Originally Posted by WmAx
In order to have a broadband, direct beam of sound, the surface area of the effective radiation area of the driver must be approaching 1 wavelength and longer of the frequency in question. Thus, it's not possible to have 'directive' sound from the surface area available on a kickpanel with a direct radiator under the treble band. The best execution would involve the ultrasonic devices I mentioned earlier, that are able to produce a true broadband directive signal dispersion.
In order to have a directive beam of sound emanating from a direct radiator, the effective surface area which emits, must be large, relative the specific frequency desired to be directed/focused. The energy is dispersed across the diaphragm from an essentially infinite number of points, essentially in-phase. If you move off the direct axis to a point at which a vector path can be drawn, and the difference is significant in relation the wavelength of a given frequency, eventually at a point the emitted energy will meet a points where it is out of phase with each other, thus cancelling itself effectively. Therefor in that case, it can said to be directive. But the wavelengths in even the upper midrange, are considerable in size, relative to the drivers used in car audio for that purpose. The ultrasonic transducers I mentioned, because the actual emmited frequencies are very high in frequency(ultra-sonic), they are easily controllable in direction with relatively small panel sizes. The ultra-sonic frequencies are combined at the termination point(ear, microphone, whatever is within the path) to create the audible content.
Originally Posted by WmAx
Remember, the soundfield must have identical reflection time direct vs. reflect, and equal amplitude vs. frequency, at the ear positions.
You have:
-direct sound emitted by transducer(s)
-reflected sound(s) from surface(s)
-reflection time(s) associated with the reflected sound(s)
The reflected properties of L vs. R channels will be considerably different, even IF you managed to achieve identical on axis sound. The reflections, especially, on the L channel(if you are in driver seat) will be considerably negative in attribute. The L channel in particular will suffer from having a strong direct sound arriving at ear, and that sound bouncing off the window from 1” give or take a little, then bouncing back to your ear again. Because of the relative short pathlength, this will be relatively high in amplitude. The R channel will not have this very close reflected panel(window) to cause this effect.
Originally Posted by WmAx
If you equalized the frequency response here using head mounted stereo binaural microphones(you'd have to E.Q. each channel assymetrically on L vs. R, due to the very different angles to ear pinna of each channel in this seating position), it would not do anything for the destructive reflection times of left soundfield.
A binaural microphone is one that mounts just inside the ear canal. This is required for your application of assisting in ideal response, because the ear structure is a dynamic filtering device(this is part of how it senses direction, etc.). The ear will modify high frequency response transfer function relative to the angle of direct sound arrival. Since the L channel will be almost directly in front of you, and R channel will to the distant right at a significant angle, then the only way to accurately compensate for this difference would be making measurements using binaural microphones and adjusting E.Q. to compensate to achieve a symmetrical response curve to each side of the head. This will not compensate for the reflected time difference.
Originally Posted by WmAx
In a home environment, you can effect directive(down through most of the midrange) speakers using direct radiators due to it being practical to have large size speakers in this environment.
An electrostatic loudspeaker has a very large size diaphragm. As I detailed earlier about how this basicly works to direct soundwaves, I don’t need to explain that part again. Obviously, it is not a problem to have a 16” wide(or larger) ESL panel in a home audio environment.
Originally Posted by WmAx
But, since the direct vs. reflected pathlengths are long enough from speaker to walls, etc.; the reflections(as long as they are roughly equivalent in frequency spectrum distribution vs. direct sound) can be beneficial in this environment, since they would be interpreted as ambience, not interference, at time differences of approx. >5ms, <20ms. A symmetrical soundfield for L and R channels, including reflection times and frequency vs. amplitude response are not a problem either.
The human ear roughly begins to sense a direct vs. reflected sound signal(of the same original signal) as ambience effect when it is equal to around 5ms(roughly 4’ in distance). Significantly shorter time difference is interpreted as negative -- a muddy type effect that hurts sound quality. The proper proportion of sufficiently delayed signals reflected from the wall(s) act like phantom sound sources. This contributes to a perceived diffused soundfield, so far as the human hearing mechanism is concerned.
-Chris