I Can an atom absorb a photon, yet its total kinetic energy is decreased?

Click For Summary
An atom can absorb a photon, which increases its total energy, but this does not necessarily mean its kinetic energy must increase. When a photon is absorbed, the entire system of the atom, including the nucleus and electrons, experiences changes in energy states. If the atom is moving in the opposite direction of the incoming photon, its kinetic energy can decrease due to momentum conservation. The potential energy is a property of the atom as a whole, not just the electron. Modern quantum theories provide a more accurate understanding of these interactions than older models like Bohr's theory.
  • #31
avicenna said:
"First, it is not the electron that absorbs the photon, it is the system nucleus + electron."

But the wiki seems to state otherwise:
(Bohr's theory)
"Electrons can only gain and lose energy by jumping from one allowed orbit to another, absorbing or emitting electromagnetic radiation with a frequency determined by the energy difference of the levels according to the Planck relation:
Bohr's theory is outdated for 98 years now. To be honest, it never was a real theory, and it worked thanks to the shear luck of the large dynamical symmetries for the harmonic oscillator as well as the hydrogen atom. For almost everything else it failed dramatically. It even fails on very simple qualitative grounds: The hydrogen atom is not a little disk but a sphere in its ground state as the chemists well know.
 
Physics news on Phys.org
  • #32
avicenna said:
It is just debating on semantics.
It actually isn’t. It has real experimental consequences. If the electron on its own had PE then a free electron could absorb a photon. But we experimentally see that electrons cannot absorb photons, they can only scatter them.

Atoms can absorb them because PE belongs to the atom, but not electrons because they don’t have PE on their own. Since your question is specifically about the absorption of a photon, not only is this distinction not merely semantics, it is directly relevant to the specific question you asked.
 
  • Like
Likes vanhees71, sophiecentaur, hutchphd and 1 other person
  • #33
avicenna said:
Can it happen that this increase in energy result in an increase of its total potential energy = E + Del(potential energy) and its total kinetic energy decreases by Del(potential energy).
For a direct answer to your question see here:

https://physics.stackexchange.com/q...-total-kinetic-energy-decreased/783085#783085

The KE decreases for any $$v<\frac{-E^2-4Em}{E^2+4Em+8m^2}$$
 
  • #34
avicenna said:
It is just debating on semantics.
No, it's not. An isolated electron is physically different from an electron in a bound system. Treating them as though they are the same does not work.

avicenna said:
The textbooks do identity "a potential energy of an electron".
Please give a specific reference, with context. I strongly suspect you will find that the context is an electron in a bound system with a proton or atomic nucleus, and that the context makes it clear that the potential energy is a property of the bound system, not the electron in isolation.

Please do not make further assertions along these lines without taking some time to read valid references carefully. This point has already been belabored too long in this thread.
 
  • Like
Likes vanhees71, Lord Jestocost and Dale
  • #35
PeterDonis said:
No, it's not. An isolated electron is physically different from an electron in a bound system. Treating them as though they are the same does not work.Please give a specific reference, with context. I strongly suspect you will find that the context is an electron in a bound system with a proton or atomic nucleus, and that the context makes it clear that the potential energy is a property of the bound system, not the electron in isolation.

Please do not make further assertions along these lines without taking some time to read valid references carefully. This point has already been belabored too long in this thread.
I have never ever said that an electron on its own can have potential energy. I only said it is a matter of semantics whether we associate the amount of energy to the electron or to tha atom(the system). The amount is the same!

From my physics textbook, pg 984:
... The further the electron is from the nucleus, the greater is its potential energy; or less negative is its potential energy.

From: University of Tennessee, Knoxville
http://labman.phys.utk.edu › modules › Electric potential

(Lecture 4: Electrostatic Potential, Electric Energy, eV, Conservative Field, Equipotential Surfaces)

http://labman.phys.utk.edu/phys222core/modules/m2/Electric potential.html#:~:text=The potential energy of the,energy and its potential energy.
Problem solving:
Reasoning:
The force on the electron is the Coulomb force between the proton and the electron. It pulls the electron towards the proton. For the electron to move in a circular orbit, the Coulomb force must equal the centripetal force. We need keqe2/r2 = mv2/r.

Details of the calculation:
mv2 = keqe2/r, so the kinetic energy of the electron is
KE(r) = ½mv2 = ½keqe2/r.
The potential energy of the electron in the field of the positive proton point charge is U(r) = -qeV(r) = - keqe2/r.
The total energy is the sum of the electron's kinetic energy and its potential energy.
KE(r) + PE(r) = -½keqe2/r = (-½) (9*109)(1.60*10-19) /(5.29*10-11) J = -2.18*10-18 J.

Do I need to make further clarifications?
 
  • Skeptical
  • Haha
Likes berkeman and gentzen
  • #36
avicenna said:
I only said it is a matter of semantics whether we associate the amount of energy to the electron or to tha atom(the system). The amount is the same!
The fact that a proton has 2000 times the mass of the electron means that you can treat the proton as 'stationary' in a mechanical collision - but that's all. Your arguing would need to change direction rapidly in the case of a diatomic molecule absorbing a photon which has energy corresponding to a change in vibrational energy. So why not talk in a consistent way, rather than hanging onto a wording that's around 100 years old to back up your preferences?
 
  • #37
PeterDonis said:
Please give a specific reference, with context
The old classic, "My Physics Textbook". :smile: Page 984.

You seem to be getting upset. The problem isn't that the OP hasn't read the answer, it's that he doesn't believe the answer. That's not something we can fix.

Sure, there will likely be negative consequences down the road, but maybe that will provide the necessary impetus for a change of his perspective.
 
  • Like
  • Haha
Likes vanhees71, Bystander, Dale and 2 others
  • #38
avicenna said:
We need keqe2/r2 = mv2/r.

Details of the calculation:
mv2 = keqe2/r, so the kinetic energy of the electron is
KE(r) = ½mv2 = ½keqe2/r.
The potential energy of the electron in the field of the positive proton point charge is U(r) = -qeV(r) = - keqe2/r.
As you mentioned “in the real world” to me earlier, I will do the same here. In the real world people, including textbook authors, often say one thing and do another. Although this author said “energy of the electron” note what they actually did in the math.

First, they used the variable ##r##. In context, ##r## describes the atom, it is not the radius of the electron nor the radius of the nucleus, it is the radius of the atom.

Second, ##m## in the KE formula is constant. If the PE belonged to the electron then as it gained PE it would also gain mass. Since an electron is so small, this would be noticeable, small but noticeable.

So although in English they say “potential energy of the electron” in math they actually do “the potential energy of the atom”.
 
  • Like
Likes mattt, vanhees71 and PeterDonis
  • #39
Dale said:
As you mentioned “in the real world” to me earlier, I will do the same here. In the real world people, including textbook authors, often say one thing and do another. Although this author said “energy of the electron” note what they actually did in the math.

First, they used the variable ##r##. In context, ##r## describes the atom, it is not the radius of the electron nor the radius of the nucleus, it is the radius of the atom.

Second, ##m## in the KE formula is constant. If the PE belonged to the electron then as it gained PE it would also gain mass. Since an electron is so small, this would be noticeable, small but noticeable.

So although in English they say “potential energy of the electron” in math they actually do “the potential energy of the atom”.
I surrender!

My level of physics has not reached the level where the mass of the electron may change. Give me time to do some catch-up!!!
 
  • #40
avicenna said:
I have never ever said that an electron on its own can have potential energy. I only said it is a matter of semantics whether we associate the amount of energy to the electron or to tha atom(the system).
You're quibbling. These two claims are the same, because associating the energy with just the electron is saying that the electron on its own can have potential energy. Which it can't.

avicenna said:
From my physics textbook
Which textbook?

avicenna said:
From my physics textbook, pg 984:
avicenna said:
From: University of Tennessee, Knoxville
As I said, you have to read these sources in context. You're not doing that.

Nobody is disputing the math; that's not the issue. The issue is that it's not "a matter of semantics" what the energy is associated with. It has to be associated with the system--in this case the atom--not just the electron. The quotes you give do not contradict that; they are just being sloppy: because they are using a frame in which the proton is at rest, they are describing the PE as though it belonged to the electron, even though it doesn't. But switch frames and this sloppiness no longer works. The actual physics is that the PE is a property of the system, not the electron, regardless of what sloppiness you can get away with in a particular frame.

As for why the actual physics is important, that should be obvious from the discussion in this thread: it explains why the answer to your original question has to be "no".
 
  • #41
avicenna said:
My level of physics has not reached the level where the mass of the electron may change.
It can't--that is precisely @Dale's point. The electron is not a bound system that can even have potential energy on its own. Its mass is a constant and can't change. Advancing your level of understanding won't change that.
 
  • #42
@avicenna Bohr's theory was meant for electron orbit states around an atom. Imagine a proton without electrons (a H+ ion) absorbing a photon. The proton is moving to the right, the photon to the left. It's simply the law of momentum conservation that the atom will be moving slower after the encounter.

In the case of electrons orbiting an atom moving contrary to an incoming photon: the electron may enter a more excited state, but due to its electronic attraction to the atom core and the gained momentum in contrary direction at first, the atom core will move slightly slower afterwards. The gained energy for the electron is less than the lost kinetic energy of the atom core. The atom's "rest energy" (with the electron still excited) might have increased but its total energy reduced.
 
  • #43
avicenna said:
My level of physics has not reached the level where the mass of the electron may change. Give me time to do some catch-up!!!
The mass of the electron doesn't change, and neither does the mass of the nucleus. This is similar to boosting the Moon into a higher orbit around the Earth. Energy has been added, and thus mass, but the mass of the Moon and the Earth don't change. How could they? An observer on the surface of either body would see no physical change in the body, no temperature increase, nowhere that mass or energy has been added. Therefore it must be the mass of the Earth-Moon system as a whole that changes, not the mass of either body.
 
  • #44
avicenna said:
I have never ever said that an electron on its own can have potential energy. I only said it is a matter of semantics whether we associate the amount of energy to the electron or to tha atom(the system). The amount is the same!
It is not semantics but a basic misunderstanding. In an atom in an energy eigenstate the electrons and the atomic nucleus are in an entangled state and thus inseparable. You have an energy of the atom as a whole. To talk about distribution of this energy to various parts of the atom doesn't make sense.

Amazingly this is not discussed in the textbooks, although it's an (if not the) important feature of quantum theory. See the following AJP paper

https://arxiv.org/abs/quant-ph/9709052
https://doi.org/10.1119/1.18977
 
  • #45
vanhees71 said:
It is not semantics but a basic misunderstanding. In an atom in an energy eigenstate the electrons and the atomic nucleus are in an entangled state and thus inseparable. You have an energy of the atom as a whole. To talk about distribution of this energy to various parts of the atom doesn't make sense.

Amazingly this is not discussed in the textbooks, although it's an (if not the) important feature of quantum theory. See the following AJP paper

https://arxiv.org/abs/quant-ph/9709052
https://doi.org/10.1119/1.18977
Why do you think it's the most important feature of quantum theory?
 
  • #46
If there's one feature which is really "quantum" in contradistinction to "classical physics", it's entanglement, I'd say, but that's of course a pretty subjective opinion.
 
  • #47
vanhees71 said:
If there's one feature which is really "quantum" in contradistinction to "classical physics", it's entanglement, I'd say, but that's of course a pretty subjective opinion.
OK, but would there be any difference from using the usual Schrödinger approach by considering the proton and electron as an entangled state vs. the electron in a coulomb potential?
 
  • #48
The usual Schrödinger approach directly leads to this result. The point is to write the Hamiltonian in terms of center-of-mass and relative coordinates. The center-of-mass motion is free, and the relative-coordinate piece leads to the usual hydrogen atom for a quasiparticle around the center (which is the center of mass of electron and proton) with the reduced mass, ##\mu=m_{\text{e}} m_{\text{p}}/(m_{\text{e}}+m_{\text{p}})##. It's as in classical mechanics (Kepler problem). While a product state in center-of-mass and relative coordinates, rewritten again in electron and proton observables, it's showing that electron and proton are in an entangled state.
 
  • #49
Maybe it's also possible that some exotic particle in high-energy physics can absorb a photon to become a higher-mass particle without the KE or PE changing?
 
  • #50
hilbert2 said:
Maybe it's also possible that some exotic particle in high-energy physics can absorb a photon to become a higher-mass particle without the KE or PE changing?
You would need to be clear what you mean by PE not changing in that case. But yes, in principle that could happen.
 
  • #51
hilbert2 said:
some exotic particle in high-energy physics can absorb a photon to become a higher-mass particle without the KE or PE changing?
If the particle is free, it is impossible for it to absorb a single photon without its momentum (and hence its KE) changing.
 
  • Like
Likes Vanadium 50
  • #52
PeterDonis said:
If the particle is free, it is impossible for it to absorb a single photon without its momentum (and hence its KE) changing.
No. You can change momentum without changing KE. It would be pretty fine tuned though. The momentum would have to start out along e.g. the negative x axis and change to the positive x axis at whatever velocity corresponds to the same KE. There should be one frame where this is true for any absorption by a free particle.
 
  • #53
Dale said:
You can change momentum without changing KE.
Hm, yes, for a very fine-tuned case this is possible.
 
  • #54
PeterDonis said:
Hm, yes, for a very fine-tuned case this is possible.
Yes, not only is it fine tuned, but also I cannot think of any reason why you would use that frame naturally. You would only use it specifically to make this point.
 
  • #55
Since the decay \Sigma^0 \rightarrow \Lambda + \gamma occurs, the inverse process \gamma + \Lambda \rightarrow \Sigma^0 must also occur.

However, both baryons cannot be at rest. There exist a frame where the baryon kinetic energies are the same and a (different) frame where the momentum magnitudes are the same. This example also relies on the baryons being composite particles.
 
  • Like
Likes hilbert2, vanhees71 and Dale

Similar threads

Replies
3
Views
1K
  • · Replies 38 ·
2
Replies
38
Views
6K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 15 ·
Replies
15
Views
3K
Replies
4
Views
1K
  • · Replies 13 ·
Replies
13
Views
2K
Replies
43
Views
5K
  • · Replies 36 ·
2
Replies
36
Views
10K
  • · Replies 23 ·
Replies
23
Views
5K