I was looking at this page from the Neumann website about sonic differences between large and small diameter condensers.
https://www.neumann.com/en-us/knowl...between-large-and-small-diaphragm-microphones
I understand why LDCs and SDCs will differ in their off-axis sound at high frequencies, with wavelengths comparable to the diaphragm diameter and shorter. (Any wavelength short enough that you have peaks and troughs diagonally across the diaphragm will mostly cancel out, because there will be stripes of high pressure across the diaphragm and stripes of low pressure in between. At long wavelengths, you'll have near-peak values across the whole diaphragm as the peaks go across, and likewise for troughs.)
To me, that would seem to mean that the effect would be to narrow the polar pattern a whole lot across a couple of octaves (?), dependent on the diaphragm diameter, and that the pattern for a small diameter (say 12 or 13 mm) diaphragm would be the about the same as for a large diameter (say 25 mm) diaphragm, just one octave higher.
But that is not what they show for examples. Here are the polar patterns by octave for a Neumann U87A LDC and a Neumann KM184 SDC
If you look at the plots for the U87A, the polar patterns vary significantly from octave to octave, being very subcardioid at 125 Hz, then somewhat less subcardioid at 250 and 500, then classically cardioid only at 1000 KHz, and supercardioid at 2000, and so on.
The plots for the KM184 are quite different. It is subcardioid only at 125 Hz, but looks classically cardioid at 250, and 500, and 1000, and 2000, and 4000. Above that it narrows a lot, as I'd expect, but there's a four-octave range (interestingly where human hearing is most acute) where the polar pattern hardly changes at all, rather than noticeably narrowing at each octave.
Is that normal?
I'm guessing this has something to do with the relationship between the diaphragm diameter and the front-to-back delay due to the capsule thickness and the acoustic delay network, but I don't understand it.
https://www.neumann.com/en-us/knowl...between-large-and-small-diaphragm-microphones
I understand why LDCs and SDCs will differ in their off-axis sound at high frequencies, with wavelengths comparable to the diaphragm diameter and shorter. (Any wavelength short enough that you have peaks and troughs diagonally across the diaphragm will mostly cancel out, because there will be stripes of high pressure across the diaphragm and stripes of low pressure in between. At long wavelengths, you'll have near-peak values across the whole diaphragm as the peaks go across, and likewise for troughs.)
To me, that would seem to mean that the effect would be to narrow the polar pattern a whole lot across a couple of octaves (?), dependent on the diaphragm diameter, and that the pattern for a small diameter (say 12 or 13 mm) diaphragm would be the about the same as for a large diameter (say 25 mm) diaphragm, just one octave higher.
But that is not what they show for examples. Here are the polar patterns by octave for a Neumann U87A LDC and a Neumann KM184 SDC
If you look at the plots for the U87A, the polar patterns vary significantly from octave to octave, being very subcardioid at 125 Hz, then somewhat less subcardioid at 250 and 500, then classically cardioid only at 1000 KHz, and supercardioid at 2000, and so on.
The plots for the KM184 are quite different. It is subcardioid only at 125 Hz, but looks classically cardioid at 250, and 500, and 1000, and 2000, and 4000. Above that it narrows a lot, as I'd expect, but there's a four-octave range (interestingly where human hearing is most acute) where the polar pattern hardly changes at all, rather than noticeably narrowing at each octave.
Is that normal?
I'm guessing this has something to do with the relationship between the diaphragm diameter and the front-to-back delay due to the capsule thickness and the acoustic delay network, but I don't understand it.
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