Here is an example to the above (
"Should a dip in the FR go or stay"), which is a key point in the video.
A few years ago I designed a speaker (hobby DIY) that sounded really good with flat tuning and low sound pressure level (SPL) when listening (with some pieces of music you could hear small conspicuities, but since SPL was low it wasn't annoying yet).
But at high sound pressure level the speaker very quickly became unbearable.
The best crossover tuning that made it possible to listen to music relaxed even at high sound pressure levels looked like this - on-axis frequency response (FR), FR of woofer, midwoofer, tweeter:
At low SPL the speaker sounded "warm" on-axis, at high SPL the speaker sounded "right" - how can that be?
As an explanation for the "warm" sound at low SPL, the on-axis FR is sufficient in this case. At low SPL the direct sound dominates and the 3dB dip around the ear canal resonance (around 2.7kHz) leads to the sound perceived as "warm".
But why does the speaker sound just right with 3dB dip at high SPL and is unbearable with flat FR at high SPL?
To answer that you have to look at the horizontal and vertical FR. To keep the example as simple as possible, we restrict ourselves here to the horizontal FR.
To see what happens we examine the horizontal FR normalized to the on-axis (this would correspond to an ideally flat equalized speaker):
We can see that in this case the
angular off-axis frequency responses in the range 1-4kHz show a hump and partly have a higher SPL than the on-axis FR.
With increasing volume, the perception of diffuse sound increases. The sound power (the radially emitted sound of the loudspeaker) has a hump exactly in the area of the ear canal resonance (where many people are particularly sensitive to sound power peaks).
It's quite different when we look at the final crossover tuning:
The on-axis dip compensates for the "errors" (caused by the loudspeaker cabinet, driver arrangement and edge diffraction) of the off-axis FR.
This is also confirmed by the sound power FR - blue curve. The black curve shows the on-axis FR and the red curve the (horizontal) directivity index, which is also a good indicator of the speaker's design flaws.
The sound power curve is so to speak an indicator or shows a tendency for the sound at high SPL in a
normal listening room - of course not in the sense of a measuring device, where every tenth deviation shows a linear dependence.
Thus, measurements and listening impressions complement each other perfectly and quickly lead to a good result without the risk of overlooking important characteristics of the loudspeaker.
Update:
The analysis is greatly simplified by omitting the vertical FR, so please do not apply the statements to loudspeakers in general.
For example, unevenness in the DI caused by the vertical radiation is to be judged differently than by the horizontal radiation, etc....