Does a photon lose potential energy and momentum when approaching a mass?

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Discussion Overview

The discussion revolves around the behavior of photons in a gravitational field, specifically whether photons lose potential energy and momentum when approaching a mass, such as the Earth. Participants explore concepts related to energy, frequency, and mass of photons in the context of gravitational effects.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants propose that as a photon approaches a mass, it loses potential energy, which could imply a decrease in frequency based on the equation E = hf.
  • Others argue that while the frequency may appear to change depending on the observer's position in the gravitational field, the energy of the photon remains constant for a single observer at the point of emission.
  • A participant questions the implications of constant energy on the mass of the photon, suggesting that if energy remains the same, mass must also remain unchanged.
  • There is a discussion about whether photons are attracted to masses and if they could be accelerated by gravity, with some asserting that photons cannot exceed the speed of light, while others suggest that local measurements may yield different results.
  • One participant highlights the complexity of the relationship between energy, mass, and momentum in a gravitational field, referencing the contravariant 4-momentum of particles.
  • Another participant expresses difficulty in understanding the technical aspects of the discussion and requests a simpler explanation.

Areas of Agreement / Disagreement

Participants express differing views on the behavior of photons in a gravitational field, particularly regarding energy, frequency, and mass. There is no consensus on whether photons lose potential energy or how their mass is affected by gravitational interactions.

Contextual Notes

The discussion involves complex concepts such as relativistic mass, local versus remote measurements, and the implications of gravitational fields on light. Participants reference specific equations and theories, indicating a reliance on advanced physics principles that may not be universally understood.

lavalamp
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I know that as things "fall" towards each other, they lose potential energy, that's fine. What I want to know is when a photon falls towards a mass does the photon also lose potential energy?
I would assume so because potons have an equivalent mass. From the equation E = hf, can I therefore assume that the frequency of a photon actually lowers when it approaches the Earth?

If so then it seems to also follow that it's momentum also lowers from the equation E = pc, this then seems to suggest that photons lose mass when approaching other mass and that an impulse is applied to the photon to cause this loss of momentum.
But this would mean that the impulse was acting away from the mass, ie: the photon was experiencing a repulsive force upon approaching some matter. Is this a positive gravitational force?
 
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Originally posted by lavalamp
I know that as things "fall" towards each other, they lose potential energy, that's fine. What I want to know is when a photon falls towards a mass does the photon also lose potential energy?
I would assume so because potons have an equivalent mass.
Yes. That is exactly correct.

From the equation E = hf, can I therefore assume that the frequency of a photon actually lowers when it approaches the Earth?
As the photons moves to a lower location the frequency as measured locally increases.

But whether the frequency or energy changes depends on who is doing the measuring. Any single observer will detect neither a change in energy nor a change in frequency as a particle moves through the g-field. Such changes are meaured locally. I.e. if an observer higher in the g-field emits a photon which then travels to an observer who is lower in the g-field. The lower observer will measure a higher frequency than the frequency which left emitter. Interpret this as a decrease in potential energy which is compensated for an increase in kinetic energy. The local observer measures zero potential energy at his location and therefore all the energy he measures is kinetic energy. For a derivation see

http://www.geocities.com/physics_world/red_shift.htm

Note: I made an error in Eq. (7) [forgot to relable the subscripts on r)

Pete
 
So you are saying that when a photon "falls" towards a mass, it's potential energy decreases while it's kinetic energy increases? I can accept that as it is true for all other particles, however this must mean that it's mass increases upon approaching a mass. Since the photon still has the same energy, it must still have the same frequency (for an observer at the point of emission of the photon), but now I am faced with another problem.
As the equation E = mc2 shows, for any value of E there is a corresponding value for m. Since the overall energy of the photon has stayed the same, would the mass of the photon have to stay the same as well?

Another problem, photons have mass and therefore they are attracted to things like the sun and black holes and all other particles. If there was a photon heading straight for the Earth, wouldn't it be accelerated by the Earth's gravitational field and therefore be traveling at a velocity greaty than c?
Since it is already traveling AT c, and it's mass is most definitely not infinite, wouldn't the force due to the Earth's gravity cause it to accelerate? Any acceleration in the same direction as the photon is traveling would cause it to travel at a speed greater than c wouldn't it?
 
Originally posted by lavalamp
So you are saying that when a photon "falls" towards a mass, it's potential energy decreases while it's kinetic energy increases?
Yes. And that means that the total energy remains constant.

I can accept that as it is true for all other particles, however this must mean that it's mass increases upon approaching a mass.
Only when measured locally. And that, of course, is its relativistic mass that we're speaking about, not its rest mass.

Since the photon still has the same energy, it must still have the same frequency ..
Now you're talking about a different measurement. Yes. The frequency remains constant as observed by any sinlge observer.

As the equation E = mc2 shows, for any value of E there is a corresponding value for m. Since the overall energy of the photon has stayed the same, would the mass of the photon have to stay the same as well?
That relationship does not hold in this case. mc2 is not the conserved quantity here. The contravariant 4-momentum of a particle is Pu = (E/c,p). In flat spacetime in an inertial frame of referance P0c = E = mc2 is a constant and is the energy of the photon. If the metric tensor is guv = diag(1,-1,-1,-1) and the covariant 4-momentum is Pu = (E/c,-p). So P0c = E too and also is a constant. However in a gravitational field P0 is not the same as P0. In a static gravitational field like the Earth's only the later is a constant.

Another problem, photons have mass and therefore they are attracted to things like the sun and black holes and all other particles. If there was a photon heading straight for the Earth, wouldn't it be accelerated by the Earth's gravitational field and therefore be traveling at a velocity greaty than c?
As measured locally the speed of light is always the same constant. If not measured locally, i.e. as measured by a remote observer far from the Earth the speed of light in the Earth's gravitational field is not a constant. The force of gravity of the photon will depend on the photons's location in the gravitational field. As far as the functional relation of speed vs. position.

Since it is already traveling AT c, and it's mass is most definitely not infinite, wouldn't the force due to the Earth's gravity cause it to accelerate?
Yes.

Any acceleration in the same direction as the photon is traveling would cause it to travel at a speed greater than c wouldn't it?
That depends on where in the field it is and who is doing the measuring.

What you're failing to take into account is the fact that the acceleration of light depends on the velocity of light. E.g. at one point the speed of light starts to slow down as the light approaches a black hole.

See also -
http://www.physlink.com/Education/AskExperts/ae13.cfm

Pete
 
The bits that looked pretty as the flew over my head:

That relationship does not hold in this case. mc2 is not the conserved quantity here. The contravariant 4-momentum of a particle is Pu = (E/c,p).

If the metric tensor is guv = diag(1,-1,-1,-1) and the covariant 4-momentum is Pu = (E/c,-p). So P0c = E too and also is a constant. However in a gravitational field P0 is not the same as P0. In a static gravitational field like the Earth's only the later is a constant.
Is there anyway that you could dumb this down into something that I might be able to grasp a bit better?

By the way, when I say does the frequency of light change? And you say, it depends where you are observing from, I usually mean from an infinite distance away (at 0 potential energy), where you are not affected by the gravitational field.
 
Originally posted by lavalamp
The bits that looked pretty as the flew over my head:

Is there anyway that you could dumb this down into something that I might be able to grasp a bit better?

By the way, when I say does the frequency of light change? And you say, it depends where you are observing from, I usually mean from an infinite distance away (at 0 potential energy), where you are not affected by the gravitational field.

Let me get back to you on that. In the mean time you can read more on this in the article

"On the Interpretation of the Redshift in a Static Gravitational Field," L.B. Okun, K.G. Selivanov, V.L. Telegdi, Am.J.Phys. 68 (2000) 115

http://xxx.lanl.gov/abs/physics/9907017

Pete
 

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