Editing Microphone (section)

==== DC-biased condenser ====
With a '''DC-biased condenser microphone''', the plates are [[Voltage bias|biased]] with a fixed charge (''Q''). The [[voltage]] maintained across the capacitor plates changes with the vibrations in the air, according to the capacitance equation (C = {{fract|Q|V}}), where Q = charge in [[coulomb]]s, C = capacitance in [[farad]]s and V = potential difference in [[volt]]s. A nearly constant charge is maintained on the capacitor. As the capacitance changes, the charge across the capacitor does change very slightly, but at audible frequencies it is sensibly constant. The capacitance of the capsule (around 5 to 100&nbsp;[[Farad|pF]]) and the value of the bias resistor (100&nbsp;[[Ohm|MΩ]] to tens of GΩ) form a filter that is high-pass for the audio signal, and low-pass for the bias voltage. Note that the time constant of an [[RC circuit]] equals the product of the resistance and capacitance.

Within the time frame of the capacitance change (as much as 50&nbsp;ms at 20&nbsp;Hz audio signal), the charge is practically constant and the voltage across the capacitor changes instantaneously to reflect the change in capacitance. The voltage across the capacitor varies above and below the bias voltage. The voltage difference between the bias and the capacitor is seen across the series resistor. The voltage across the resistor is amplified for performance or recording. In most cases, the electronics in the microphone itself contribute no voltage gain as the voltage differential is quite significant, up to several volts for high sound levels.