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What is the radiation force $F$ due to a beam of photons of power $P$ undergoing perfect reflection? Is it

$$a) F = 2 P / c$$

or

$$b) F = 2 P / v_g$$ where $v_g$ is the group velocity

?

Note that $v_g$ varies spatially in waveguides and in asymmetric cavities too, even in the absence of a dielectric.

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  • $\begingroup$ It seems that by you specifying "perfect reflection," you already selected answer a)! If you don't have perfect reflection, then I believe it would be answer b). $\endgroup$ – Guill Jun 26 '15 at 23:46
  • $\begingroup$ Its not related to wether the reflection is perfect or not. That would affect the coefficient. It would be 1 instead of 2 if it was completely absorbing media. $\endgroup$ – Ronan Tarik Drevon Jun 27 '15 at 11:03
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    $\begingroup$ This is a great question. Here's a link to another discussion of a similar question -- I'm not sure how authoritative it is, though. quora.com/… $\endgroup$ – kleingordon Jun 29 '15 at 22:46
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The radiation pressure varies with the phase velocity of the light, not the group velocity, although you must keep in mind that the phase velocity in matter might be different from $c$ and vary with wavelength in a dispersive medium.

This has been experimentally demonstrated and described in this paper, in which it was found that the radiation force felt on a mirror will vary in direct proportion to the index of refraction of the material in which the mirror is immersed.

Intuitively, for higher index of refraction (slower phase velocity), there are more photons per unit length, increasing their energy density and pressure.

While the pressure on the mirror once the photons arrive will depend on the phase velocity, the group velocity still controls the rate at which information can be transferred.

Update

To be explicit, for a beam of photons with wavelength $\lambda_0$ emitted with power $P$ traveling through a medium with index of refraction $n(\lambda_0)$ impinging directly on a mirror immersed in that medium (angle of incidence is zero), the force $F$ felt by the mirror is given by

$$ F = \frac{2 n(\lambda_0) P}{c} \, \, .$$

The index of refraction is related to the phase velocity at that given wavelength, $v_{ph}(\lambda_0)$, by the relation

$$ n(\lambda_0) = \frac{c}{v_{ph}(\lambda_0)} \, \, ,$$

so that the radiation force for this single-wavelength beam can also be written as

$$ F = \frac{2 P}{v_{ph}(\lambda_0)} \, \, .$$

For light composed of a range of wavelengths, you must integrate this expression over the photon distribution of the beam with respect to wavelength, taking into account how the index of refraction varies with wavelength.

Further update (microscopic description)

Microscopically, you can think of the momentum being carried simultaneously by the E&M fields, and "an additional co-traveling momentum within the medium from the mechanical momentum of the electrons in the molecular dipoles in response to the incident traveling wave" (J.D. Jackson, Classical Electrodynamics 3rd edition, p. 262, and its corresponding reference to this paper).

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  • $\begingroup$ If the answer is neither a) nor b), please write down the correct answer $\endgroup$ – Andrew Palfreyman Jul 2 '15 at 23:42
  • $\begingroup$ Sorry, I thought it might have been clear from what I had already written, but I have updated the answer to be even more explicit. $\endgroup$ – kleingordon Jul 3 '15 at 18:36
  • $\begingroup$ Thank you - very clear. It implies that, within cavities and waveguides in vacuum where the phase velocity is c, answer a) is the correct one (coincidentally Sir Rudolph Peierls viva'd me for my M.A. in physics many years ago) $\endgroup$ – Andrew Palfreyman Jul 4 '15 at 19:18
  • $\begingroup$ Inside a waveguide or cavity, the relation holds $$v_g*v_p = c^2$$. Usually $v_g < c$, so $v_p > c$. Therefore, if you are correct, the force is less than is predicted by a). $\endgroup$ – Andrew Palfreyman Jul 21 '15 at 19:03
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About radiation force in a waveguide:

  • Group velocity conveys energy, momentum and information in a waveguide.
  • Phase velocity is superluminal in a waveguide.

See for example "Phase, Group, and Signal Velocity" about the case of a waveguide:

A waveguide imposes a "cutoff frequency" $\omega_0$ on any propagating electromagnetic waves based on the geometry of the tube, and will not sustain waves of any lower frequency. This is roughly analogous to how the pipes in a Church organ will sustain only certain resonant patterns. As a result, the dominant wave pattern of a propagating wave with a frequency of $\omega$ will have a wave number $k$ given by

$$k = \frac{1}{c} \sqrt{\omega^2-\omega_0\,^2}$$

Since (as we've seen) the phase velocity is $\omega/k$, this implies that the (dominant) phase velocity in a waveguide with cutoff frequency $\omega_0$ is

$$v_p = \frac{c}{\sqrt{{1}-\left(\frac{\omega_0}{\omega}\right)^2}}$$

Hence, not only is the phase velocity generally greater than c, it approaches infinity as $\omega$ approaches the cutoff frequency $\omega_0$. However, the speed at which information and energy actually propagates down a waveguide is the group velocity, which (as we've seen) is given by ${\mathrm d \omega}/{\mathrm d k}$. Taking the derivative of the preceding expression for $k$ with respect to $\omega$ gives

$$\frac{\mathrm d k}{\mathrm d \omega} = \frac{\omega}{c\sqrt{\omega^2-\omega_0\,^2}}$$

so the group velocity in a waveguide with cutoff frequency $\omega_0$ is

$$v_g = \frac{\mathrm d \omega}{\mathrm d k} = c {\sqrt{{1}-\left(\frac{\omega_0}{\omega}\right)^2}}$$

which of course is always less than or equal to c.

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  • $\begingroup$ Fair enough - so do you vote for a), b) or c) phase velocity? $\endgroup$ – Andrew Palfreyman Jul 26 '15 at 15:40
  • $\begingroup$ Sorry, didn't came back here before. I'd say a) in free space propagation and c) i.e. according to group velocity in waveguides and resonant cavities. $\endgroup$ – flux_capacitor Sep 18 '18 at 16:19
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If you adopt a photonic model where the photons are seen as little particles like gas particle then the following simple demonstration indicates :

enter image description here

The fundamental principle of mechanics gives :

$N\frac{\triangle p}{\triangle t}=pS_{yz}$

Where N is the number of photons inside the cavity, p the radiation pressure and ${\triangle p}$ the change of momentum of every photons.

The time it takes for the photon to travel ${2\triangle z}$ is :

$\triangle t=\frac{2\triangle z}{v_{g}}$

The change of momentum of the photon is as usual:

$\triangle p=2\frac{h\nu}{c}$

though only a fraction $\frac{v_{g}}{c}$ will actually be used to act as a force against the surface S

Hence the radiation pressure gives :

$p=\frac{Nh\nu}{\mathcal{V}}(\frac{v_{g}}{c})^2$

since $\mathcal{E}_{em}=\frac{Nh\nu}{\mathcal{V}}$ we have the following expression for the radiation pressure :

$p=\mathcal{E}_{em}(\frac{v_{g}}{c})^{2}$

As in a cavity the group velocity is expressed in term of tilted plane waves $v_{g}=c.cos\theta$ then we recover the classic expression for tilted plane waves :

$p=\mathcal{E}_{em}cos^{2}\theta$

In the case of asymmetric cavity the radiation pressure has to be calculated by using the surface charges and surface currents existing on the surface of the perfect conducting walls. I do not know if a simple picture with photon can be carried out in such a case.

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  • $\begingroup$ A photon never travels at any other speed than the speed of light hence its momentum is always $p=E/c$. Though, its path can be such that its apparent speed is slower. It corresponds to saying that only a part of its momentum can actually be used as a force/pressure on a surface $\endgroup$ – Ronan Tarik Drevon Jun 25 '15 at 12:48
  • $\begingroup$ Sorry but you don't define all your terms, you contradict yourself, and you do not choose a) or b), which is the question here. $\endgroup$ – Andrew Palfreyman Jun 28 '15 at 18:26
  • $\begingroup$ you curiously say that I do not define my terms where you did not even say what was P in your expression : Is it a pressure or a momentum, or a power. Assuming it is a power which would make the equation dimension correct, the power of a photon is not a physical concept. Moreover the main answer I give you is that the momentum is p=E/c always but finding the corresponding radiation pressure gets tricky in 3 dimensions and needs proper calculation of the energy and power inside the cavity. I do not see where I contradicted myself though $\endgroup$ – Ronan Tarik Drevon Jun 29 '15 at 12:16
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I would go for: $$F=\frac{2P}{c}$$ This is my reasoning: the force exerced by the light beam is due to momentum conservation. Therefore, we just have to know what the momentum of the light beam is, multiply this by 2 (because of the perfect reflection) and voilà, we have the answer.

Now, as in General Relativity, we can define the energy-momentum tensor (or stress-energy tensor depending on the crowd ^^) $T_{\mu \nu}$ (see https://en.wikipedia.org/wiki/Stress%E2%80%93energy_tensor). The first line of this matrix is the density of energy and momentum. The remaining lines gives the fluxes of those in the different directions of space. Now, it turns out that this tensor is symmetric ($T_{\mu \nu} = T_{\nu \mu}$). It means that the flux density of energy (that is the power density) in the direction $x$ for instance is the same quantity as the momentum density in the direction $x$.

The factor $c$ therefore is just a conversion factor between space and time coordinates and does not refer to the speed of the beam.

In particular, it is interesting to see that this argument is valid for any object not just light. The force exerced by a beam of massive non-relativistic (slow) particles is also $\frac{2P}{c}$. But we should be careful: the power involved takes into account every kind of energy, including mass energy. The factor $c$ that appears in $E= mc^2$ would then cancel out to give the usual expression.

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