I love it when you egg-heads start talking dirty.
I've no idea what you're talking about, but then I've no idea what my wife 
means when she explains why this red is better than that one, nor when my son 
explains how the design of a differential could be better designed for 
off-roading, nor when my daughter patiently explains why this particular 
car-thief is way, way cuter than that one.
Ah well, the older I get, the more and more I know about less and less. Soon, 
I'll know everything about nothing. Or vice versa.
I'm sure all will be revealed in the fullness of time...
Dr Peter Lennox

Principal Researcher,
Signal Processing and Applications Research Group (SPARG)
School of Technology,
Faculty of Arts, design and Technology
University of Derby, UK
e: [email protected]
t: 01332 593155
w: http://sparg.derby.ac.uk/SPARG/Staff_PLX.asp
________________________________________
From: [email protected] [[email protected]] On Behalf 
Of Sampo Syreeni [[email protected]]
Sent: 04 November 2010 21:36
To: Surround Sound discussion group
Subject: Re: [Sursound] Help !! -- For AMB-decoding theory freaks only

On 2010-11-04, [email protected] wrote:

> Seems you are completely out of touch with the context of this thread.

That more than possible. But still, if you don't mind my asking, why be
so harsh about it, all of a sudden?

> There's nothing 'naïve' about in-phase. It may look as something
> fundamental to you but it isn't.

To me in-phase is one of the fundamental decoding cases because in
Stanzial et al's energy propagation sense it minimizes the standing part
of the field within the array wrt the propagating one. Or rather it
comes close to that: without lots of extra symmetry I'm not willing to
say this is the minimum, or even a local minimum, but I'm still willing
to claim that it's within a bounded distance of the optimum in absolute
complex magnitude integrated over the inside of the rig, where the
distance should be able to be bounded above by one or another
asymmetricity metric wrt the rig geometry.

My comment started with my age-old disagreement with Filippo about how
free-field mic arrays interact with soundfields. Originally I was
thoroughly certain that a sphere of mics in the free field could always
capture the entire soundfield, if properly spaced and processed right.
In the end, Filippo showed that I was wrong, on physical grounds: this
is not possible using just a curtain of monophones, because the boundary
conditions needed for the wave equation were not there in this case.
After that I privately convinced myself that it couldn't really be done
in theory even with directional microphones, eventhough arrays of
directional microphones could still come increasingly close to what
Philippo and the literature said was the primary condition: a boundary
within the array.

Now, we all know from the ground up that mics and capture on the one
hand, and speakers and playback on the other are very much dual within
the ambisonic framework. If something goes amiss with one, it pretty
much always goes amiss with the other as well, and for the same reasons.
So, I've mulled for a long time over what might go wrong with a rig,
analogously to that mic example Filippo gave me.

I am not sure whether this acute problem has anything to do with what
I've been thinking about. As such, I presented a simple test to try it
out: does the problem go away if the array diameter is sunk, while the
directional aspects stay the same? That would suggest it has something
to do with diameter above directionality. So would the possibility that
the problem shifts to a different frequency band.

In particular, this kind of problem would manifest itself audibly with
very regular, rotationally symmetric arrays, which pretty much nobody
outside of this list has. If somebody else heard them, they would likely
mistake them for room modes or somesuch.

So I think a mere question and a simple suggestion for a test is
justified here.
--
Sampo Syreeni, aka decoy - [email protected], http://decoy.iki.fi/front
+358-50-5756111, 025E D175 ABE5 027C 9494 EEB0 E090 8BA9 0509 85C2
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