Before I show you the directivity plots, let me post a new measurement I have not shown before which indicates at what distance the speaker acts as if it is in far field:
This says that above 400 Hz, that distance is 1.5 meters (where the circles is on blue line) Lower frequencies take forever to get this way so I have excluded them.
Not sure if you watched Erin’s (
@hardisj, just to tag him) talk with Klippel (1hr 23min mark):
You
don’t look at the highest order to determine far-field, you
look at Total Power. Look at how huge your y-axis is, that is throwing off the intuitive nature, we don’t need the 11th spherical harmonic to be -200dB down from the monopole. He states (as well as one of Klippel’s PDFs) that
the far-field limit is when Total Power reaches 0.5dB from being monopole.
Also, showing it at 400Hz just shows it at 400Hz, not it and above.
So at 400Hz it’s not 1.54m but around 10^(-0.8)m (your scale is too huge to see 0.5dB increments). This makes sense as it’s mostly the woofer playing that frequency. You stated as you went lower in Hz that the distance increased,
which makes sense as this is a rear-ported speaker so the sound field is more complex in the bass and you need to be further away for the port and woofer to sum.
The guy at Klippel said that they are working on generating far-field transition distance for all frequencies, but that it needs work.
However, due to my understanding, there is a manual way. You first look at the Radiated Sound Power graph:
And
look at where the monopole nature is most reduced, in this case around 1500Hz.
I am willing to bet if you look at the Apparent Sound Power for ~1500Hz, it will have the max distance to be considered far-field.
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Assuming the Apparent Sound Power data can be exported, can it only be exported as 1 frequency (what the graph is limited to), or can you export it for all frequencies? Because if so and you are willing, I can find the far-field distance.