by Kevin Gilmore
Grado headphones, for me, are terribly uncomfortable, but my amp sure makes them sound nice. (The ones in the picture are the SR225; I also have a pair of HP-1.) They are the only low impedance headphones out there that I know of. Most if not all of the standard opamp-only headphone amps have trouble driving Grados with any decent bass, because they want a high current output. This amplifier can output up to 0.5W into a 32-ohm load – which is unbelievably loud for the Grados.
I built this headphone amplifier for dynamic headphones based on my rules of proper audio design. People who know my designs will realize that this amplifer is much more than just a headphone amp. It is a pure class A design containing a new never-before-seen servo loop that is not part of the audio signal chain in any way. I should patent it, but in any case, it is “copyright 2001 Kevin Gilmore.”
Kevin’s Rules of Proper Audio Design
- Capacitors in the audio signal path are BAD. Even the best silver-mica or poly caps exhibit non-linearities at low voltage levels. Capacitors belong in power supply sections and nowhere else. Capacitors used to compensate an amplifer generally mean that the amplifier is otherwise unstable, with poles in the right half plane and is therefore a bad design.
- Transformers in the audio signal path are even worse: non-linearities in the gain structure, parasitic capacitance between windings, impedance problems…. Transformers belong in linear power supplies and nowhere else.
- Ultra high open loop gain: REAL, REAL BAD!!! That basically means anything with an opamp in it. Opamp circuits with open loop gains of 10,000 or more require large amounts of feedback to make them usable. While this reduces THD, the intermodulation products, and especially the transient intermodulation products are much higher than they should be.
- Servo loops MUST NOT be in the audio feedback loop. This rule is also very important. Two of my favorite high-end audio electronics manufacturers put servo loops into the minus input of their amplifiers. Most other manufacturers that use servo loops do the same thing. opamps used for servo loops do not have an output impedance low enough to make them suitable for this purpose. Furthermore the dynamic output impedance of opamps adds non-linearities to the audio when put in series with the gain resistor on the minus input.
Kind of makes designing ultra high quality audio stuff tough. My design goals in this amplifier were: keep the gain per stage down, keep all stages in class A, keep the differential front end from coming even close to clipping by the use of a current source. Because the amplifier has a low overall gain and little feedback, a servo helps to prevent DC voltages at the output. In general, if the open loop gain is kept down to eliminate all or most of transient intermodulation distortion, then the amplifier circuitry has to be extremely linear and low distortion. Otherwise, you end up with something that measures and performs like crap.
The schematic for the standard (non-bridged output) version of the headphone amplifier is shown in figure 1. The open loop gain of the amplifer is about 35. Even with the feedback removed, the THD is less than .01%. That’s important because the more linear an amplifier is without feedback, the more the THD, IM and TIM distortions are reduced to unmeasurable levels with feedback added.
Stage 1 is a dual FET fully-differential fully-balanced front-end. The idling current is 2mA total per dual FET (1mA per FET) and 4mA for the complete front-end stage which consists of both dual FETs. The dual FETs generate the bias which runs the second stage, and keeps it and the resulting output section in class A at all times. The FETs are ultra low noise dual units specifically designed for audio uses. The total voltage gain of the first stage is 50.
Stage 2 is the driver stage. It is a standard class A voltage amplifier – in this case used as a voltage shifter. The voltage gain is 0.5 and the idling current 4.3mA.
The push-pull class A output stage is a series of paralleled emitter follower, current buffers. The voltage gain is 0.9 and the current gain is 75. The idling current is 15mA per transistor (or 60mA for the 8 transistors off the +16VDC rail and 60mA for the 8 transistors off the -16VDC rail). I have designed the output section to run at what I have determined is the sweet spot for these transistors, which is 15mA each. Yeah, it gets hot; its supposed to get hot (but not hot enough to require heatsinks). It’s not possible to make an amplifier with an output impedance less than 0.1 ohm without throwing around a fair amount of current.
The servo circuit is new: most of the servo designs (Mark Levinson and Krell, for example) put the output of the DC servo back into the – leg of the amplifier. I just do not like this. That puts the noise and non-linearities of the opamp inside the audio loop.
My servo feeds back to the current sources for the dual FETs in stage 1. Like all servos, it is an integrator. Due to the large (relatively) integration capacitor and the 1 meg resistor, the frequency of this filter is 0.05 Hz. With even a decent opamp, the servo’s noise is in the tens of microvolts, and does not affect the operation of the current sources significantly.
The servo opamp in this amplifier measures the DC at the output, if any, integrates it and applies it to the midpoint of the two LEDs. The LEDs do have a slight change in voltage with respect to current, about 3 or 4%, and that is enough to make the servo work. Notice that if the transistors or the resistors are very poorly matched, the servo will not work because its total control range is at most 10%. Most standard servos (such as the Mark Levinson or Krell servos) have a much wider range.
For high impedance headphones, a little DC will not hurt the phones. With the low impedance Grados, even 0.1VDC over a long period of time will definitely damage and/or change the sound. If all the parts are hand matched, the power supplies are exactly the same and all the resistors are really good quality, the amp should be stable and should not drift. In that case, the servo could be omitted or replaced with a 20K trimmer pot wired from +16VDC to -16VDC, with the wiper going to the DC adjust pin. The prototype uses 0.05% tolerance resistors, and I hand-matched the transistors. The output DC is less than 6mV and has stayed absolutely stable for the few months I have had the unit.
The amp gives about 0.5W into 32 ohms. In the classical definition of class A, the top transistors would be sourcing 120mA and the bottom transistors sinking 0mA. However the two 3k resistors in the second stage actually prevent the total shutdown of either transistor bank by keeping the opposing stage at an absolute minimum of 5mA. In any case, 0.5W into Grados is unbelieveably loud.
The balanced bridge output version of the amplifier (figure 2) is for those headphones that can be wired as dual mono (see the addendum for instructions on converting a pair of standard Grado SR-80 headphones into dual mono headphones). It has twice the voltage swing, twice the slew rate and 4 times the output power (competes with the $2600 HeadRoom balanced Max amplifier).
The ultra-regulation of the power supply (figure 3) is so over the top and unnecessary that most, if not all, people building this amplifier would not even notice the difference. However there are a number of benefits to this design. First its a dual tracking design. Because the open loop gain of the amp is low, its common mode rejection due to the power supply is not great. However if both the + and – voltage rails move up and down the same amount, there is no bias drift.
Because of the pre-regulators, the total line/load variations are under 0.0001%. The fast capactors allow the power supply to react rapidly and in a controlled manner with highly reactive loads like the Grados. The opamp outputs are active in both directions; they can push or pull to keep the power supply at exactly the right point. The power supply design was an attempt to come up with the absolutely best power supply I could. It is even quieter than batteries.
Download high resolution images of PCB pattern and layout 1
Download high resolution images of PCB pattern and layout 2
The prototype was built with point to point wiring, keeping it tight and tiny. The layout is exactly as shown on the schematic, which is also why the board is only one layer. Although the amplifier is easy to build without a PC board, I designed one for the amplifier. Each board (you need 2 for the standard amplifier or 4 for the bridged version) is 3.3″ x 3.8″. In a few months, I may redo the board in one of the systems where I can ship the file over the internet and get boards back (like expresspcb.com).
The servo’s total control range is at most 10%, so the some of the servo-related parts must be closely matched for optimal operation of the servo. The 500 ohm resistors, 1.6V LEDs, bias transistors and second stage transistors must be matched to within 0.5% or even 0.25% for optimal operation of the servo (the dual FETs are already matched). To match the LEDs, put one in series with a 10k resistor, hook it to 15VDC and measure the voltage across it. Do it to a few of them and pick the closest match.
I used a Tektronix curve tracer to match the transistors. Figure 4 shows two circuits for matching the beta (gain) of the NPN and PNP transistors using just a voltmeter. Simply measure (and match) the voltage of each transistor’s collector with respect to ground. It should be in the range of 10V to 11V for the NPNs or 5V to 6V for the PNPs.
There are no substitutes for the FETs. The PNP and NPN transistors in the prototype were the MPS8099 and MPS8599. Onsemi has discontinued them, but there are still lots available. I am buying all my transistors now over the web from MCM Electronics. I have had too much trouble with everyone else. The 2SA1015 PNPs are $0.46 each; the 2SC1815 NPNs are $0.41 each. The 2SJ109 p-channel dual FET is about $6.50; its n-channel counterpart is $5.90. By the time you add it all up, it’s still under the minimum MCM order, so you’ve got to buy something else.
The high-speed 5uF capacitors in the power supply are not critical. They satisfy the “lunatic fringe” in audio. These capacitors are rated for a slew rate (dv/dt) of about 4 times a standard capacitor. They cost $7.50 from the Illinois Capacitor Company. Similarly, the opamps in the power supply are not critical. In the prototype power supply, I used the Apex PA09, which has a 400V/uS slew rate and costs $167 each (remember, I am crazy). Normal people should use the Texas Instruments OPA549 (10V/uS) that cost $11 each. The LM3xx regulators are heatsinked (dissipating at least 3W each, 6W for the bridged version of the amplifier).
The enclosure is the Mod.U.Line by Precision Fabrication Technologies Inc. (part number 03-1209-BW), available from Newark Electronics. They are about $85 a piece these days. The aluminum enclosure is easy of use, easy to punch, and keeps a decent paint job. The headphone jack is a cheap Radio Shack one. Although it works fine. I have since gotten some Neutrik connectors which I will put in at some point. In theory, there is a ground loop between the RCA jacks on the back plate and the headphone jack on the front plate. Although the 60 Hz hum is about 110 db down, the Neutrik jacks are isolated and will make this problem go away.
The amplifier’s output is voltage limited (not current limited) because the second stage runs out of voltage swing – typically about 6V rms. For a 32 ohm load, the maximum output power is 1.125W (0.1875A). For a 300 ohm load such as the Sennheiser HD600, the maximum output power is 0.125W (0.02A). To increase the maximum output voltage to, say, 10V rms, try increasing the power supply to ±20VDC and change the 500 ohm resistors in the current sources/sinks to 600 ohms (or ±24VDC and 700 ohms – but careful not to fry the output transistors).
The bridged version will output 4.5W into the 32-ohm Grados and 0.5W into the 300-ohm Sennheiser HD600. At full blast, the amp does drop out of class A, but at levels that will fry your ears anyway.
Adjustments: In the power supply, adjust the top 20K trimmer pot for +24 volts at the tap after the LM317. Then adjust the bottom 20K trimmer pot for -24V at the tap after LM337. (Note: the ±48V taps are shown for reference only; they are not actually used by the amplifier.) If the servo has been replaced with a 20K trimmer pot, adjust the trimmer so that the output measures 0VDC. Anything under 25mV is fine.
I listened to the balanced HeadRoom Max at The Home Electronics Show. The low frequency bass slam is absent from the unit. When I listened to the BlockHead ($3333) and compared it to my unbalanced/balanced amp, the same thing happened. Without the kaboom, it’s just not as much fun to listen to.
This amp gives the Grados and Etymotic Canalphones a fuller and much more upfront sound than the built-in headphone jacks on various players – the bass has a snap to it that it never used to have. And the image moves from around your head to the center of your nose. The Etymotics tend to sound kind of thin and distant with other amps. In general, I have to say that this amp produces bass that is much more solid – similar to putting the microphone in front of a bass violin instead of inside it.
c. 2001, Kevin Gilmore.
From The Homepage of Kevin Gilmore. Republished with permission.
10/25/2001: The author provides instructions for converting a standard pair of Grado SR80 headphones into dual-mono headphones for use with the bridged version of the dynamic headphone amplifier. He writes:
Dual mono Grado SR-80s have more and tighter bass when driven with the bridged dynamic amplifier, which can output twice the voltage, twice the current (not at the same time) and double the slew rate, giving better control of the diaphragm and a higher damping factor.
I cut apart a pair of Grado SR-80s. I had to take them apart anyway – one side was damaged by my toy terriers. There are two ways to wire Grados for dual mono operation: the easy way and the harder way. The easy way is to cut the wires just above the “Y” of the headphone cord. Carefully splice new mono connections to each of the wires.
The hard way is to take the headphones completely apart and rewire all the way to the transducers.
- Take the transducers out of the headband.
- Take the ear pads off.
- Very carefully, with a sharp jeweler’s screwdriver, pry around the side seal. It is superglued in only a couple of spots. Comes apart real easy.
- Buy a set of 20-ft, 1/4″ headphone jack extender cables from Radio Shack. Cut one end off at the length you want and then solder to the transducer. I use the tip and sleeve part of a stereo 1/4 jack, and leave the ground connection unconnected.
- On the amplifier, use 2 separate stereo 1/4″ headphone jacks (one for each channel) and wire the tip and sleeve to match the headphone plugs. The ground sleeve IS connected to ground in the headphone jacks only (actually decreases the noise level a bit).
1 thought on “A Pure Class A Dynamic Headphone Amplifier.”
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