A monopole radiator is - by definition - a spherically symmetric source
that radiates equally in all directions.  You could make an acoustic
monopole radiator by, for example, making a little sphere with a radius
that moves in and out with time.  It moves out and pushes air away from
itself, then moves in and sucks it towards itself, etc.  Woofers in
sealed boxes are pretty close to that, since the entire box vibrates in
and out, but directional sources like tweeter are nowhere close to it. 
The acoustic radiation of a tweeter in a box is *not* monopolar. 

An acoustic dipole radiator is two monopoles sitting close together and
oscillating out of phase.  A speaker driver in free space or an open
baffle is a pretty good approximation to that.  For tweeters the magnet
assembly on the back is big enough that it absorbs quite a bit of the
back-directed radiation, making it less like a dipole.  That's why the
Orions have a back-directed tweeeter.

There is no ambiguity about these term (and by the way that wikipedia
article doesn't disagree - it's just not very detailed).  They are a
useful way of characterizing sound because any sound field can be
decomposed into a sum over multipoles, each having certain unique
characteristics, and because acoustics is close to linear.

As for the room, you have to normalize to something.  We're only
talking about bass here (room modes get averaged out for treble), where
the radiation of a box speaker is pretty much monopolar (so it radiates
in ALL directions).  The point is you have to normalize either the SPL
at some point or the power going into the speaker.  Then you want to
ask what the amplitude of the room modes is.  If you normalize to the
SPL on axis, a dipole radiator radiates 1/2 as much power as the
monopole (basically because it's not radiating to the sides).


-- 
opaqueice
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