If light has no weight, how can it push objects?

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    Light Push Weight
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Discussion Overview

The discussion centers around the concept of how light, despite having no rest mass, can exert force and push objects, particularly in the context of solar sails and radiometers. Participants explore the implications of light's momentum and energy transfer, raising questions about the nature of momentum in massless particles and the behavior of light in various scenarios.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Some participants assert that photons do not have rest mass but carry momentum, which is defined by the equation p=E/c, where E is the energy of the photon.
  • Others argue that light can push objects due to the momentum it carries, despite the absence of rest mass.
  • A participant questions the validity of the assumption that momentum is solely dependent on mass and velocity, suggesting that the formula for momentum is different for massless particles.
  • Some participants discuss the operation of a Crookes radiometer, noting that it turns due to heat generated by absorbed light rather than direct light pressure, leading to debates about the mechanisms at play.
  • There are inquiries about the relationship between energy and mass, particularly referencing Einstein's equation E=mc² and its applicability to massless particles.
  • A participant raises concerns about the presence of air currents in a vacuum radiometer, questioning how this affects the observed behavior of the device.
  • Some participants express confusion about the implications of light's momentum and its ability to transfer energy to matter.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the nature of momentum in light or the mechanisms behind the operation of radiometers. Multiple competing views remain regarding the interpretation of light's ability to exert force and the implications of Einstein's equations.

Contextual Notes

There are unresolved questions regarding the assumptions made about momentum and energy transfer in massless particles. The discussion also highlights the complexity of interpreting experimental observations, such as those related to the Crookes radiometer.

  • #61
cmb said:
Can anyone link to a write-up of an experiment that proves absorption of photons results in a momentum exchange to the object absorbing the photons?

D.S. Weiss et al., "Precision measurement of the photon recoil of an atom using atomic interferometry" Phys. Rev. Lett. 70, 2706 (1993).

G.K. Campbell et al., "Photon Recoil Momentum in Dispersive Media" Phys. Rev. Lett. 94, 170403 (2005).

Zz.
 
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  • #62
D H said:
You are asking us to write a book. Unless you are a junior in an undergrad physics program taking the introductory condensed matter course, any quantum explanation of reflection is going to be hand-waving at best. I gave the hand-waving, semiclassical description above.

Ultimately it must be an electric-magnetic interaction. One might therefore interpret this as some sort of magnetic repulsion of two distant bodies, for which the photon is 'only' a mediation.
 
  • #63
cmb said:
Ultimately it must be an electric-magnetic interaction. One might therefore interpret this as some sort of magnetic repulsion of two distant bodies, for which the photon is 'only' a mediation.
Ultimately, it is quantum electrodynamics that explains the interaction of photons and matter, and that is way, way beyond the scope of this thread.
 
  • #64
DaleSpam said:
In order to get specular reflection you need structures which are significantly larger than a wavelength and are smooth over that scale. That simply doesn't happen at the molecular level, so a specular reflection implies an interaction of a photon with a continuum of molecules.



OK, but am I'm right in saying the underlying physical mechanism is the interaction of an electromagnetic field with charged particle(s) (ie, electrons)?

And, if I understand you correctly, you are objecting that the magnetic field of the photon is so large compared to the size of electrons and molecules that the interaction is between a photon's magnetic field and 1000's or 10's of thousands of electrons -- a sea of electrons (metals) or a lattice of electrons (a crystal) or a sea of molecules (water), instead of with just one electron. Which makes sense.

And then what happens next, after the charged particles get the magnetic "push" from the photon's magnetic field, they move of course, which gives a little push to the protons/neutrons of all the nearby molecules? This effect ultimately being caused by the effect that keeps electrons from getting too close to a proton/neutron?
 
  • #65
dlr said:
the magnetic field of the photon

What is this? I don't even
 
  • #66
It's easier to see from a classical em viewpoint. You have a positive charge sitting stationary in space. A step function em wave approaches from the left with the electric field always pointing down your computer screen and magnetic field always pointing into the screen. The charge accelerates downward due to the E field, so its velocity increases. That downward velocity interacts with the em wave's magnetic field via v X B, resulting in a force to the right, which accelerates the charge to the right. Voila, the em wave has imparted downstream velocity/momentum to the charge.

One interesting special case is when the charge is initially traveling with or against the em wave. In that case, v X B becomes -v/c * E and the resulting total initial force on the charge is (1 - v/c)*E. Looks a lot like a "Doppler Shift" of the electric field strength, eh? You'll note in the extreme case of v = c (i.e. when the charge is moving with the wave at the speed of light) there is no net force on it.

That's what classical em says ... not that I believe it (or QM). I don't have any better answer so I basically keep my mouth shut!
 
  • #67
fizzle said:
The charge accelerates downward due to the E field, so its velocity increases. That downward velocity interacts with the em wave's magnetic field via v X B, resulting in a force to the right, which accelerates the charge to the right. Voila, the em wave has imparted downstream velocity/momentum to the charge.


Yes, the force is perpendicular to the direction of travel of the light ray. So then, why does the solar sail move directly away from the light rays hitting it?
 
  • #68
Last edited:
  • #69
dlr said:
Yes, the force is perpendicular to the direction of travel of the light ray. So then, why does the solar sail move directly away from the light rays hitting it?
I was showing above that a simple, constant step wave transfers downstream momentum to a charge. For light, which is a circularly polarized (CP) em wave, you don't get the down-the-screen motion because the E field rotates; so the charge rotates in a circle while being accelerated downstream by v x B. The overall path is a helix in the direction of the wave.

BTW, if you do a full relativistic/classical em analysis of a CP wave interacting with a charge you can derive the Compton Scattering equations - as Compton noted in his original paper. The problem is that the transfer a "photon" of energy to the charge requires an unrealistically high E field (10^16 V/m or more) in the CP wave, sort of a Compton catastrophe. This is the root cause of QM and its associated weirdness (e.g. a photon is a particle+wave, wave function collapse, zero-point energy with its enormous but "hidden" fields, etc.). No one was able to figure out how a realistic CP em wave could transfer so much energy to a single charge.

"speculation deleted"

Integral
 
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