The Very Simple Phono Stage
This page decribes the original version of the VSPS circuit. The parts values and parts numbering are a little different in the current versions I have available on the products page. R3 has been removed, the resistors renumbered, and the frequency response has been tweaked slightly.
Presenting a simple, versatile phono stage for moving magnet or high output moving coil cartridges using a bare minimum number of parts and the following features:
- 27 parts per stereo unit. Low parts count makes it cheap to build and easy to optimize.
- Wide choice of op amps. Just about any op amp can be used in this circuit.
- Accurate RIAA equalization obtained using common, standard value components. Uses Allen Wright's modified curve, with the additional zero at 3.2 µS.
- User variable gain. The circuit can be easily adapted to work with moving magnet and medium-to-high output moving coil cartriges.
- Low power consumption.
- Single stage, active equalization, non-inverting topology.
This circuit is appealing for beginners, of course, but the simplicity also offers more experienced builders the chance to evaluate and optimize each individual part. Taking my cue from 47 Labs I would also like to think there is an inherent benefit of a simple circuit, sonically, coming from the tighter layouts and better grounding arrangements - the direct result of having fewer parts to deal with. The VSPS is the most popular circuit I have developed, many people have successfully built it. Its proved to be an amazingly rugged and reliable project, coming up with the goods again and again.
The Amplifier Circuit
An op amp is configured as a non-inverting gain stage. The RIAA equalization is done within the feedback loop. This is a classic circuit, but not seen too often in DIY since calculating the values of resistance and capacitance needed can be a pain. Modern software like MathCAD makes this task a breeze, however.
This circuit has two fundamental problems both of which are neatly circumvented by adopting the Allen Wright RIAA response curve.
The first issue is the limitation that the gain of a non-inverting amp cannot fall below unity. In principle the RIAA response calls for the high frequency attenuation to decrease by 6 dB per octave, so at some point the op-amp cannot provide sufficient attenuation to properly track the response. With the AW curve, however, this treble cut is deliberately defeated at 50 kHz so the treble reponse is kept above unity provided the total mid-band gain is set greater than 30 dB. (It levels off at about +12 dB in the standard configuration.)
The second disadvantage concerns the impedance of the active filter: without R3 the impedance of the feedback loop approaches zero at high frequencies. (The capacitor C1 essentially becomes a short circuit.) The op-amp, under these conditions, drives R2 directly in parallel with the output load. The output signal will have high distortion if R2 is lower or close to the op amps optimum load resistance. This is avoided by adding resistance R3 in series with C1 to set up the fourth 3.18µs time constant. The high frequency impedance of the feedback loop is now R2+R3 = approx. 3k. Whether or not the Allen Wright correction is legitimate or not (recently it has come into doubt) R3 still fulfills a useful purpose.
The circuit is otherwise so basic that each component can be discussed individually.
|R1||47k||This resistor (and optional capacitor) should be set as directed by the cartridge manufacturer.|
|R2||680R||This resistor sets the gain. Lower values result in more the gain. Use 2.2k for 30dB, 680R for 40dB, and 220R for 50dB.|
|R3||2.2k||Allen Wright Mod., cuts treble attenuation above 50 kHz. If you adjust R2, R3 must also be changed according to the following formula [R3 = 3000-R2], rounding to the nearest convenient value. (The exact value is not critical.)|
|R4||110k||RIAA. Match between channels. Use 105k if available and increased accuracy is desired.|
|R5||750k||RIAA. Match between channels. Use 732k if available and increased accuracy is desired.|
|R6||47R||Isolates the op amp from the effects of output lead capacitance.|
|R7||33k||The value of this resistor isn't critical, it mainly serves to drain off charge from the output side of C3.|
|C1||1.00n||RIAA. Match between channels.|
|C2||3.00n||RIAA. Match between channels. Use 3x 1nF in parallel.|
|C3||2.2µ||Output coupling. Must be non-polar.|
|U1||NE5534 or OPA134||Any audio op-amp could be used with satisfactory results. Stereo layouts require dual op-amps e.g. NE5532, OPA2134.|
RIAA values shown in bold. With these exact numbers the response is accurate to ±0.1 dB. Increased accuracy can be obtained by using 1% resistors, 105k for R4 and 732k for R5. Since these are hard to find and not available in carbon film, I suggest using the standard the values of 110k and 750k instead. Unless the capacitors are within 1% of the list value there is no point worrying about the extra accuracy of the resistors.
As seen in the simulation, the Allen Wright modification boosts the treble by 0.5 dB at 20 kHz, a modest change by any measure (blue trace). The VSPS follows this modified response (red trace).
The phono preamplifier circuit is powered by regulated, low noise, split 12 V supplies. Normally the voltage regulation and filtering is placed on the same board as the phono circuit. The power transformer and rectifier diodes are typically in a separate chassis connected by an umbilical cable. The Construction Guide explains how to put everything together.
Boards are available, see the products page page for details.
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