OK. Sorry for the delay. As a matter of review and to redirect this thread a bit, I've pulled the following from an earlier post:
So, there are a couple of basic ways around this reflection thing in cars. One is to try to minimize them and the other is to "spread the chaos around". Minimizing them is damn difficult if you want to have a car that can be driven. Spreading the chaos around simply means that we try to make all the reflections have similar frequency response so we can EQ them and the sound of the speakers using the same filters. Using the speakers where the dispersion is wide is the way to do this.
Using horns and big diaphragms for "pattern control" is the way to minimize the reflections from adjacent boundaries, but those adjacent boundaries are responsible mainly for altering the frequency response and not the image. Image narrowing and causing the car to sound like a car is mostly caused by reflections of right channel information from boundaries near our left ear and reflections of left channel information from surfaces on our right. This crosstalk partially destroys stereo, as each of our ears hears both speakers and the arrival times are within 20mS. This is worse in cars than in rooms, because the surfaces are closer. That means the intensity (loudness) of the reflections is greater and our perception that they and the initial sound are the same is greater. This is what makes a car sound like a car rather than a much larger space. This condition is what "Ambisonics" tries to fix.
I've tried both of these routes to great sound and I find that the "spread the chaos around" method is the most straightforward and because the conditions in the car make this much easier. The cheesy drawing below makes this a little more obvious, if the car is compared to a room.
The first rule of equalization is that you can't put energy back into a null caused by destructive interference in the acoustic system. You can remove energy from a peak caused by constructve interference.
The second rule is that high-Q (narrow) peaks and dips are less audible than low-Q peaks and dips. When we listen to music, our ability to perceive high-Q peaks and dips is further decreased because the chances that a particular sound will happen at precisely the right frequency, thereby energizing the high-Q peak or dip is reduced. In essence, this means that there may be no need to smooth the high frequency part of the comb, but the low frequency part of the comb, particularly the first (lowest-frequency null) is a problem. Plus, many listeners like the way the top of the comb sounds, because it adds a sense of width by screwing up the phase between the speakers and drawing our attention to the locations. This is very hard to hear in the frequencies that tweeters play, but a bit easier, lower in the midrange.
Patrick's method is different than my method and both work. Patrick's goal is to control both frequency response and directivity (through narrow passbands and pattern control--(horns) and using speakers in the range where they beam) and the method I suggest is the opposite. The reason that they both work is because, as I've suggested before, we don't hear the reflections as separate events. Patrick attempts to eliminate adjacent boundary reflections, and I suggest simply EQing them along with the direct sound.
It's important to note, that neither method will eliminate the reflections from boundaries close to our ears, and those reflections are the ones that make a car sound small--those reflections contribute crosstalk (left sounds at our right ear and right sounds at our left ear).
OK, so if you're following me, the basics are that we have to have a right and left speaker system that covers the band of frequencies from the crossover point between them and the sub and 20kHz without huge holes in either the on-axis response or the off-axis response. Of course, the off axis response will exhibit gradual attenuation as frequency increases, but it shouldn't have big peaks or dips near any crossover point. Below is a nearly ideal frequency response and directivity index:
Obviously, the red curve is slightly better than the blue one. For the speaker in the graph above, we use a waveguide on the tweeter to match the directivity of the tweeter to that of the woofer at the crossover. A similar curve (a directivity index that's reasonably flat with no peaks or dips) can be achieved by using multiple drivers in the regions where they DON'T beam. This is why I suggest a 3-way system in the front doors.
The frequency response plot below is one for a 2-way component system that doesn't include any measures to match directivity between the drivers. The crossover point between the mid and tweeter is too high (the mid starts to beam off axis). There's no directivity index plotted here, but it would include a peak in the region where the off-axis response shows a dip.
OK, so now that we've placed a great deal of importance on getting the speaker system right to begin with, here's an example of why that's all good system design practice, but in the end, doesn't matter nearly as much as it might seem. It is important to be sure that the entire bandwidth is covered competently, because we can't put energy into a system if there's no source for that energy--if your speaker system has a big hole at the crossover, you can't get it back.
Below is the near-field respone of the OE speaker in the door of a Mini Cooper. The measurement was taken about a half inch form the grille. Despite the dip at 1k, the response isn't too bad. BTW, I didn't investigate the cause of the dip
If I were building this system, I'd add a 3" mid and cross the 6" at 1kHz. The OE system doesn't include a low pass on the 6" and includes a small tweeter in the top of the door. Anyway, if I close the door and place the microphone at the driver's listening position, this is what the response looks like:
Nice, huh? What's the difference? Reflections and a tweeter. Good luck trying to eliminate all of that--no matter what you do, you'll never get back to the previous graph. The stuff below 1kHz can't be eliminated by anything other than dramatically changing the shape of the interior surfaces and the size of the vehicle. Between 1kHz and about 10kHz, adjacent boundaries contribute to the mess. Above about 10kHz, adding foam and carpet here and there might tame this somewhat, but the benefit isn't worth the effort.
Fortunately (or unfortunately) the response above is what we hear and it can be adequately equalized. Below is the target response I suggest:
the big problems at lower frequencies have to be fixed. It won't be possible to put energy back into the biggest hole, so the peaks will have to be reduced to match.
At this point, looking at a lower-resolution graph may be helpful--we don't want to be distracted by all of that high-Q stuff at high frequencies.
. Here are the steps, including selection of a high pass filter frequency:
Of course, this can't be done with a 31-band graphic EQ and that's why those aren't useful. It also can't be done by moving speakers, changing the aiming, swapping the speaker for something better, adjusting the crossover point between the mid and tweeter slightly, adding damping material to the doors, or anything else. EQ is the only thing that will help.
This is why I suggest the method I suggest.
TA should be set first, especially if you can align the tweeter and mid separately. After TA, set your EQ according to the process above. Once the left and right have been EQed so thay have the same response and the arrival times match, add the sub. EQ the right with the sub. Then turn the right off and EQ the left with the sub. Then, turn on both channels and listen. If you need to make further adjustments, be sure to EQ right and left equally--you're just shaping the response now and you can't equalize frequency reponse problems that appear in the measured response of both channels, measured at the same time (see the lengthy discussion of comb filtering in the previous post). In fact, what you see on the RTA won't even look like what you hear, so don't pay much attention to the RTA of both channels playing at the same time for any frequency above about 150Hz (the region where the sub contributes).
Also, moving the microophone around a head-sized area will help you determine whether to fix the high-Q peaks at higher frequencies. If they change or go away as you move the mic, don't worry too much about them unless they annoy you when you listen to music. Then, pick the annoying one and get rid of it.
BTW, we have a new 2-channel auto EQ algorithm that does precisely what I've suggested and it makes even this Mini Cooper with the factory speakers sound GREAT.