SSLtech
Well-known member
While I agree largely with the spirit of the post, this little section is not technically accurate, insofar as the SoundField microphones can be polar-pattern and axial-angle adjusted after the fact.JohnRoberts said:So long story short you can gat a similar sound for limited conditions, but there is no way ever to change a mic's pick up pattern after the fact "in the mix".
In fact I'd go even further than you do John; even ON-AXIS a mic can pick up differently, because of pressure wave versus velocity wave.
A theoretical demonstration: Take two extremely different microphones: for the sake of this example let's consider a dipole mic such as a simple ribbon, and take a pressure mic such as a sealed capsule mic. (envisage a tin can with the top removed, and cling-film stretched over the opening. Now imagine how varying external pressure makes the film dip in and bulge out.)
Put the two mics in the exact middle of a length of plastic pipe maybe eight inches diameter. Now seal each end with an 8" loudspeaker drive unit. Wire the two speakers in series, "in-phase". -Now when a tone is played through the speakers, BOTH speakers will move inwards together, and outwards together. The pipe will pressurize and depressurize. The Omni capsule (the bean-can) will hear lots of signal. the velocity at the middle of the tube however, is zero. That means that the velocity mic (the 'ribbon') will 'hear' nothing.
Now flip the polarity of one speaker, so that when one pushes air into the pipe, the one at the other end pulls air out of the pipe. -Now we have a slug of air moving along the pipe and back again, but never increasing or decreasing in pressure. The Ribbon mic produces a fine signal, but the omni (pressure) mic produces no signal...
Now, how does that play out in real life? -Well, different instruments produce sounds differently, but let's start by considering a simple, infinite baffle (completely sealed) speaker cabinet. The speaker cone swings in and out, alternately pressurizing and depressurizing the air inside the cabinet, and conversely depressurizing and pressurizing the air outside the cabinet. It's a simple pressure variance, though effected through what is effectively a piston surface.
Some speaker designs however use porting, or veltilation like the simple bass-reflex design. -The bass reflex addresses the issue of the low frequency rolloff by venting a 'timed' wave from the REAR of the cone to 'assist' the faltering response driven by the front. -The result -if done right- is held to be an extension of an octave of flat response before the low frequency rolloff, but then the response falls off TWICE as steeply. -You do get TWO octaves of positive boost 'for free' before the tradeoff goes negative.
The combination of a pressure wave from the front of the cone face and a velocity wave from the port means that an omni mic and a dipole mic will record VERY different frequency/amplitude responses, even ON-AXIS, in an anechoic chamber, even using perfect;y "flat" microphones (if you can find a satisfactorily flat ribbon!)
Okay, so what else APART from a speaker cabinet? -Pretty much everything in fact. -The human voice is an excellent example where most of the 'guided/channeled' air coming from the mouth is velocity wave, but sibilants/fricatives are pressure. (Anyone thinking that Chinese mics sounding "spitty" in a manner where simple EQ doesn't solve the problem sounds familiar right about now?)
"Mmmmm" sounds and chest resonance is largely pressure wave, "aaaaaaaaa" is largely velocity wave... and the balance between component waves varies across the spectrum.
...So good luck to anyone trying to pick THAT little puzzle apart. -Yes it's possible. -But you'd have to start with a mic like a Soudfield, or -at the very least- a Josephson C700a.
Then perhaps all on and off-axis patterns could be modeled, along with pressure/velocity correction. -But not before.
That -in a long-winded way of explaining- is why the 'Royer simulation' in the video is laughably impossible.