Arcing in a parallel-plate air-filled capacitor

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SUMMARY

The discussion centers on the arcing phenomenon in constant-charge capacitor microphones, which utilize a parallel-plate capacitor configuration. The polarizing voltage typically ranges from 48V to 200V, while the distance between the plates is approximately 20 micrometers. Given the dielectric strength of dry air at 3*10^6 V/m, arcing should theoretically occur at 60V. Participants explore the implications of using inert gases to potentially increase the arc-over voltage, indicating a gap in understanding the operational limits of these microphones.

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  • Knowledge of RC filter circuits and their cut-off frequency calculations
  • Familiarity with dielectric strength and arcing concepts
  • Basic principles of microphone design and operation
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The_Lobster
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I'm reading about constant-charge capacitor microphones, and they are essentially made up of a parallel-plate capacitor (one plate fixed, the other moving to sound pressure), in a circuit with a series resistor and DC source to provide polarising voltage.

The circuit is basically an RC filter, with a cut-off frequency down to 10-20Hz (so from f = 1/2piRC it requires a large R if C is small). The polarising voltage from the DC source is often around 48V, but can be as large as 200V for some microphones.

My question now is: The distance between the parallel plates in the capacitor is often around 20 micrometers. Now, if the dielectric strength of dry air is 3*10^6 V/m, there should be arcing at 3*10^6 V/m * 20 * 10^-6 m = 60 V. So from my theory it seems that most of these mics should arc due to the polarising voltage, just by turning them on! Clearly I must have a gap in my understanding some place?

Thanks!
 
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The_Lobster said:
I'm reading about constant-charge capacitor microphones, and they are essentially made up of a parallel-plate capacitor (one plate fixed, the other moving to sound pressure), in a circuit with a series resistor and DC source to provide polarising voltage.

The circuit is basically an RC filter, with a cut-off frequency down to 10-20Hz (so from f = 1/2piRC it requires a large R if C is small). The polarising voltage from the DC source is often around 48V, but can be as large as 200V for some microphones.

My question now is: The distance between the parallel plates in the capacitor is often around 20 micrometers. Now, if the dielectric strength of dry air is 3*10^6 V/m, there should be arcing at 3*10^6 V/m * 20 * 10^-6 m = 60 V. So from my theory it seems that most of these mics should arc due to the polarising voltage, just by turning them on! Clearly I must have a gap in my understanding some place?

Thanks!

That's a good question! I don't think the inner space could be filled with partial vacuum (to take advantage of the Paschen curve) because that would inhibit the movement of the flexible plate. But what if it were filled with an inert gas? Would that raise the arc-over voltage enough?
 

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