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Quote from: Bored chemist on 24/09/2020 12:57:57The properties concerned are energy and momentum.Incoming photon transfers energy and momentum to an electron. Why does the electron then emit a photon with the same energy, same momentum vector parallel to the surface, but reversed momentum vector perpendicular to the surface? If the temperature is above absolute zero, the electrons are all jiggling about and quite capable of transferring energy and momentum to the mass of the mirror.
The properties concerned are energy and momentum.
A simplified model could view it as a result of Lenz's Law.- An electromagnetic wave approaching a metallic reflecting surface induces a current in the metal which opposes the external magnetic field. If it is a good reflector, the opposing field will be equal and opposite to the incoming wave.- The incoming wave cancels the "mirror image" wave in the metal, so the incoming wave does not propagate into the metal surface.- But the external wave and the wave in the metal surface does have constructive interference, producing an outgoing wave which is a mirror-image of the incoming wave, and the angle of incidence = the angle of reflection.See: https://en.wikipedia.org/wiki/Lenz%27s_lawOf course, this is only part of the story, since non-conductive surfaces (eg glass) can also act as partial mirrors if they are in a medium with a very different speed of light.
It's a very clear exposition of the propagation and interference of a monochromatic, coherent em wave from a structure whose periodicity matches that of the wave, but(a) it isn't clear how this would apply to an incoherent, broad spectrum incident on a periodic structure (say polished metal) whose periodicity is a thousandth of the wavelength of the beam, or an aperiodic structure (glass, liquid metal)(b) in describing microwave dishes, it assumes that we know that i = r without explaining why!
The fact that a mirror is not a static regular array of dipole elements with spacing of the order of λ/2, but a sea of delocalised electrons.
The maths simply doesn't work if the array doesn't meet those conditions, but the phenomenon is obvious.
The interference pattern of a dipole array depends on the phase relationship of adjacent dipoles, as shown in your excellent RCAF clip. If the array periodicity is λ/2 you get constructive interference and maximum lobes perpendicular to the plane of the array. If you place your reflector dipoles λ/4 behind the array, you get unidirectional transmission. But if the phase relationships are not exactly as stated you get wobbly lobes and partial reflection.In an optical mirror you don't have dipoles or a regular array of anything commensurate with λ, so you need another mechanism to explain optical reflection.
Which part of those isn't clear yet?
Quote from: hamdani yusuf on 04/10/2020 06:25:13Which part of those isn't clear yet?The absence of dipoles.
Just out of curiosity, what happens as you move the elements closer together?What pattern would you get from an extended array of conductors at lambda/10 or lambda/100?
lambda/10 or lambda/100?
Quote from: Bored Chemistlambda/10 or lambda/100?Waves tend to ignore individual structures much less than λ/4, and go around them.A series of structures much less than λ/4 apart, appears much like a continuous surface.