I wanted to kick this thread off with a bit of talk on a topic that has come up a few times in the discussion of powerful amplifiers for headphones, that being the use of Class-D amplifiers.
Class-D is something that has become all the more prevalent in the speaker world, with many hugely powerful and excellently performing class-D options becoming available, and in situations like subwoofers, seeing anything other than class-D is almost unheard of! So why don’t we see class-D amplifiers in the headphone space more often? Or in fact how come there are hardly any at all?
Well, if you’ve not watched it already, I’d first recommend checking out my ‘Amp classes explained’ video, as this should help explain in fairly easy terms what differentiates Class A, AB, and D amplifiers.
Class D is unique in that rather than just amplifying what goes in, directly outputting an as-close-to-identical copy of the signal as possible, it actually “creates” a new signal. A stream of very high frequency, high amplitude pulses, which when filtered to leave only the low frequency (<20khz when possible) content, leaves only an amplified version of the signal that was originally fed to the input.
But there is a problem: This means class-D amplifiers need to have an output filter to remove this unwanted high frequency content from the output, and typically, the load/speaker itself actually forms a part of this filter circuit:
This in turn means that class-D amps and their filters need to be designed for a specific load impedance. And a change in impedance of the load will cause the filter to behave differently. We can show this by just doing a frequency sweep through a class-D amp with different load impedances. Here is one done by Amir at ASR of the Fosi Audio V3 with a 4 ohm load and an 8 ohm load:
As you can see, with the 8 ohm load, the frequency response amplifies high frequency content a fair bit, whereas with a 4 ohm load it attenuates it. This implies the amplifier was designed/optimised for likely around a 6 ohm load.
This is generally sensible given as an ‘8 ohm’ speaker will probably have dips in its impedance vs frequency curve to values lower than 8 ohm and so aiming for 8 ohm on the dot would likely not provide the best actual result.
With speakers, you can be pretty certain that almost any speaker is going to fall in the 4-8 ohm range with some exceptions. You have a narrow impedance range to target and so you can design your filter in a way that will work similarly well for the vast majority of speakers. Even if you put a 4 ohm speaker on a class-D amp designed for an 8-ohm load, you might attenuate the uppermost frequencies by a fraction of a dB as shown above, not really a big deal.
Headphones are quite a different story…..
Headphones can range anywhere from 2 - 1000+ ohms, and so designing a class-D output filter with a target impedance in mind is going to leave you with something that only works properly with a small number of headphones no matter what value you target.
Aim for a ~60 ohm impedance for planars? Well now almost any 300-600Ohm dynamic driver headphone is going to be way off. As will any planar that happens to be lower at say 20 Ohm.
Vice versa if you target ~300 ohm dynamic driver headphones, then low impedance planars will not perform correctly.
And with greater impedance differences come greater risks……
Below is a simulation of the frequency response of the class-D output filter circuit at the beginning of this post, with a few load impedance values ranging from 4 ohm to 155 ohm (Modhouse Tungsten)
The following values were used to try to get this filter design to match the behaviour seen by the Fosi amp in the ASR measurement:
L = 11.26uH
Cbtl = 0.703uF
When this hypothetical Class-D amplifier is connected to either a 4 or 8 ohm speaker, it will behave pretty much exactly as seen in ASR’s measurement of the Fosi amplifier. Under 20khz any differences are pretty small and unlikely to be of any concern. And with most ‘8 ohm’ or slightly below speakers it’ll behave pretty much exactly as intended.
But when we swap to higher impedance headphones, suddenly our high frequency content gets MASSIVELY boosted, not just by the couple dB we saw earlier…..
Even a 32 Ohm headphone sees a +2dB boost in audible band content by 20khz, and a roughly 15dB boost in content around 40khz.
If you were to put the 155 ohm modhouse tungsten on this amp, you could see a 30-40dB boost in content around 40khz. Go for a 300 Ohm headphone and it’d get even worse.
The elevation in upper treble is not ideal, but not necessarily the end of the world. However this enormous boost in content just above 20khz IS a problem, and you risk damaging your headphones or possibly ears, maybe even without realising it’s happening.
You might not be able to hear 30-40khz, but if you were playing ~90dB music, and accidentally pumping content up to 130dB or higher through your headphones, you could absolutely damage your hearing or your headphones.
Drivers don’t care what your upper hearing range limit is, they’ll break all the same if you overdrive them. And studies have shown that exposure to ultrasonic content can indeed damage hearing.
The TLDR:
If you use headphones on a class-D amplifier, you could be damaging your headphones and/or your hearing, and because you can’t directly hear the dangerous content, you might not even realise it’s happening until it’s too late.
So, that’s one of the main reasons we don’t often see class-D amplifiers in the headphone space. They can be difficult to make work for the massive range of impedances we see in the headphone market, risky, and personally I’d strongly recommend avoiding them.
That being said, some more modern designs from HypeX/Purifi use a feedback approach that does indeed make them load invariant and avoids the issue shown above. Keeping a flat frequency response up to the cutoff frequency regardless of the load impedance.
I’ve yet to test whether running high impedance headphones on these amps then causes a degradation in other areas of performance or higher distortion, but will do so whenever I next get ahold of one to test.
The other reason however is simply: Class D just isn’t needed for headphones.
Class-D amplifiers have an immense advantage in efficiency compared to Class-A and Class-AB amplifiers. Often comfortably above 90% compared to the ~40% on a REALLY good day of a class-A amplifier. Or 50-75% of typical AB amplifiers.
If you’re building a 3000W subwoofer, you can’t have a class-A amplifier that is dumping 7000-10,000W of heat into the room at all times unless you’re building a sound system that doubles as a sauna heater. And even a class-AB amplifier that gets 75% efficiency would mean that 3000W sub could be pulling roughly 4000W from the wall with around 1000W of that being dissipated as heat. Your subwoofer is going to need some SERIOUS heatsinks and cooling.
A class D amplifier with 90% efficiency would pull 3300W from the wall to output 3000W to the sub, and only 300W of heat would be generated at most. Probably far less during general operation, leaving you able to fit a nice compact amp into your sub, with maybe a small, hardly even noticeable heatsink on the back. Some like the SVS SB-16 ultra even get away with just dissipating what little heat they need to through the backplate itself despite the amp being capable of up to 1500W continuous or 5000W peak!
This is what allows Class D amplifiers to be so compact yet so powerful. Their huge efficiency advantage allows you to put much more powerful amps into smaller spaces with less heat dissipation as you just aren’t burning anywhere near as much energy as wasted heat. Almost all of what power comes into the amp from the wall is going directly to driving the load.
This is a big factor when you’re dumping hundreds of watts into speakers, and ESPECIALLY when pumping thousands of watts into subwoofers.
But with headphones, where you are using at the very most a few watts with even the most demanding headphones on the market, who cares if your 6W amplifier pulls 13W from the wall vs 20-25W? Five to ten watts of extra heat is almost nothing, and even class-A headphone amplifiers can still be pretty small because….well….dissipating twenty or so watts of heat is very easy. Your own body outputs about 100W of heat into the room at rest or 300-400W if exercising.
Class-D solves an important challenge in speakers. But with headphones, we simply don’t need the efficiency benefits of class-D when we are dealing with such relatively tiny amounts of power and heat anyway, meaning there is little reason not to just build class A and AB amps for headphones even before we consider the risks described in the first part of this post.