Audio Amplifiers

NE5532 Ultra-Low-Noise Inverting Microphone Preamplifier

Single-channel ultra-low-noise inverting audio preamplifier based on the Texas Instruments NE5532 op-amp, featuring +33.4 dB closed-loop gain, input DC blocking, and high-frequency phase compensation.

Closed-Loop AC Gain (Av)
-47 V/V (+33.44 dB, 180° phase inversion)
Components
9
Formulas
4
Gotchas
4
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Schematic workbench

NE5532 Dual Low-Noise Inverting Microphone PreamplifierExported from CircuitBaseMIC_IN+C110µFR11kΩU1ANE5532PR247kΩC247pFR31kΩ+C310µFGNDGNDR447Ω+C610µFAUDIO_OUT+15V-15V

Circuit overview

Closed-Loop AC Gain (Av)
-47 V/V (+33.44 dB, 180° phase inversion)
Components
9
Formulas
4
Gotchas
4

Click any component in the schematic above to inspect its electrical ratings, function, and connections.

Circuit overview

This preamplifier implements an ultra-low-noise audio gain stage optimized for low-impedance dynamic microphones (150 Ω to 600 Ω) using the Texas Instruments NE5532 operational amplifier (datasheet SLOS075K). Powered from symmetrical ±15 V rails, the circuit operates in an inverting configuration with closed-loop voltage gain Av = -RF / RI = -47 kΩ / 1 kΩ = -47 V/V (+33.44 dB, 180° phase inversion). Setting input resistor R1 to 1 kΩ matches dynamic microphone capsules while suppressing the op-amp input noise current contribution (0.7 pA/√Hz). Input DC blocking capacitor C1 (10 µF) forms a 15.9 Hz high-pass corner, eliminating phantom bias or transducer DC currents from shifting the internal summing node. Phase compensation capacitor C2 (47 pF C0G) shunts feedback resistor R2 above 72 kHz, guaranteeing high-frequency stability and blocking RF interference without compromising audio fidelity. The non-inverting input (pin 3) is referenced to ground via DC bias resistor R3 (1 kΩ) to equalize input bias current voltage drops, while capacitor C3 (10 µF) provides an AC noise ground. Series resistor R4 (47 Ω) isolates the op-amp output from capacitive cable loading, and output capacitor C6 (10 µF) ensures clean DC-isolated line-level delivery.

Key Technical Specifications

Closed-Loop AC Gain (Av)-47 V/V (+33.44 dB, 180° phase inversion)
Input Resistor (RI / R1)1 kΩ, 1%, 0.125 W metal film
Feedback Resistor (RF / R2)47 kΩ, 1%, 0.125 W metal film
Frequency Response (-3 dB)15.9 Hz to 72.0 kHz
Equivalent Input Noise Voltage≈ 6.5 nV/√Hz total (5.0 nV/√Hz op-amp broadband)
Power Supply Rails (V+ / V-)±15 V symmetrical split supply (±3 V to ±20 V)
Input Impedance (ZIN)1 kΩ (set by R1 at virtual ground node)
Output Drive CapabilityUp to ±38 mA short-circuit current, drives 600 Ω loads

Theory of Operation & Working Principle

01

Symmetrical dual power rails and dynamic headroom

The NE5532 operational amplifier is energized from symmetrical ±15 V regulated rails (+15 V on pin 8, -15 V on pin 4). These split rails permit the internal Class-AB output stage to swing symmetrical AC audio waveforms up to ±13.5 V peak-to-peak into standard loads without DC rail biasing. Symmetrical supplies eliminate crossover distortion artifacts and maintain wide dynamic range exceeding 110 dB.

02

Virtual ground summing node and inverting gain

The non-inverting input (pin 3) is held at 0 V DC ground potential. Because the NE5532 exhibits high open-loop DC voltage gain (A_OL ≈ 100 dB) and wide 10 MHz unity-gain bandwidth, negative feedback forces the inverting terminal (pin 2) to match pin 3, creating an ideal virtual ground node at 0 V. Signal current generated by the microphone flows across input resistor R1 (1 kΩ) directly into the feedback network. The closed-loop AC voltage gain is governed strictly by the resistor ratio:

FORMULA & CALCULATION
AV = -(RF) / (RI) = -(47 kΩ) / (1 kΩ) = -47 V/V

In decibels, this corresponds to 20 \log10(47) ≈ +33.44 dB of clean voltage gain with 180° phase inversion.

03

AC coupling and low-frequency cutoff

Direct current is blocked from the input transducer by series capacitor C1 (10 µF). Together with input resistor R1 (1 kΩ), capacitor C1 establishes a single-pole high-pass transfer characteristic with a -3 dB low-frequency cutoff frequency:

FORMULA & CALCULATION
fL = (1) / (2\pi × RI × C1) = (1) / (2\pi × 1000\,Ω × 10 × 10^(-6) F) ≈ 15.9 Hz

This cutoff passes the full audible bass spectrum down to 20 Hz with less than 0.8 dB attenuation and prevents low-frequency subsonic handling rumble from driving the amplifier into saturation.

04

Ultrasonic phase compensation and bandwidth limiting

In parallel with feedback resistor R2, ceramic capacitor C2 (47 pF C0G) introduces a feedback zero that rolls off circuit gain above the audible range:

FORMULA & CALCULATION
fH = (1) / (2\pi × RF × CF) = (1) / (2\pi × 47000\,Ω × 47 × 10^(-12) F) ≈ 72.0 kHz

Restricting high-frequency gain prevents RF interference from mobile transmitters and switch-mode power supplies from entering the feedback loop, preserving wide phase margin and ensuring unconditional stability under all operating conditions.

05

Input bias equalization and output cable isolation

The NE5532 bipolar input stage draws input bias currents (I_B ≈ 200 nA typical) through both differential bases. Non-inverting input resistor R3 (1 kΩ) matches the DC source resistance seen by the inverting node (R1 || R2 ≈ 980 Ω), cancelling input offset voltage drift. Capacitor C3 (10 µF) shorts R3 thermal noise to ground at audio frequencies (> 16 Hz). At the output, isolation resistor R4 (47 Ω) de-Q's any capacitive reactance from external interconnect cables, preventing high-frequency output ringing while output capacitor C6 (10 µF) delivers a pristine DC-isolated audio signal.

Design Equations & Calculations

Closed-Loop Inverting AC Voltage Gain

AV = − RFRI

Calculates the closed-loop voltage gain magnitude and phase inversion determined by the feedback-to-input resistance ratio.

SymbolParameterTypical value
AVClosed-loop voltage gain-47V/V
RFFeedback resistor47kΩ
RIInput series resistor1kΩ

Low-Frequency -3 dB High-Pass Cutoff

fL = 12π · RI · C1

Calculates the low-frequency high-pass corner frequency established by input DC blocking capacitor C1 and input resistance R1.

SymbolParameterTypical value
fLLow-frequency -3 dB cutoff15.9Hz
RIInput series resistance1kΩ
C1Input coupling capacitor10µF

High-Frequency -3 dB Low-Pass Cutoff

fH = 12π · RF · CF

Calculates the high-frequency roll-off pole set by feedback capacitor C2 in parallel with feedback resistor R2.

SymbolParameterTypical value
fHHigh-frequency -3 dB cutoff72.0kHz
RFFeedback resistance47kΩ
CFFeedback compensation capacitor47pF

Total Equivalent Input Noise Voltage

en(total) = \sqrt{en(amp)2 + 4 kB T RI + (in RI)2}

Calculates total input-referred equivalent noise voltage density including amplifier noise voltage, resistor Johnson noise, and noise current.

SymbolParameterTypical value
en(total)Total input noise density6.5nV/√Hz
en(amp)NE5532 broadband voltage noise5.0nV/√Hz
RIInput source resistance1.0kΩ
inNE5532 input noise current0.7pA/√Hz

Bill of Materials (BOM)

Every part needed to build this circuit. Select a reference designator to inspect it on the schematic.

RefDesComponentValue / ratingPackageRole in circuitReference
Dual Low-Noise High-Speed Audio Operational Amplifier

Texas Instruments NE5532P, SLOS075K Rev. K; Pin 1 OUT1, Pin 2 IN1-, Pin 3 IN1+, Pin 4 V- (-15V), Pin 8 V+ (+15V).

NE5532PPDIP-8Inverting audio microphone preamplifier stage (Channel A used)Dual Low-Noise High-Speed Audio Operational Amplifier pinout & datasheet
Input Series Resistor

1 kΩ, 1%, 0.125 W metal film resistor. Sets input impedance to 1 kΩ to minimize Johnson thermal noise.

1kΩAxial / 0805Input signal scaling and impedance definition—
Closed-Loop Feedback Resistor

47 kΩ, 1%, 0.125 W metal film resistor. Establishes closed-loop AC voltage gain of Av = -47 V/V (+33.4 dB).

47kΩAxial / 0805Closed-loop voltage gain setting—
Non-Inverting Input DC Bias Resistor

1 kΩ, 1%, 0.125 W metal film resistor. Balances DC source resistance seen by differential input terminals.

1kΩAxial / 0805Input bias current DC offset compensation—
Output Cable Isolation Resistor

47 Ω, 1%, 0.125 W metal film resistor. Prevents op-amp phase erosion and parasitic oscillation under cable capacitance.

47ΩAxial / 0805Capacitive cable load isolation—
Input AC Coupling Capacitor

10 µF, 50 V aluminum electrolytic / bipolar capacitor. Establishes 15.9 Hz low-frequency high-pass corner with R1.

10µFRadial / 1206Input DC blocking—
Feedback Phase Compensation Capacitor

47 pF, 50 V C0G/NP0 ceramic capacitor. Forms 72 kHz high-frequency low-pass roll-off with R2.

47pF0805 / RadialHigh-frequency RF suppression and loop stability—
Non-Inverting Bias AC Bypass Capacitor

10 µF, 50 V aluminum electrolytic capacitor. Shorts thermal Johnson noise of R3 to ground across audio frequencies.

10µFRadial / 1206AC grounding of non-inverting bias node—
Output AC Coupling Capacitor

10 µF, 50 V aluminum electrolytic / bipolar capacitor. Blocks residual DC output offset from subsequent audio equipment.

10µFRadial / 1206Output DC blocking—

Practical Applications & Target Domains

Studio and live-sound dynamic microphone preamplification (150 Ω to 600 Ω transducers)
Low-noise active audio mixer summing and channel gain stage
Balanced audio line receiver and instrumentation acoustic sensing interface
High-fidelity educational reference benchmark for low-noise bipolar operational amplifiers

Critical Design Traps & Engineering Gotchas

Traps found in real builds, with the fix for each.

Critical

Excessive Source Impedance Noise Penalty

Because the NE5532 has a bipolar input stage with an input noise current density of 0.7 pA/√Hz, using source or input resistances above 10 kΩ causes current-induced noise voltage (i_n · R) and resistor Johnson noise to overpower the low 5 nV/√Hz voltage noise.

Mitigation

Keep input resistor R1 at or below 1 kΩ and ensure driving transducer impedance is low (150 Ω to 600 Ω). For high-impedance sources like guitar pickups (> 100 kΩ), use a JFET-input op-amp such as the OPA2134 or TL072.

Warning

Capacitive Cable Loading Output Instability

Driving long shielded audio cables or capacitive loads exceeding 100 pF directly from the NE5532 output creates an additional pole with the op-amp open-loop output impedance (Zo ≈ 50 Ω to 100 Ω), eroding phase margin and triggering ultrasonic parasitic oscillation between 5 MHz and 15 MHz.

Mitigation

Install series isolation resistor R4 (47 Ω, 1% metal film) directly adjacent to the op-amp output pin ahead of coupling capacitor C6 and the output cable terminal.

Warning

Bipolar Input Clamp Diodes Overvoltage Conduction

The NE5532 input stage features internal back-to-back protective diodes across the inverting and non-inverting terminals. In an inverting configuration with large input transients or DC power interruptions, differential voltage exceeding ±0.6 V forces heavy conduction through these diodes, creating sudden input distortion and excessive current draw.

Mitigation

Ensure input coupling capacitor C1 is rated for full supply voltage (50 V) and verify that input signal transients do not exceed the linear operating range. Input resistor R1 (1 kΩ) provides safe current limiting during large overdrive conditions.

Critical

Power Rail Inductive Ringing and High-Frequency PSRR Loss

At frequencies above 100 kHz, the NE5532 power supply rejection ratio (PSRR) degrades significantly. Operating from symmetrical ±15 V rails without local ceramic bypass capacitors leads to high-frequency supply ripple feedthrough and inter-channel crosstalk.

Mitigation

Mount 100 nF X7R ceramic bypass capacitors directly between pin 8 (V+) and GND, and between pin 4 (V-) and GND, within 5 mm of the IC package terminals with low-inductance ground plane connections.

Primary sources

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