Love the smashing orangey bit, someone at Kef must like Jaffa cakes.Spay painted my loudspeaker stands yesterday to colour match them to my LS50 since after optimising their EQ and positioning I really love them and use them in my main system again,
before
View attachment 88253
and after
View attachment 88254
I've not seen that target before, it has a very shallow slope to 10k.By the way, this is current Harman target to which I EQ them MMM based (var. smoothing):
View attachment 88270
It's from a Arcam Dirac Live and was posted in a discussion about the Revel 206 or 226. I tend to prefer it in my room to the other Harman ones I used before.I've not seen that target before, it has a very shallow slope to 10k.
Spay painted my loudspeaker stands yesterday to colour match them to my LS50 since after optimising their EQ and positioning I really love them and use them in my main system again,
before
View attachment 88253
and after
View attachment 88254
Do you have a collection of these curves? If so do you mind sharing them.It's from a Arcam Dirac Live and was posted in a discussion about the Revel 206 or 226. I tend to prefer it in my room to the other Harman ones I used before.
Sure, I had posted some there, but the one I am using currently is attached below.Do you have a collection of these curves? If so do you mind sharing them.
By the way it seems to originate from this Toole graph:Sure, I had posted some there, but the one I am using currently is attached below.
Very inteeresting to see what he used to make that. Basically anyone who can afford a Umik, a cake turntable, and a microphone boom and REW can pretty much do the same--though there is a learning curve.Thanks for the link, very cool to see people producing quality spins without an anechoic chamber. This one actually appears to be highly accurate and matches very closely with my in room measurements when I had them, most notably the emphasis in the 2k region and the dip just before that.
View attachment 88563
Very inteeresting to see what he used to make that. Basically anyone who can afford a Umik, a cake turntable, and a microphone boom and REW can pretty much do the same--though there is a learning curve.
Very inteeresting to see what he used to make that. Basically anyone who can afford a Umik, a cake turntable, and a microphone boom and REW can pretty much do the same--though there is a learning curve.
It becomes much more difficult with towers that usually have the reference axis at the tweeter and their center of gravity somewhere way different as I'm sure @hardisj can attest to .
To say nothing of less expensive.While the results are helpful, there is a practical limit to how accurate they are. His farfield gating results in the lowest measurable frequency before reflection as being 500Hz. This also means an accuracy of 500Hz; a data point every 500Hz. So, if there is a mild-Q dip or bump at 800Hz, his measurement method is hardly going to show it. And it definitely won't show a high-Q resonance like the Buchardt S400 has.
The problem in measuring accurately is the midrange. In his case, he merges farfield and nearfield between 350 and 550Hz. IOW, IMHO, that data is only valid above maybe 1kHz (which still is only about 1/3-octave resolution with a step every 500Hz) and below 350Hz. Everything else is a "best guess". Not trying to be mean about it at all. That's just the nature of that kind of measurement. That's how I measured for years. So I know. If it were more accurate than this, trust me, I would be using that method. Because it is a hell of a lot easier than doing what I have to do...
While the results are helpful, there is a practical limit to how accurate they are. His farfield gating results in the lowest measurable frequency before reflection as being 500Hz. This also means an accuracy of 500Hz; a data point every 500Hz. So, if there is a mild-Q dip or bump at 800Hz, his measurement method is hardly going to show it. And it definitely won't show a high-Q resonance like the Buchardt S400 has.
The problem in measuring accurately is the midrange. In his case, he merges farfield and nearfield between 350 and 550Hz. IOW, IMHO, that data is only valid above maybe 1kHz (which still is only about 1/3-octave resolution with a step every 500Hz) and below 350Hz. Everything else is a "best guess". Not trying to be mean about it at all. That's just the nature of that kind of measurement. That's how I measured for years. So I know. If it were more accurate than this, trust me, I would be using that method. Because it is a hell of a lot easier than doing what I have to do...
Thanks for this! Lines up nicely with other LS50 measurements. I hope you get the chance to check out the active LS50W sometime - curious to see what the measured differences are. Mine showed both flatter on-axis and more controlled off-axis than measurements fo the passive versions I've seen, but I've not had the passive LS50 in-house to compare myself. Relatively Smooth DI curve should mean decent EQ-ability, as expected from a KEF coax.
solved by experimenting with positioning