The broadband amplifier NE592 can be used also for building a simple selective audio amplifier. By means of the +6 V and +12 V supply voltages, a DC coupling between the product detector and the AF amplifier is possible. The DC level at the differential inputs is about 4.5 V. The mixer drives the differential input of the NE592 - after suppression of the RF proportions by two 47 nF capacitors - with the remaining AF signal. RF blocking between the outputs is feasible with only one capacitor, but not between the single outputs and ground. But the latter is absolutely necessary due to the wide amplifier bandwidth. The AF stage offers a gain of 200 (46 dB) at 660 Hz center frequency. Headphones with Ri > 1 kOhm are mandatory due to the relatively high output resistance of the NE592 amp. 18 mA quiescent current isn't low, but it is insignificant in case of stationary operation and supply by a small ac-operated power supply. You can reduce the AF stage current consumption down to 2 mA when using a dual op amp TL072/082 instead of the NE592 broadband amp. These consumer op amps have a lower output resistance, so that they are able to drive 2 x 32 ohms headphones connected in series with a 470 ohms resistor. When using a NE5532, no additional resistor is necessary because the outputs have a less lower impedance. The transfer characteristic is the same as the one displayed for the first circuit (AF amp with NE592). Low distortion, CW selectivity, high gain, low noise, and a high output voltage are the features of the following circuit. This circuit is seldom used despite its good characteristics. The latter is perhaps because of the fact that one must try different resistance values for R4 and R5 depending upon the quiescent current through IC1. This is okay for building a single device but not acceptable for a series product.
The NE592 broadband amplifier is a versatile component suitable for constructing a selective audio amplifier with high-performance characteristics. The circuit operates with dual supply voltages of +6 V and +12 V, enabling DC coupling between the product detector and the audio frequency (AF) amplifier. The differential inputs of the NE592 are set at a nominal DC level of approximately 4.5 V, facilitating optimal performance.
In the configuration, RF interference is mitigated through the use of two 47 nF capacitors, which filter out RF components before the AF signal is applied to the differential input of the NE592. Additionally, RF blocking between the outputs can be achieved with a single capacitor; however, it is crucial to maintain isolation between the outputs and ground to prevent distortion, particularly due to the amplifier's wide bandwidth.
The audio frequency stage of the amplifier is designed to provide a gain of 200 (46 dB) at a center frequency of 660 Hz, making it suitable for various audio applications. It is important to note that headphones with an impedance greater than 1 kOhm are recommended due to the relatively high output resistance of the NE592. The quiescent current of 18 mA is manageable in stationary applications, especially when powered by a compact AC-operated power supply.
For applications requiring lower power consumption, the use of dual op-amps such as the TL072 or TL082 is suggested, which can reduce the AF stage current consumption to 2 mA. These op-amps possess a lower output resistance, enabling them to effectively drive headphones with lower impedance, such as 2 x 32 ohms when connected in series with a 470-ohm resistor. Alternatively, the NE5532 can be utilized without the need for an additional resistor due to its inherently lower output impedance.
The circuit exhibits low distortion, excellent continuous wave (CW) selectivity, high gain, low noise, and a high output voltage. Despite its advantageous features, the circuit is not commonly implemented, possibly due to the requirement for adjusting resistor values R4 and R5 based on the quiescent current through IC1, which complicates mass production compared to single prototype devices.
This comprehensive description outlines the functionality and design considerations of the NE592-based audio amplifier circuit, emphasizing its capability to deliver high-quality audio amplification while addressing potential challenges in component selection and circuit implementation.The broadband amplifier NE592 can be used also for building a simple selective audio amplifier. By means of the +6 V and +12 V supply voltages a DC coupling between the product detector and the AF amplifier is possible. The DC level at the differential inputs is about 4,5 V. The mixer drives the differential input of the NE592 - after suppression of the RF proportions by two 47 nF capacitors - with the remaining AF signal.
RF blocking between the outputs is feasible with only one capacitor, but not between the single outputs and ground. But the latter is absolutly necessary due to the wide amplifier bandwidth. The AF stage offers a gain of 200 (46 dB) at 660 Hz center frequency. Headphones with Ri > 1 kOhm are mandatory due to the relatively high output resistance of the NE592 amp. 18 mA quietscent current isn't low, but it is insignificant in case of stationary operation and supply by a small ac-operated power supply.
You can reduce the AF stage current consumtion down to 2 mA when with a dual op amp TL072/082 instead of the NE592 broadband amp. These consumer op amps have a lower output resistance, so that they are able to drive 2 x 32 ohms headphones connected in series with a 470 ohms resistor.
When using a NE5532 no additional resistor is necessary, because the outputs have a less lower impedance. The transfer characteristic is the same as the one displayed for the first circuit (AF amp with NE592).
Low distortion, CW selectivity, high gain, low noise and a high output voltage are the features of the following circuit. This circuit is seldom used despite its good characteristics. The latter is perhaps because of the fact that one must try different resistance values for R4 and R5 depending upon the quiescent current through IC1.
This is ok for building a single device but not acceptable for a series product. Parts Value
R1 10 kOhm
R2 8,2 kOhm
R3 1,8 kOhm
R4, 5 390 Ohm
R6 47 Ohm
R7 470 Ohm
R8 4,7 kOhm
C1,4 47 uF, electrolytic cap. C2 10 uF
C3 2,2 uF
C5 150 pF
C6,7 100 uF, electrolytic cap. C8 220 pF
P1 10 kOhm, linear
Dr1 33 mH
VT1 2N3906
VT2 2N3904
IC1 NE592 🔗 External reference
The circuit is a preamplifier with digital regulation intensity of sound. It is separated into three departments. The first schematic (Fig.1) shows the control circuit of the electronic potentiometer. The control is achieved through two pressing switches. The S1...
A simple linear voltage-controlled amplifier can be constructed with one operational amplifier (op amp) and two junction field-effect transistors (JFETs). This amplifier can achieve an 80-dB dynamic control range with less than ±0.2% linearity error for 0 V.
The described...
A magnetic pickup from an old record player can function effectively as a pressure and vibration sensor. By replacing the needle with a thin metal plate (copper from a PCB is suitable), an excellent touch sensor can be created....
The TDA 2030 is a widely used 14W audio power amplifier monolithic integrated circuit in a Pentawatt package, intended for use as a low-frequency Class AB amplifier. Some home theater prototypes utilize the TDA 2030 as a low-frequency subwoofer...
A small headphone amplifier is a valuable device capable of driving multiple pairs of headphones. The headphone amplifier's task is simplified due to the relatively low output power requirements and the manageable load characteristics. Headphones generally have an impedance...
The circuit is straightforward yet capable of excellent performance. It has been specifically designed for use as an amplifier for the digital sound card in a computer. Audio input can be sourced from any two-channel line-level device such as...
We use cookies to enhance your experience, analyze traffic, and serve personalized ads.
By clicking "Accept", you agree to our use of cookies.
Learn more