Condenser microphone uses dc-coupled impedance converter
Dimitri Danyuk, Miami, FL - March 15, 2012
The diaphragm of a condenser
microphone is the movable plate
of a capacitor. With a polarized capacitor,
the vibration of the diaphragm in
relation to the back plate produces an
ac audio-output voltage. The condenser
capsule has a capacitance of 10 to 60
pF; thus, you should connect it to an
impedance converter with extremely
high input impedance for a flat frequency
response.
The conventional impedance converter
is a JFET source follower with
an additional amplifying and power-decoupling
circuit. You supply power
to the impedance-converter circuitry
using the same microphone-cable
conductors that carry the audio signal.
The balanced audio pair at the
XLR connector’s pins 2 and 3 both
carry the same positive dc voltage,
or phantom power, relative to Pin 1’s
ground. The amplifying/decoupling
circuit contains an audio transformer or a couple of capacitors to separate
the dc power from the audio signal.
High-value dc-blocking capacitors can generate measurable and audible distortion (Reference 1). Microphone circuits rarely use the highest-quality capacitors because of space limitations. You can design the impedance converter without dc-blocking capacitors.
Figure 1 shows the self-balanced impedance converter. The self-polarized electret condenser-microphone capsule, X1, connects to the high-impedance gate of JFET Q1. Q2, an ac-current source, loads source follower Q1. Q2, thanks to C2, has high impedance but allows a fixed dc voltage on the Q1 source.

The circuit sources phantom power
at 48V dc through RPH1 and RPH2 at
the mixing-console end of the microphone
cable. Q2’s emitter drives—and
RPH1 loads—emitter follower Q3. The
signal from Q3’s emitter bootstraps the
drain of Q1, reducing the ac voltage
across the gate-to-drain capacitance
and resulting in lower input capacitance
at the gate of Q1. RPH2 supplies
current for shunt-regulator-voltage
sources D2 and Q4. R4 and C4 attenuate
zener-diode noise. Integrator IC1
compares the dc voltages on the XLR
connector’s pins 2 and 3 and, through
Q2 and Q3, maintains a difference equal to the op amp’s input offset voltage.
Thus, if the microphone input
at the mixer console is transformer-coupled,
both ends of its winding are
at the same voltage. No dc will flow
through the winding and saturate the
core. IC1 should have a common-mode-input-voltage range equal to
that of the positive-supply rail. You
can accomplish this task using, for
example, an op amp with a P-channel
JFET input stage. Tables 1 and 2 and
Figure 2 show typical performance
parameters for the impedance converter
in Figure 1.

The conventional impedance converter
is a JFET source follower with
an additional amplifying and power-decoupling
circuit. You supply power
to the impedance-converter circuitry
using the same microphone-cable
conductors that carry the audio signal.
The balanced audio pair at the
XLR connector’s pins 2 and 3 both
carry the same positive dc voltage,
or phantom power, relative to Pin 1’s
ground. The amplifying/decoupling
circuit contains an audio transformer or a couple of capacitors to separate
the dc power from the audio signal.High-value dc-blocking capacitors can generate measurable and audible distortion (Reference 1). Microphone circuits rarely use the highest-quality capacitors because of space limitations. You can design the impedance converter without dc-blocking capacitors.
Figure 1 shows the self-balanced impedance converter. The self-polarized electret condenser-microphone capsule, X1, connects to the high-impedance gate of JFET Q1. Q2, an ac-current source, loads source follower Q1. Q2, thanks to C2, has high impedance but allows a fixed dc voltage on the Q1 source.

The circuit sources phantom power
at 48V dc through RPH1 and RPH2 at
the mixing-console end of the microphone
cable. Q2’s emitter drives—and
RPH1 loads—emitter follower Q3. The
signal from Q3’s emitter bootstraps the
drain of Q1, reducing the ac voltage
across the gate-to-drain capacitance
and resulting in lower input capacitance
at the gate of Q1. RPH2 supplies
current for shunt-regulator-voltage
sources D2 and Q4. R4 and C4 attenuate
zener-diode noise. Integrator IC1
compares the dc voltages on the XLR
connector’s pins 2 and 3 and, through
Q2 and Q3, maintains a difference equal to the op amp’s input offset voltage.
Thus, if the microphone input
at the mixer console is transformer-coupled,
both ends of its winding are
at the same voltage. No dc will flow
through the winding and saturate the
core. IC1 should have a common-mode-input-voltage range equal to
that of the positive-supply rail. You
can accomplish this task using, for
example, an op amp with a P-channel
JFET input stage. Tables 1 and 2 and
Figure 2 show typical performance
parameters for the impedance converter
in Figure 1.
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