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This question already has an answer here:

I don't understand fully why aluminium foil sparks in a microwave oven?

I think what is happening is the oven sets up an electric field, and the field induces a current in the foil (how?), and current in the foil then produces a very strong electric field which causes dielectric breakdown of the air, which is why we see sparks.

I think I'm confusing some electromagnetism concepts or something.

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marked as duplicate by Kyle Kanos, John Rennie, Steeven, Qmechanic May 27 '15 at 16:45

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  • $\begingroup$ possible duplicate of Why do metal objects in microwaves spark? $\endgroup$ – Kyle Kanos May 27 '15 at 0:46
  • $\begingroup$ The answers given there don't explain the phenomenon in any detail. It would be helpful if someone could elaborate and explain exactly whats going on. $\endgroup$ – Joshua Benabou May 27 '15 at 2:45
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The reason for the sparking is the photo-electric effect. The microwaves energize outer orbital electrons in metals and causes emission. Due to the conductive nature of the Al and insulting nature of the air (it's a dielectric), the electron charge can build. However, recombination of electrons into the orbitals is possible, but very slow compared to the discharge rate. The resulting charge becomes strong enough to ionize the air and create a conductive path to the walls of the microwave.

The electro-magnetic fields are highly dependent on the topology of the metal object. Where you have a sharp edge, there is a significant concentration of electric potential and therefore, the edge is more likely to discharge the electrical charge build-up.

Another example of this topological effect are tesla coils, where you'll often observe that folks place a rod on the torus to force the arc to originate that the end of the rod. The charging mechanism of electrons to the torus is completely different in this case, however.

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  • $\begingroup$ Hey ! Great answer +1. It's just that your reference to air as being insulating is a tad insulting. :) $\endgroup$ – Gaurav May 27 '15 at 4:51
  • $\begingroup$ Would there be significantly less sparking if the aluminium were extremely flat? $\endgroup$ – drglove May 27 '15 at 16:45
  • $\begingroup$ Not entirely. You still have edges and the electrical conductivity of Aluminium is very high. The most likely reason, if there is less sparking observed, is that more volume of aluminium is present in the "crumpled" case and that the "peaks and valleys" of the microwave EMF may correspond to the volume of the aluminium. However, both of these are easy to control for, if one were to experiment. However, in an ideal configuration - no, a flat piece wouldn't spark less. It, even so, has very sharp edges! $\endgroup$ – Jesse Johns May 28 '15 at 3:05
  • $\begingroup$ If you have a perfect sphere of aluminium, which, when it sparks doesn't gain or lose its oxide layer, would spark randomly. Edges increase the likelihood and predictability of where those sparks will be. The potential between the walls and the aluminium will not change because the surface topology of the aluminium changes. $\endgroup$ – Jesse Johns May 28 '15 at 3:08
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I have read no less than six different explanations of why aluminum foil sometimes sparks in a microwave. This is my best guess: Microwave ovens operate at about 2.45 Ghz. Water absorbs the non-ionizing radiation and becomes more active, creating heat. But aluminum foil, like all shiny metal, does not absorb microwaves - it reflects them.

Because the microwave energy is limited to the surface of reflective metal, only the surface electrons of the aluminum foil are excited (although if the foil is REALLY thin, it could transfer surface excitation heat to the food beneath).

Loosely bound to their nuclei, mobile among molecules (which is why metal carries electric current well), and driven by the microwave magnetron, these excited surface electrons set up currents and electric fields.

If there are sharp edges and crinkles in the metal, the fields intensify there. This is because electrons, which all have like charge, want to avoid each other, so in the absence of a positive charge to attract them, they flow to narrow sharp edges where the electron population is not as numerous as on the flat surfaces. Intensifying fields at sharp edges may create enough potential difference to cause a current to jump to the microwave oven's metal walls.

Microwave ovens are designed to discourage such antenna-like behavior, but if a current does jump through the air within the oven, it may exceed the dielectric breakdown strength of the air molecules (30 Kv per centimeter) and strip electrons from them, ionizing the air through which current travels. When the air becomes a conductor, it creates a spark. If the circuit breaker doesn't blow, an electric arc may appear.

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  • $\begingroup$ Ok but (1) how does the microwave establish a current in the foil and (2) if you have a high concentration of electrons at one sharp edge, and another concentration at anther sharp edge, wouldn't the resulting potential difference be small between these edges, so no arc? $\endgroup$ – Joshua Benabou May 27 '15 at 2:49
  • $\begingroup$ And also the foil is a conductor so it tries to establish equipotential on its surface so why would you get points on the surface with great potential difference? $\endgroup$ – Joshua Benabou May 27 '15 at 2:55
  • $\begingroup$ @JoshuaBenabou I think the answer to your questions is that it's not a statics problem. The fields in the box are oscillating at 2 GHz, driving currents through the material. No material is a perfect conductor, so the fields are able to penetrate the foil. $\endgroup$ – Gabe May 27 '15 at 3:09
  • $\begingroup$ @JohuaBenabou: The potential difference is between crinkles in the aluminum foil and other objects in the oven. Although a conductor tries to establish equipotential, the shape of the aluminum surface sometimes thwarts this. I've edited the answer to try to address your questions. Also, see Jesse Johns' answer which is better, clearer, and more complete than mine. $\endgroup$ – Ernie May 27 '15 at 13:48

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