Most operational amplifier circuits require a dual-polarity power supply - one having +V and -V. However, there are times when a DP supply simply isn't conveniently available. Single-polarity modifications to DP designs often achieve their effect by referencing the input to a "synthetic ground," derived using a resistive voltage divider. This renders the resulting circuit highly sensitive to power supply noise, since any variation in the power supply will be divided by the divider, then used as an input reference, and amplified by the circuit in question. While this is of little concern with battery sources, AC "wall-warts" and many DIY power supplies are chock full of horrendous 60Hz buzz that is sure to get into the circuit. By powering an op amp with a dual-polarity supply, it is possible to reference all signals to a definite solid 0V ground.
This circuit starts with a single-polarity (GND and +V) input and produces an approximate opposite voltage (-V), enabling dual-polarity op amp circuits to be used with single-polarity supplies.
Theory of Operation: This circuit is designed to power a microphone preamp from an unregulated, noisy, single-polarity 12V supply that also powers other devices. The circuit employs a multivibrator configuration using transistors Q1 and Q2, along with capacitors C1 and C2, and resistors R1 through R4. The multivibrator generates oscillating signals that drive transistors Q3 and Q4, which act as current amplifiers.
When Q3 is activated, it connects the positive voltage (+V) to capacitor C3, allowing it to charge. Once C3 is charged, Q3 deactivates and Q4 is activated, connecting the negative terminal of C3 to ground. This results in C3's negative terminal being at a voltage level that is below ground, effectively producing a negative voltage output. The output voltage is taken through diode D2. Capacitor C4 acts as a filter capacitor for the negative voltage, providing current during the charging cycles of C3, ensuring a stable output voltage.
The component values are as follows:
- Resistors: R1 = 1K, R2 = 10K, R3 = 10K, R4 = 1K, R5 = 1K, R6 = 1K
- Capacitors: C1 = 0.1µF, C2 = 0.1µF, C3 = 1000µF, C4 = 1000µF
- Transistors: All transistors are 2N3906 General Purpose PNP types.
- Diodes: Generic silicon rectifiers are used.
This configuration provides a practical solution for applications requiring dual-polarity power supplies from single-polarity sources, while also highlighting potential noise issues inherent in the design.Most operational amplifier circuits require a dual-polarity power supply - one having +V and -V. However, there are times when a DP supply simply isn't conveniently available. Single-polarity modifications to DP designs often acheive their effect by referencing the input to a "synthetic ground", derived using a resistive voltage divider. This renders the resulting circuit highly sensitive to power supply noise, since any variation in the power supply will be divided by the divider, then used as an input reference, and amplified by the circuit in question.
While this is of little concern with battery sources, AC "wall-warts" and many DIY power supplies are chock full of horrendous 60Hz buzz that is sure to get into the circuit. By powering an op amp with a dual-polarity supply, we are able to reference all signals to a definite solid 0V ground. This circuit starts with a single-polarity (GND and +V) input and produces an approximate opposite voltage (-V), enabling dual-polarity op amp circuits to be used with single-polarity supplies.
Theory of Operation
This circuit was built in a pinch because I needed to power a microphone preamp from an unregulated, noisy, single-polarity 12V supply that also powers a couple of power-hungry sirens and a video camera. While said preamp is now working relatively successfully, this circuit is a quick design that has not been put through extensive testing.
I do not know its current limitations. Some components on the board can be heard to be "whining", much like a switchmode power supply. This does not indicate a problem, as none of the components run particularly hot. Also like a SMPS, this noise is slightly detectable on the output. Q1, Q2, C1, C2, R1, R2, R3, and R4 form a multivibrator -- an oscillator. We are using both of its outputs which are opposites of one another: when one is on, the other is off. These outputs go through R5 and R6 to turn on Q3 and Q4 - one at a time, of course. This applies a wave oscillating from +V to GND to C3. This is where things get interesting. Q3 and Q4 form a current amplifier. When Q3 is turned on, +V is applied to C3. We can envision the current going through C3 and D1 to ground. This charges C3. Next, Q3 turns off and Q4 turns on, applying GND to C3. C3's + terminal is now at GND. Since C3 is charged to nV, its - terminal has to be n volts below its + terminal, meaning that its - terminal is n volts below GND.
This goes through D2 and is our output. C4 is a filter capacitor for -V, and serves up the current filling in the gaps when C3 is charging. R1 1K
R2 10K
R3 10K
R4 1K
R5 1K
R6 1K
Capacitors
C1 .1uF
C2 .1uF
C3 1,000uF
C4 1,000uF
All transistors: 2N3906 General Purpose PNP
All diodes: Generic silicon rectifiers 🔗 External reference
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