Hi
Have to redo the graphs, but I don't think the conclusion will change.
I had estimated the first reflection points using the mirror method and calculated them using that formula on ethan winer's real traps website. I could not find a second reflection point - it was outside the room.
Today I started by connecting one of the speakers out of phase and using the mic to find the sweet spot, using pink noise from the REW signal generator and the RTA display . At the sweet spot the two waves should cancel each other, I settled for the lowest volume I could get. Confirmed the position was equidistant using a string. For the rest of the stuff, the mic stayed there for the rest of the test.
Having done that set down to measuring the impulse response, one speaker at a time. Four long 40 - 20k sweeps per measurement. That because the *&%# upstairs is forever rolling gas cylinders or thumping the floor. A busy railway track about 300 m away too.
I started with a bare floor, then added a mattress on the floor, then some padding on fronts of two single seater thingies on the rhs, and finally plugging the six inch gap between the rockwool pads on the front wall and covering the TV. I goofed in labelling / saving the files, so no graphs to paste, but that as I said does not matter.
Regardless of the treatment, one thing jumped out. a prominent perfect reflection for the rhs speaker on all its impulse graphs. At 3.98 ms on all of them.
A little crude measuring gets me to the rhs corner on the front wall. That outside the room second reflection point exists at that corner.
Will confirm with another set of measurements tomorrow. That will lead me to the RFZ that is likely to be beneficial to Dirac. What I pity I did not figure this out before the trial ended. sigh!
So, that was the outcome of the train of thought your post flagged off. Thanks
, so I need a an area rug, and I need to do something about that rhs front wall corner
ciao
gr