B Relativistic Mass of Sub-Atomic Particles: What Does it Mean?

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  • #51
1977ub said:
When, for example, I reach in and then move half the mass to one end and half the mass to the other end, and then close it up again, there will be a greater [...] mass since we have increased the gravitational potential energy.

You don't move mass. You move stuff, like in this case maybe you are moving matter? And if that matter is attracted to the other half of the matter in the box, then when you separate the two halves you increase the potential energy and thus the mass, since the two are equivalent.
 
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  • #52
If I open the box and shoot light at the box, this will increase the effective mass if any of it "sticks" in some way - chemically or as heat.
 
  • #53
1977ub said:
Some of the things I can do to what is in there which increase effective mass are clearly a matter of *adding* *something*
Any method of increasing the mass involves adding four-momentum. Whether you call that *something* or not is semantics. The key question is whether or not four-momentum was added, not whether that four-momentum is attached to some specific thing.
 
  • #54
I'm focusing on where the energy has to come from as well. Presumably after I reach into the box and move the different parts of the mass to different corners, this will have taken my own chemical energy in my muscles. So this will reduce the mass-energy of my body.
 
  • #55
1977ub said:
I'm focusing on where the energy has to come from as well. Presumably after I reach into the box and move the different parts of the mass to different corners, this will have taken my own chemical energy in my muscles. So this will reduce the mass-energy of my body.
Yes, but because you aren't part of the box this reduction is irrelevant to the mass of the box.
 
  • #56
1977ub said:
I'm focusing on where the energy has to come from as well.
It doesn't matter where it comes from, what form it is in when it enters the box, or what it turns into within the box. That is the elegance of conservation principles ... the details do not matter.
 
  • #57
from wikipedia: "the mass of an atomic nucleus is less than the total mass of the protons and neutrons that make it up, but this is only true after this energy from binding has been removed in the form of a gamma ray (which in this system, carries away the mass of the energy of binding). This mass decrease is also equivalent to the energy required to break up the nucleus into individual protons and neutrons (in this case, work and mass would need to be supplied). Similarly, the mass of the solar system is slightly less than the sum of the individual masses of the sun and planets."
https://en.wikipedia.org/wiki/Mass–energy_equivalence

I'm not sure what the phrase "only true after" gamma ray has been removed. Will the mass of an intact nucleus be found to be less than the sum of the protons and neutrons ?
 
  • #58
1977ub said:
Will the mass of an intact nucleus be found to be less than the sum of the protons and neutrons ?

Yes. The article's phrasing is clumsy. What they are trying to say is that, in order to make an intact nucleus out of a bunch of free protons and neutrons, you have to remove energy from the protons and neutrons. Gamma rays are a common way for energy to be carried off from nuclear reactions, but there is no single nuclear reaction that will make, for example, an iron-56 nucleus out of 26 free protons and 30 free neutrons; it would take a long series of reactions, some of which would have products other than gamma rays. So the article is not describing a process that actually happens; it's just trying to make a general point, and doing it in a confusing way.
 
  • #59
1977ub said:
I'm not sure what the phrase "only true after" gamma ray has been removed. Will the mass of an intact nucleus be found to be less than the sum of the protons and neutrons ?
I think the article is idealising the process as

1. You have protons and neutrons.
2. You fuse them.
3. They emit a gamma ray.

Step 2 would be a nucleus in an excited state. Step 3 would be a nucleus in its ground state. Step 2 would have the same mass as the particles in step 1. Step 3 would have a lower mass as long as you let the photon escape.

As Peter says, it doesn't actually happen in three easy steps like that.
 
  • #60
Of course I agree that it does not happen in easy steps as the Wiki article says. However, to pile on a bit to the question "does the nucleus have less mass than the sum of the proton and neutron masses?" a clear indication of this should be the fact that the proton mass in atomic units is 1.007u and the neutron mass 1.009u. The atomic mass unit is defined as 1/12 of the mass of a unbound neutral carbon-12 atom and clearly the mass of 6 protons and 6 neutrons is larger.
 
  • #61
1977ub said:
Will the mass of an intact nucleus be found to be less than the sum of the protons and neutrons ?
Yes
 
  • #62
Also I guess I forgot gravitational potential energy is negative - in other words, you open the box, move things from the center out to the edges of the box, then close it. It is now found to have less inertial and gravitational mass.
 
  • #63
1977ub said:
in other words, you open the box, move things from the center out to the edges of the box, then close it. It is now found to have less inertial and gravitational mass.
You have that backwards.
 
  • #64
If the solar system is found to have less mass than the individual bodies, is this not due to the gravitational potential energy of their being separated in space?
 
  • #65
1977ub said:
If the solar system is found to have less mass than the individual bodies, is this not due to the gravitational potential energy of their being separated in space?

No, it's due to the (negative) gravitational potential energy because they are not separated a lot more in space--i.e., because they are in a bound system with a finite size that is small on cosmological scales, instead of being spread out very far away from each other.

1977ub said:
you open the box, move things from the center out to the edges of the box, then close it. It is now found to have less inertial and gravitational mass.

No, it will have more, because the things in the box are separated by a larger distance than they were before. That means you added energy to the box in order to move them apart.

If you want to decrease the inertial and gravitational mass of the box, without removing any of the objects inside, you would need to open the box and remove energy from it, bringing the objects inside closer together (i.e., making them more tightly bound) in the process.
 
  • #66
PeterDonis said:
No, it's due to the (negative) gravitational potential energy because they are not separated a lot more in space--i.e., because they are in a bound system with a finite size that is small on cosmological scales, instead of being spread out very far away from each other.
No, it will have more, because the things in the box are separated by a larger distance than they were before. That means you added energy to the box in order to move them apart.

If you want to decrease the inertial and gravitational mass of the box, without removing any of the objects inside, you would need to open the box and remove energy from it, bringing the objects inside closer together (i.e., making them more tightly bound) in the process.

Ok then I'm back with my nagging biases. To make things more tightly bound, does this not imply perhaps that electromagnetic energy was contributed?

Aren't all forms of potential energy related to fundamental forces?
 
  • #67
1977ub said:
To make things more tightly bound, does this not imply perhaps that electromagnetic energy was contributed?

You don't "contribute" energy to make things more tightly bound. You take away energy. As for what form the energy taken away can take, that depends on the details of how you do it. In natural processes like the formation of stars or planetary systems, electromagnetic radiation is typically the way that energy is taken away from the system to allow it to become more tightly bound.
 
  • #68
1977ub said:
make things more tightly bound, does this not imply perhaps that electromagnetic energy was contributed?
It doesn't matter! It can be any form.

1977ub said:
Aren't all forms of potential energy related to fundamental forces?
It doesn't matter.

The form of the energy is an irrelevant detail, all that matters is that it is a component of the conserved four-momentum. I feel like you are just ignoring this key fact. The whole purpose of establishing conservation laws is because once you do so you don't need to worry about the details.
 
  • #69
PeterDonis said:
You don't "contribute" energy to make things more tightly bound. You take away energy. As for what form the energy taken away can take, that depends on the details of how you do it. In natural processes like the formation of stars or planetary systems, electromagnetic radiation is typically the way that energy is taken away from the system to allow it to become more tightly bound.

Ok. So my impression seems correct. You send electromagnetic energy into the box and it becomes warmer and heavier, or more spread out and heavier, or starts moving around and gets heavier. What ways are there to remove energy / mass from a system without particles (massive or photons) being removed?
 
  • #70
1977ub said:
You send electromagnetic energy into the box and it becomes warmer and heavier, or more spread out and heavier, or starts moving around and gets heavier.

Yes.

1977ub said:
What ways are there to remove energy / mass from a system without particles (massive or photons) being removed?

At the fundamental level, there are only four interactions known (electromagnetic, weak, strong, and gravitational), and only two of them give rise to radiation that can travel long distances (the weak and strong interactions are short range and don't give rise to radiation). So the only other option besides the ones you list is gravitational radiation. But gravitational radiation from almost any system will be so much weaker than electromagnetic radiation that it can be ignored for all practical purposes. (The only exceptions are the kinds of systems we have detected gravitational waves from--black hole mergers, neutron stars merging to form black holes, etc.)
 
  • #71
1977ub said:
Also I guess I forgot gravitational potential energy is negative - in other words, you open the box, move things from the center out to the edges of the box, then close it. It is now found to have less inertial and gravitational mass.
That's not what negative potential energy means. The negative potential energy just means that we're using the arbitrary (but very convenient, which is why we do it) convention that the potential energy at infinite separation is zero. Whether the potential energy is negative or positive is irrelevant. What matters is whether the change in potential energy is positive or negative as you move things away from the center; and that change is positive.
 
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  • #72
1977ub said:
What ways are there to remove energy / mass from a system without particles (massive or photons) being removed?
One of the most common ways is for the system to emit electromagnetic radiation. This process cannot be described as photons "being removed".
 
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  • #73
Nugatory said:
One of the most common ways is for the system to emit electromagnetic radiation. This process cannot be described as photons "being removed".

The EM radiation can't leave without going somewhere, right? There have to be photons elsewhere which take this energy on then, right?
 
  • #74
Nugatory said:
That's not what negative potential energy means. The negative potential energy just means that we're using the arbitrary (but very convenient, which is why we do it) convention that the potential energy at infinite separation is zero. Whether the potential energy is negative or positive is irrelevant. What matters is whether the change in potential energy is positive or negative as you move things away from the center; and that change is positive.

Is this convention really arbitrary in the context of reckoning a system's rest energy?
 
  • #75
1977ub said:
The EM radiation can't leave without going somewhere, right? There have to be photons elsewhere which take this energy on then, right?
Photons aren't what you think they are; and you should reread post #39 of this thread.
 
  • #76
Nugatory said:
Photons aren't what you think they are; and you should reread post #39 of this thread.

I understand plenty about photons, I think. I reread post #39. I don't think I have any further questions about this.
 
  • #77
1977ub said:
If the solar system is found to have less mass than the individual bodies, is this not due to the gravitational potential energy of their being separated in space?

Not separated, collected.
 
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  • #78
@1977ub

Mass is just a measure of how much energy a system has in its rest frame: ##E_0 = mc^2##, where ##E_0## is the system's rest energy.

What contributes to a system's rest energy? Answer: all of the energy "internal" to the system.

Say that the system is full of gas molecules. To calculate the system's rest energy (i.e., its mass), we must add up all of the "internal" energy contributions: the kinetic energies of the gas molecules (as measured in the system's rest frame, of course), the potential energy associated with their relative positions, and also the rest energies (masses) of the individual particles.

Then we could "zoom in" on a single molecule and itemize its rest energy as the sum of the kinetic, potential, and rest energies associated with its constituent atoms. We could "zoom in" on a single atom in the molecule and itemize its rest energy as the sum of the kinetic, potential, and rest energies associated with its subatomic particles.

Etc.

The potential-energy contributions associated with the relative positions of a system's constituents can be positive or negative, depending on whether the force in question is repulsive (positive) or attractive (negative). The potential-energy contributions approach zero in the limit that the system's constituents are infinitely far apart.
 
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  • #79
SiennaTheGr8 said:
@1977ub

To calculate the system's rest energy (i.e., its mass), we must add up all of the "internal" energy contributions ...

(or we can just weigh it) :wink:
 
  • #80
SiennaTheGr8 said:
Is this convention really arbitrary in the context of reckoning a system's rest energy?
You're right, it's not arbitrary for that purpose. I was trying/hoping to avoid that subtlety because much of the recent discussion has been about how the rest energy changes as energy enters and leaves the system; and because (as you pointed out while I was writing this) we can jus weigh the system to establish its rest energy.
 
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  • #81
SiennaTheGr8 said:
What contributes to a system's rest energy? Answer: all of the energy "internal" to the system.

SiennaTheGr8 said:
The potential-energy contributions associated with the relative positions of a system's constituents can be positive or negative, depending on whether the force in question is repulsive (positive) or attractive (negative). The potential-energy contributions approach zero in the limit that the system's constituents are infinitely far apart.

SiennaTheGr8 said:
(or we can just weigh it)

Since we're having this discussion in the relativity forum (as opposed to the classical physics forum), it's worth pointing out that, in GR, all of these statements have limitations.

First, in relativity, the idea of determining a system's rest energy by adding up all of the "internal" contributions is formalized in what is called the Komar energy (more usually called "Komar mass", because in relativity energy and mass are just different units for the same quantity, and the term "mass" is more usual in the GR literature--as opposed to, say, the QFT literature, where the term "energy" or even "momentum" is more usual). The basic idea is that you integrate the stress-energy tensor over all of space, paying appropriate attention to the fact that spacetime is curved.

However, the Komar energy integral is only well-defined in a limited class of spacetimes, the stationary spacetimes--which are basically the ones in which there is a notion of "space" that is independent of "time" (I use the quotes because for precision these terms should be formalized and made precise, and they can be, but there are a lot of pitfalls lurking for the unwary in doing so). It turns out that these are also the only spacetimes in which there is a well-defined concept of "gravitational potential energy"; and it turns out that, in these spacetimes, the Komar energy integral is what you would expect it to be for a bound system, taking the (negative) contribution of gravitational potential energy into account (basically because taking proper account of spacetime curvature, in such spacetimes, is taking the contribution of gravitational potential energy into account).

Interestingly, the other notion of total energy you mention--just weigh the system--corresponds, if we take "weigh" to mean "determine by measurements purely external to the system", to a different concept of energy in relativity--actually, to two of them, called the ADM energy and the Bondi energy. These are well-defined for a different limited class of spacetimes, the asymptotically flat spacetimes--which are basically the ones which describe an isolated system surrounded by empty space. The difference between them is that the ADM energy never changes--even for a system that emits radiation that escapes to infinity. (The reason is that, at any finite time, the radiation has only traveled some finite distance from the system, because of the finite speed of light, so it is always present somewhere in the spacetime, and the ADM energy will therefore include it.) The Bondi energy was developed in order to make rigorous the idea that systems which emit radiation away to infinity lose energy: basically, the Bondi energy is the ADM energy minus whatever energy is carried away to infinity by radiation. This means that the Bondi energy, unlike the ADM energy, can change with "time" (again, this term needs to be properly formalized and made precise) as a system radiates and becomes more tightly bound.

For the even more limited class of spacetimes which have both properties--stationary and asymptotically flat--the Komar energy and the ADM energy are the same, so everything fits together consistently. But there are also important spacetimes--such as the FRW spacetimes used in cosmology--where none of these concepts of energy are well-defined, and so none of the ideas we have been talking about in this discussion apply.
 
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  • #82
Thanks, @PeterDonis. Very informative write-up, there.
 
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