There are a multitude of options in obtaining a phono preamplifier with a flat frequency response suitable for needle-drop recording and subsequent processing in Stereo Lab.
These range from low-cost, DIY solutions and our unique Virtual Preamplifier to active preamplifier adaptors, to precision preamplifiers with laboratory-standard accuracy and dynamic-range provided by our partner company Phædrus Audio.
For vinylistas who use moving-coil cartridges with Stereo Lab, there are a range of options.
At its most basic, you can experiment without any sort of phono preamp at all, and simply apply the output of the phono cartridge to a commercial external pro-audio interface like the one illustrated below and apply the pickup signal to an interface via the microphone inputs.
This options is illustrated in the diagram below.
The microphone input will work for moving-coil (MC) cartridges which have a great deal in common with dynamic microphones (moving-coils and ribbons), albeit with a signal about 4 times lower than a typical moving-coil microphone.
Acceptable results may be obtained if the microphone preamp' is well designed and the cartridge leads can be fed balanced to the microphone inputs with the shield derived from the turntable chassis and arm tubing. Even single-ended will work if care is taken to keep leads short, well made and away from sources of interference. But this solution is likely to lead to noisy recordings.
Moving magnet (MM) cartridges are more problematic. Because of their inductive source impedance, the low-Z microphone inputs will load the moving-magnet motor unacceptably and this results in completely unsatisfactory recordings.
In either case, when connecting a phono cartridge to the microphone inputs of a sound-card, never energise the +48V phantom power. To do so will damage the cartridge irreversibly.
Happily, Stereo Lab (Phonograph & Audiophile) Ver. 3.1.15 incorporates a Virtual Preamplifier which adapts microphone inputs in software, so that moving-magnet cartridges may be used for needle-drops without any preamplifier being necessary.
The Virtual Preamplifier is accessed via the Modern Equalisations processing mode menu.
Performance of the Virtual Preamplifier is heavily dependent on the quality of the soundcard. Tested with a representative of modern, excellent-value, external soundcards (Focusrite Scarlett 2i2 Interface) and a typical MM cartridge (Gold Note Vasari Gold), frequency response is 20Hz - 20kHz (±2dB) and noise is some 30dB below LP surface noise - very good results.
There are some disadvantages to the Virtual Preamplifier approach because only RIAA recordings are suitable and the pop & click processing is not effective. The virtual approach will not work either for JVC CD-4 quadraphonic discs because they require a wide bandwidth preamplifier.
A better solution for collectors with a wide variety of discs is one of the Groove Sleuth Adaptors of the Groove Sleuth Preamplifier.
Phædrus Audio Groove Sleuth Adaptor preamplifiers were developed to convert the XLR socket microphone inputs on commercial computer sound cards to non-equalised phono cartridge inputs.
Commercial soundcards designed for the highly competitive musical instrument and recording sector often integrate excellent, low-noise preamplifiers and fast, high-resolution (24 bit) analogue-to-digital converters to convert the analogue signals so that they can be recorded into the computer at sample rates up to 192 kHz. They therefore make the basis of an excellent and good-value capture front-end for Stereo Lab software. At least, they do almost.....
The problem is that the preamplifiers are microphone preamps, not phono preamps. They have more than enough gain to raise the output from a phono cartridge to line level. But microphone inputs do not present the phono cartridge with the correct impedance and attempting to connect a phono cartridge directly to a microphone input will destroy the high-frequency response because the impedance mismatch isn't small, it's wrong by nearly two orders of magnitude!
Phædrus Audio Groove Sleuth Adaptors ensure the phono cartridge and the microphone inputs are presented with the appropriate signal levels and impedances. The 48V phantom-power for microphones is remodelled to power the miniature Groove Sleuth Adaptor preamplifiers.
Groove Sleuth Adaptors are designed to work with Pspatial Audio’s Stereo Lab software. With a wide frequency-response and deep dynamic range, they offer a very high-quality solution for recording non-equalised needle-drops at a reasonable price.
Three versions exist of the Groove Sleuth Adaptors, their roles are as follows:
Go to Phædrus Audio for more information. Or contact email@example.com to order Groove Sleuth Adaptors.
Download the manual for the Groove Sleuth Adaptor preamplifiers.
The Groove Sleuth MICRO non-equalising phono preamplifier is the diminutive alternative to the Groove Sleuth Mk. II.
The Groove Sleuth MICRO preamplifier is suitable for all high-output moving-coil and moving-magnet cartridges. It is also suitable for Phædrus Audio PHLUX II active moving-magnet cartridges (add the PHLUX-Bridge order option).
For use with moving-coil cartridges, the MICRO may be partnered by the Groove Sleuth TRANSFORMER
Like the Groove Sleuth Mk. II preamplifier, the Groove Sleuth MICRO preamplifier incorporates the very low-noise battery supply. This means the preamplifier can be powered from a conventional, international-style power supply but be switched to battery supply during operation to ensure the very best possible noise and distortion performance. This delivers first-rate quality at a very reasonable price.
A switch on the front-panel allows the battery supply to be selected. The Groove Sleuth MICRO preamplifier has over 4 days operational charge, but we recommend battery play be limited to approximately 12 hours. The unit may be kept in charge mode when listening with only a minute loss of quality.
Further information about the Groove Sleuth MICRO preamplifier is available from Phædrus Audio.
Lastly, a good solution - if you are practical - is to build a flat-response preamplifier or modify an existing phono preamplifier unit so that it has a flat response and then apply the output of this to the computer audio interface/ sound-card at line-level. Here, we cover the build of flat preamplifiers and the necessary modifications to pre-existing phono preamp's.
A commercial phono stage is a good starting point for modification because the designer will have taken the trouble to provide high-quality amplification, low-noise circuitry, decent power supplies and the correct cartridge loading.
"Strap the big capacitor; remove the little capacitor.....is the golden rule!"
RIAA correction may be implemented in various different ways. In a passive circuit: or in an active circuit, in which the frequency-dependent impedance is part of a feedback network. It may be implemented with discrete transistors, or valves (tubes), or with operational amplifiers. But in all these various incarnations, the modifications may usually be accomplished with a little detective-work and care.
The figure right illustrates a typical passive configuration of an RIAA equaliser. The necessary modifications are marked in red. As you can see, the golden rule is.....Strap the big capacitor; remove the little capacitor.
By these simple means, the RIAA correction is modified to give a gain a few dB from the 1kHz reference point so that neither noise, nor overload margin of the preamplifier is compromised. The only practical thing to watch out for is that the capacitors (both the larger value and the smaller value) may be made out of several discrete components so that the designer could get a special value.
A discrete-BJT feedback stage is modified in a very similar way: the larger-value capacitor is strapped (bridged out of circuit) and the lower value of the two capacitors is removed from circuit. If you keep hold of the lower value capacitors (or tape them to the inside of the unit for safekeeping), the preamp' may easily be returned to its original design if you wish to do so at a later stage.
Op-amp circuits are similar too, as illustrated below. Most modern RIAA preamplifiers will be of this type.
Building your own battery powered needle-drop flat-response preamp is certainly possible. Remember, all that is needed is some gain: it's not like it needs precision equalisation. RIAA (or other) EQ on the baseband signal is all accomplished in the software.
It is possible to use something as simple as the attached little circuit to very good effect. It's built around a dual op-amp which could be something as modest as a NE5532. We prefer the recommended OP284EPZ. It's a lot more expensive (10 Euros), but it's rail to rail which gives better headroom and has a low quiescent current which prolongs battery life.
The gain is 33dB which is more than adequate to drive sound cards from the majority of MM cartridges. Note that the value of R1 can be changed. Some older CD-4 cartridges prefer loads >47k. This can go as high as 470k to give an input R of 100k.
Moving-coil (MC) cartridges have a voltage-output about one-tenth that of the moving-magnet (MM) type. Rather than adapt the main preamplifier to provide for the higher gain, the best engineering approach¹ is to precede the standard MM preamplifier (such as those described above) with a head-amp to raise the signal of the moving-coil cartridge to a level similar to the MM type.
For vinylistas who want to use moving-coil cartridges with Stereo Lab, there are a range of options:
Groove Sleuth TRANSFORMER
Housed in the same diminutive chassis as the Groove Sleuth MICRO preamplifier, the Phædrus Audio Groove Sleuth TRANSFORMER includes a pair of step-up transformers to extend the range of the Groove Sleuth MICRO, (or any other standard MM preamplifier) to include all moving-coil and moving-iron cartridges.
By incorporating a range of high permeability, nickel-iron alloy cored transformers (fitted as a time-of-order option), the Groove Sleuth TRANSFORMER can adapt to the complete range of cartridges: from high-end, low-output devices; to high-output moving-coils which rather "under-load" standard MM input stages without a transformer.
Click for more information about the Phædrus Audio Groove Sleuth TRANSFORMER.
There are few examples in modern, small-signal electronics where integrated op-amps don't outperform discrete circuitry. Suprisingly, even in the second decade of the 21st century, moving-coil phono head-amps remain an exception. This circuit is based on a design by Nordholt and Van Vierzen from 1980 and published in the Journal of the Audio Engineering Society¹.
The amplifier circuit illustrated is a straightforward complimentary-transistor pair amplifier. Gain is defined by 1 + the ratio of R3 to R8; or 11 times (21dB). There is a small amount of loss due to the termination resistor (R23), so the overall gain for a cartridge with a source impedance of 10Ω is 10 (20dB).
Termination in 100Ω is a very common choice for MC cartridges and is a good starting point. There is scope for some experimentation and some manufacturers recommend a different value for their products.
The second 2N4401 input transistor is there to reduce the noise generated in the intrinsic base-spreading resistance (rbb) of the transistor. The 2N4401 is chosen as the input device because of its low base-spreading resistance and putting two devices in parallel reduces rbb still further. Theoretically, there is no limit to this process so that 3 transistors will be better than 2 and so on. However, in test, whilst the second device improved the noise by a worthwhile 1dB, beyond this, the law of diminishing returns set in very quickly, so there is little point in going beyond a pair of devices. The preferred commercial transistor type in the original article¹ is the RF transistor BFW16A, but these are now rare and expensive. The 2N4401 is cheap and available from most component retailers.
Circuit harmonic distortion is very low. For a 1kHz input signal of 5mV RMS which is representative of the largest signal encountered, the distortion is less than -80dBc (0.01%)² and essentially all 2nd harmonic.
The frequency response demonstrates less than 0.1dB variation from 20Hz to well above 100kHz into the MHz. (The low impedance circuitry ensures that frequency response exceeds anything required for audio.)
Wideband noise, measured at the output with a 10Ω source, is 1µV RMS in a bandwidth of 20kHz. This gives an EIN of -138dBu or 74dB below nominal level from the cartridge. In op-amp terms we'd say that the amplifier has a input voltage-noise of 0.7nV/√Hz. That's 4dB better than any of the best, low-noise operational-amplifiers.
Overload margin is enormous. The amplifier will comfortably swing 2V pk-pk (0.7V RMS), which requires an input signal of 70mV RMS which is 43dB above nominal level. Adding 74dB and 43dB, we can say that the amplifier has a dynamic range of ≈ 117dB; equivalent to 20 bit resolution.
DC bias is set by R5 and R2. DC conditions proved very stable in production and the circuit operates acceptably over a wide temperature range of 0° to 40°C ambient.
Although the power supply voltage requirement modest (a single-rail ≈5V supply), the power-supply voltage must be smooth and quiet. This amplifier pulls about 21mA so, the total current-requirement for a stereo pair is ≈ 42mA³.
For prototyping (and for use, as long as the batteries are changed every 50 hours or so) a 4.5V flat, alkaline battery makes a very good temporary supply. If you want to stick with the battery as a permanent solution, then drop the value of R2 to 3.9k.
1. Ultra Low Noise Preamp For Moving-Coil Phono Cartridges. Nordholt, E.H and Van Vierzen, R.M JOURNAL OF THE AUDIO ENGINEERING SOCIETY, 1980 APRIL, VOLUME 28, NUMBER 4
2. dBc means dB relative to carrier. Although mainly a term used in RF engineering, here it describes the second harmonic amplitude relative to the amplitude of the test sinewave. Because the term employs decibels, which more nearly mimic the logarithmic response of the hearing system, dBc works better to describe relative importance of distortion than using percent.
3. One of the surprises about with moving-magnet head-amps is that — despite signal levels measured in µV — the necessity to keep all of the circuit elements low-impedance to minimise noise contribution, ensures that the (Class-A) circuits run in much higher standing-current than one expects from circuits carrying such tiny signals.
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