  • Special and General Relativity
2
Replies
36
Views
2K
  • Special and General Relativity
Replies
6
Views
831
  • Special and General Relativity
Replies
5
Views
434
  • Special and General Relativity
Replies
9
Views
977
  • Special and General Relativity
Replies
33
Views
1K
Back
Top