Mikhail Naganov

Headphone Equalization For The Spatializer

As I have mostly finished my lengthy experiments with different approaches to stereo spatialization and finally settled up on the processing chain described in this post, I could pour my attention into researching the right tuning for the headphones. Initially I was relying on the headphone manufacturers to do the right thing. What I was hoping for, is that I could take headphones properly tuned to either “free field” or “diffuse field” target, and apply just some minor corrections in my chain. You can read about my attempts to implement “free to diffuse” and “diffuse to free field” transforms applied to the Mid/Side representation of a stereo track.

Why Factory Headphone Tuning Can’t Be Used

However, since in the last version of my spatializer I actually came closer to simulating a dummy head recording, I realized that using any factory equalization of any headphones simply does not work—it always produces an incorrect timbre. The reason is that my spatializer simulates speakers and the room, as well as torso reflections, and even some aspects of the pinna filtering—by applying different EQ to “front” (correlated) and “back” (anti-correlated) components of a stereo recording. “3D audio” spatializers (they are also called “binaural synthesis systems”) that use real HRTFs come even closer to simulating a dummy head recording. That means, if you play the spatialized audio over headphones with their original, say, “free field target” tuning, you will apply similar human body-related filtering twice: once by the headphones themselves, and then also by the spatializer.

At some point I used to think that using headphones calibrated to the diffuse field target is fine, because they are “neutral” (do not favor any particular direction), but this assumption is also false. That’s because diffuse field equalization is an average over HRTFs for all directions—thus it’s still based on the human body-related filter. This is why more advanced “3D sound” renderers have a setting where you specify the headphones being used—by knowing that, they can reverse the factory tuning. I also experimented with AirPods Pro and confirmed that they change their tuning when switching between “stereo” and “spatialized” modes.

By the way, in the reasoning above I use dummy head recordings and synthetic “3D audio” spatializatoin interchangeably, but is it conceptually the same thing if we view it from the listening aspect? I think so. Dummy head recordings are taken using a real person, or a head and torso simulator (HATS) with microphones mounted at the ear canal entrances. Sometimes it’s not a complete HATS, but just a pair of ears placed at the distance similar to the diameter of a human head. In any case, the microphones placed into these ears block the ear canal (in the case of HATS the canal might not even exist). Now, if we turn our attention to HRTF-based 3D audio rendering, HRTFs are also typically measured with mics placed at the blocked ear canals of a person (see the book “Head-Related Transfer Function and Acoustic Virtual Reality” by K. Iida as an example). So basically, a dummy head recording captures some real venue (or maybe a recording playing over speakers in a room), while a “3D audio” system renders a similar experience from “dry” audio sources by applying HRTF filters and room reverb IRs to them.

It’s actually a useful insight because it means that we can use the same equalization of headphones for all of these: dummy head recordings, “realistic” spatializers, and my stereo spatializer. Essentially, I can decouple the tuning of my spatializer from the tuning of the headphones, and validate the latter using other spatial audio sources. And I am also able to compare these different sources directly, switching between them instantly, which provides ideal conditions for doing A/B or blind comparisons.

Hear-Through Transfer Function

The problem is, finding correct equalization for playing any of the spatial audio sources over headphones is actually a bit tricky. As I’ve mentioned above, first we need to “erase” the factory tuning of the headphones, and then re-calibrate them. But to what target? If we think about it, it must be a transfer function from an entrance of a blocked ear canal to the eardrum. This actually sounds like a familiar problem. For example, if we consider AirPods Pro, by their design they isolate the user from outside noises, however one can enable the “transparency” mode which adds the outer world back in. In the audio engineering industry this is also known as the “hear-through” function.

There is a good paper “Insert earphone calibration for hear-through options” by P. Hoffmann, F. Christensen, and D. Hammershøi on the transfer function of a “hear-through” device. The TF they use schematically looks like this:

The curve starts flat, then it begins to elevate at 300 Hz, reaching a peak between 2–3 kHz, then a sharper peak between 8–9 kHz. It also has a downward slope after 4 kHz. Note that in the paper there is a discrepancy between the curve shown on the Fig. 2 and the target curve for headphone tunings which appears on the Fig. 4.

In practice, we should consider this curve as an approximation only, since for each particular earphone and ear canal the center frequencies of the peaks and their amplitudes will be different. The previously published paper “Sound transmission to and within the human ear canal” by D. Hammershøi, and H. Møller shows that rather high individual variation exists between subjects when the TF from the outside of the ear canal to the ear drum is measured.

Also note that this TF applies to in-ear monitors (IEMs) only. The paper describes re-calibration of different IEMs to this target. Some of them comply well with re-tuning, some are not. For my experiment, I decided to use EarPods because they are comfortable—I have no physical ear fatigue whatsoever, they use a low distortion dynamic driver (see measurements on RTINGS.com), and they are cheap! Plus, you can put them into and out of your ear very easily, unlike true IEM designs that require some fiddling in order to achieve good sealing which blocks outside noises. Obviously, the lack of this sealing with EarPods is one of their drawbacks. After putting them in, you still hear everything outside, and what’s worse, the timbre of outside sounds is changed, although since we are not using them for augmented reality purposes, this is not an issue. Yet another annoyance is that the 3.5 mm connector is rather flimsy, however, I have worked around that by wrapping it into heat-shrink tubing:

These drawbacks are not really serious—since we are not implementing actual hear-through for augmented reality, there is no concern about hearing modified sounds from the outside, and we will partially override them with music. However, here is the main drawback of EarPods: due to their shape, it is not easy to make a DIY matching coupler for them. Basically, you need a coupler imitating a human ear. Luckily, I now have access to a B&K head 5128-B. Thanks to its human-like design, EarPods can be easily mounted on it and I could obtain reliable measurements.

Yet another challenge comes from the fact that I wanted to create an individual hear-through calibration. That means, I wanted to be able to adjust the peaks of the hear-through target on the fly. These peaks actually depend on the resonances of the ear canal and the middle ear, which are all individual. The B&K head has its own resonances, too. Thus, even if I knew my individual HT target, calibrating to it on a B&K head might not give me what I want due to interaction between an EarPod and the ear canal of the B&K head.

So I came up with the following approach:

  1. Tune EarPods to “flat”, as measured by the B&K head.
  2. Figure out (at least approximately) the TF of the B&K ear canal and microphone.
  3. Add the TF from item 2 back to the “flat” calibration TF.
  4. On top of the TF from item 3, add the generic “hear-through” (HT) TF, and adjust its peaks by ear.

Why does this approach work? Let’s represent it symbolically. These are the TFs that we have:

We can note that P_epbk can be approximated by P_eb * P_bk, where P_eb is the TF that we could measure by coupling an EarPod directly to a microphone calibrated to a flat response. What we intend to do is to remove P_eb, and replace it with a TF that yields P_ht when EarPods are coupled with my ear canal. That is, our target TF is:

P_tg = P_ht / P_eb

When I calibrate EarPods to yield a flat response on the B&K head, I get an inverse of P_epbk, that is, 1 / P_epbk, and we can substitute 1 / (P_eb * P_bk) instead. Thus, to get P_tg we can combine the TFs as follows:

P_tg = P_ht * 1 / (P_eb * P_bk) * P_bk = P_ht * P_bk * 1 / P_ebbk

And that’s exactly what I have described in my approach above. I must note that all these representations are of course approximate. Exact positions of transfer function peaks shift as we move the sound source back and forth in the ear canal, and move outside of it—one can see real measurements in the “Sound transmission to and within the human ear canal” paper I’ve mentioned previously. That’s why it would be naive to expect that we can obtain an exact target TF just from measurements, however they are still indispensable as the starting point.

Approximating B&K 5128 Transfer Function

So, the only thing which has to be figured out is the P_bk transfer function. As I understand it, without a purposefully built earphone which is combined with a microphone inside the ear, this is not an easy task. The problem is that the SPL from the driver greatly depends on the acoustic load. For example, if we use a simplest coupler—a silicon tube between the earphone and a measurement mic, the measured SPL will depend on the amount of air between them, and the dependency is not trivial. What I mean, it’s not just changing resonances and power decay due to distance increase.

I checked B&K’s own technical report “The Impedance of Real and Artificial Ears” with lots of diagrams for impedance and transfer functions. I also tried some measurements on my own using low distortion dynamic driver IEM (the Truthear Zero:Red I mentioned in my previous posts). The main understanding that I have achieved is that the ear canal and microphone of the B&K head exhibit a tilt towards high frequencies. I was suspecting that because the EarPods tuned to “flat” on the B&K (the 1 / (P_eb * P_bk) TF) did sound very “dark.” So I ended up with creating a similar tilt, and the actual amount was initially tuned based on listening, and then corrected when measuring the entire rig of EarPods via P_tg on the same B&K head.

Individual Hear-Through Tuning

As I’ve already mentioned before, the hear-through TF from the paper could only be considered as a guideline because of individuality of ear canals and the actual depth of insertion of earphones into them.

In order to figure out the individual resonances of the left and right ears I used pink noise rendered into one stereo channel and spatialized via my processing chain. I had two goals: get rid of the “hollow” sound (pipe resonance), and make sure that the pink noise sounds like a coherent point source. When the tuning is not right, it can sound as if consists of two components, with the high frequency band placed separately in the auditory space.

For this tuning process, I have created a prototype HT TF in a linear phase equalizer (DDMF LP10), and then was tweaking center frequencies of the peaks and their amplitudes. My final settings for the left and right ears look like this:

As you can see, compared to the “generic” TF pictured before, some changes had to be made. However, they are only needed to compensate for the features that got “erased” by the “flat” tuning. I had to restore back some bass, and also diminish the region around 6 kHz to avoid hearing sharp sibilants. This is how the final tuning looks like when EarPods are measured by the B&K head:

It looks rather similar to the target described in the “Insert earphone calibration…” paper. Note that the difference in the level of bass between the left and the right ear are due to my inability to achieve the same level sealing on both artificial ears— I must say, coupling EarPods is really non-trivial. Yet another difference is addition of dips around 60 and 70 Hz, as otherwise I could feel the vibration of the drivers in my ears.

Listening Impressions

As I have mentioned above, since we can consider dummy head recordings, “3D audio” renderings, and my spatializer as equally footed sources which require the same “hear-through” earphone calibration, I started with the first two.

I have made some dummy head recording using MS-TFB-2-MKII binaural mics by Sound Professionals mounted on my own head. I tried both just recording sounds of my home, and also recording pink noise played over stereo speakers (left only, right only, correlated PN, anti-correlated PN, and correlated PN from the back). For the “3D audio” rendering I used Anaglyph plugin. This is a free and simple to use plugin which allows rendering a mono audio source via different HRTFs, and apply different kinds of room reverbs.

I must say, I was impressed by the realism achieved! When playing sources recorded or rendered in front of me, I was sure the sound comes from the laptop sitting on my knees. Note that in Anaglyph I have set the source height at -15° for achieving this effect.

Playing sources recorded from the back was a bit of a surprise—I have experienced a strong back-front reversal with my own dummy head recording. However, the rendering by Anaglyph and my own spatialization chain produced much more realistic positioning. Thus, either Sound Professional’s mics have some flaw which makes behind sources less “real,” or “reality” is not what we want to achieve with these renderings— perhaps the brain requires stronger “clues” to avoid FB reversals, and these clues for some reason are not so strong in a dummy head recording.

But other than that, the dummy head recordings done with these mics are very convincing. If you play a record back exactly at the same location where it was recorded, the mind automatically connects sounds with the objects around. Or you will experience a bit confusing feeling if the visual scene has changed, say, a person which was talking on the recording has left, and now the reproduced sound comes from an empty place.

I also noted how much the feeling of distance and location “collapses” when a dummy head recording is played in another setting—another room for example. Our visual channel indeed has a strong dominance over the audio channel, and seeing a wall at the location where the sound is “coming from” in the recording completely changes the perception of the source’s distance to the listener.

Also, the feeling of the distance is greatly affected by the loudness of playback, and perceived dynamic range. Thus, don’t expect a lot of realism from simple studio-produced stereo recordings, even when rendering them via a “spatialization” engine.

Fine-Tuning the Spatializer

Using these realisting reference recordings and renderings I was able to fine tune my spatializer. Basically, I used pink noise positioned at different locations, and was quickly switching between my spatializer and a dummy head recording, or a rendering by Anaglyph. This was much more precise and easier than trying to compare the sound in headphones with sound in speakers! Even if you train yourself to put the headphones very quickly on and off, and switching the speakers off and on at the same time, this still does not happen quick enough. I’ve heard from James “JJ” Johnston that switching time must be no longer than 200 ms. With instant switching, I could compare both positioning of sources and their tonality. Note that these attributes are not independent because the auditory system basically “derives” this information from incomplete data which it receives from ears.

I noticed that the perceived distance to the sources rendered by my spatializer is less than the distance of “real” or “3D audio” sources. When switching between my spatializer and a DH recording, or Anaglyph, the source was literally jumping between “far” and “near” while staying at the same lateral angle and height. Increasing the level of the reverb in my spatializer puts the source a bit further away, at the cost of cleanness. Similar thing with Anaglyph: with reverb turned off the sound is perceived as being very close to the head. Yet, reverb adds significant tonal artifacts. Since I’m not doing a VR, I decided that it’s better to have a cleaner sound closer to the face. In fact, a well produced recording has a lot of reverb on its own, which helps to “feel” the sources as if they are far away.

As a result of these comparisons, I have adjusted the level of the cross-feed, and adjusted directional bands the Mid/Side equalization for better rendering of “frontal” and “behind the back” sources. As I have mentioned above, the sources from behind ended up sounding more “realistic” with my rendering, compared to my own dummy head recordings.

Another interesting observation was that my spatialization produces more “heavier” sounding pink noise than a dummy head recording. I actually noticed the same thing with Apple’s spatializer. I think this heavier tonality is better for spatializing music, and maybe movies as well, so I decided not to attempt to “fix” that.

Bonus

While researching this topic, I found a paper by Bob Schulein and Dan Mapes-Riordan with a very long title “The Design, Calibration and Validation of a Binaural Recording and Playback System for Headphone and Two-Speaker 3D-Audio Reproduction” on their approach to doing dummy head recordings. The paper also suggests a headphone equalization approach which is similar to what I ended up using. In fact, the “Transfer function T2” from the paper has a lot in common with the “hear-through” target function I used. From the paper, I came to Bob’s YouTube channel which features some useful dummy head calibration recordings, as well as recordings of music performances, both captured by the mannequin called Dexter which Bob built.

Some notes on these recordings. I could hear that the tuning applied to the recording is different on older vs. newer videos—it is indeed hard to come up with the right tuning! Then, on the “calibration” recordings where Bob walks around Dexter, I was experiencing front-back reversals as well—that’s when listening to recordings with my eyes closed. Thus, one either needs to always look at the visual—this is what Bob proposes, or incorporate head tracking into the reproduction process. However, using head tracking requires replacing in the recording process the dummy head with ambisonics mic, which captures the sound field in a more “generic” form, and then rendering this ambisonics capture via a “3D audio” renderer.

Another weak point of “old style” dummy head recordings that I have noticed is that minor creaking and coughing sounds coming from the audience immediately distract attention from the performance. This happens unconsciously, probably because you don’t see the sources of these creaks, and this forces you to look into the direction of the sound as it can be potentially dangerous. When sitting in a concert hall, this unconscious switching of the attention happens much less because you have a wider field of view, compared to the video recording. Whereas, in stereo recordings the performance is captured using mics that are set close to the performers, so all sounds from the auditory can be suppressed if needed during the mixing stage.

Conclusions

I’m really glad I have solved the “last mile” problem of the stereo spatialization chain. Also, the headphone tuning I came up with allows listening to dummy head and “3D audio” recordings delivered with a great degree of realism. It’s also interesting that it turns out, for music enjoyment we don’t always need the reproduction to be “real.” Much like a painting or a photograph, not mentioning movies, actually represents some “enhanced” rendering of reality and reveal the author’s attitude to it. Sound engineers also work hard on every recording to make it sound “real” but at the same time interesting. Thus, the reproduction chain must not ignore this aspect.