Assembly Tips

Hookup Wiring

You may have noticed that the wire pads are not placed where they might be closest to the panel where each component is most likely to be placed. For example, the audio input jacks are usually on the back panel, yet the input pads are near the front of the board. The reason is that when laying out the components on the board, we favored short traces and a minimum of layer changes to layouts that would have made for shorter hookup wires.

We made this tradeoff because hookup wires are flexible. Bad sound due to a poor PCB means you have to throw out the whole PCB, but bad sound due to suboptimal hookup wiring is fixable by using a better hookup scheme.

It is possible that these longer hookup wires could act as antennas, bringing interference into the amplifier. I haven't found any such problems in the amps I've built on this board. If you do encounter a problem, the single easiest and most effective fix is to twist related wires together: the wires going to each set of input or output jacks, for example. You could also look into things like rerouting each wire's path from board to panel component.

During the prototype process, I took a pair of "naked" amps (no cases) to RFI Hell. I live in rural New Mexico, in a county of about 100,000 people. So, every TV, radio and microwave antenna in the whole area is up on single bluff overlooking the area's major city (pop. 40,000). I parked my car within sight of 12 towers, most of which had multiple antennas on them. All of these antennas were close by — the furthest was probably less than 200 yards away. My car stereo was doing funny things in the middle of this RF bath; if my house were up there, I would be worried about having Funny Lookin' Kids. To cut this long story short: I got no hum, no hiss, no AM radio through the headphones, just dead silence, even with the volume control cranked all the way up and high-efficiency headphones plugged in. I drove back and forth through the area a few times, and heard no change at all through the headphones. Satisfied, I spent an hour watching the traffic going by while I listened to some tunes. :)

Configuring the Amplifier Topology

The four feedback resistors — R3/R4 and R5/R6 — act in pairs to set global and local feedback, respectively. They set the gain for each amplifier, and they also have an influence on the noise behavior and stability of the op-amp chip.

Depending on how you populate R3 through R6, you can set up one of three different amplifier topologies. In increasing order of preference, they are as follows:

Buffer outside the feedback loop (local feedback only) — This is like a CMoy amp with an EL2001 acting as a voltage follower after the voltage amplification stage. To set this up, leave R4 unpopulated, jumper across R3, and pick values for R5 and R6 to set your amplifier's gain. You can also leave the output buffers out and jumper across their position (pin 2 to 7) which turns the META42 board into a kind of über CMoy.

Buffer inside the feedback loop (global feedback only) — This makes the buffer and the op-amp act together as a single system, which helps control errors. To set this up, leave R6 unpopulated, jumper across R5, and pick values for R3 and R4 to set your amplifier's gain.

Jung multiloop (global and local feedback) — (Named after the inventor, Walt, Jung.) This configuration uses all four positions, which sets up a configuration that minimizes all sources of error and distortion under our control. (See the original article for details on how this is accomplished.) The R3/R4 pair have the main contribution to the overall system gain, so pick them as though you were configuring the amp for global feedback only. See the next section for information on how to pick values for the inner loop.

Optimizing the Loops in a Multiloop-Topology Amplifier

The gain of the inner and outer loops are more or less independent. Changing the inner loop's gain usually won't change the overall system gain very much at all. The amplifier's "real" gain is configured by the outer loop. Use the multiloop gain calculator to be sure, though. There are edge cases where the inner loop's gain can affect the overall system gain significantly.

The purpose of gain in the inner loop (R5/R6) in a multiloop topology is to optimize the bandwidth of the op-amp. For voltage-feedback op-amps (the typical kind), gain and bandwidth have a linear relationship. That is, increasing gain by a factor of, say, 10 will decrease bandwidth by a factor of 10. The op-amp's datasheet will have a spec called the gain-bandwidth product (GBP) which expresses this relationship. If the GBP is 16 MHz, then with a gain of 100, you will get 160 kHz of bandwidth.

So, how is this useful? Since we're only interested in the audio bandwidth (5-30,000 Hz, generously speaking), what use is an 80 MHz op-amp? Partly we're interested in the higher slew-rate a high-bandwidth op-amp gives us. The downside is that high-speed op-amps are harder to make stable. Since we don't actually need more than about 30 kHz of bandwidth, can we have our cake and eat it, too? Yes. If you intentionally raise the gain high enough that you get bandwidth down into the 100 kHz range, the op-amp retains its high slew rate while reducing its bandwidth. Lower bandwidth means immunity to ultrasonic noise (i.e. most electrical interference) and greater phase margin. Both of these translate into greater stability.

(Why use 100 kHz, and not, say, 30 kHz or even 20 kHz? It's mainly a "fudge factor" — we don't want to cut it too close to the audio bandwidth, in case the op-amp has some nonideal characteristics that cause it to have problems with the bandwidth limited so tightly to the audio bandwidth. Allowing 2 to 3x the bandwidth actually required is safe.)

You can use a gain of 80-100 with most op-amp chips if you don't want to worry about this. This is suitable for op-amps with GBPs as low as 8 MHz, which is the slowest op-amp you should use for a META42.

Once you have the local loop configured, you can pick values for the global feedback resistors (R3/R4). A global gain of 2 to 15 is typical for a headphone amplifier; the proper value will depend on your source, the pot's value, your headphones, and your music listening style. You can use the gain goal-seeker to find resistor values that will give a particular gain value, and then use the multiloop gain calculator to find the exact gain you can expect for your chosen resistor values.

The outer loop's resistor values should be lower than the inner loop's values. As a rough rule of thumb, make R3 five to ten times lower than R5. Also, remember that the lower these resistor values are, the more current your amp will use. I personally try to make R3 no lower than about 220 Ω, which means that R4 would be 2 kΩ for a gain of 10; then, R5 would be 1.2 kΩ or higher, making R6 120 kΩ for a ~100× inner loop gain. At the same time, you don't want to go too high with these values, either, because that increases the chances that noise will get amplified along with the music signal. Avoid resistances over 1 MΩ if you can. Not only do larger values risk noise pickup in the amp, large-value 1% resistors tend to be expensive.

<< Step-by-Step Assembly Guide
Tweaks >>
Updated Sun Jan 18 2015 04:23 MST Go back to META42 Headphone Amplifier Go to my home page