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3-D Sound and Spatial Audio
MUS_TECH 348 3-D Sound and Spatial Audio
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Intensity Panning with Loudspeakers
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sin (ß) / sin (q) = (L - R ) / (L + R)
Stereo Law of Sines sin (ß) / sin (q) = (L - R ) / (L + R) Where ß is the angle of the virtual image and q is the angle of the loudspeaker from center “Phaser Analysis of Some Stereophonic Phenomena” Ben Bauer 1961
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By the way, just HOW does panning work?
L R Panning with stereo loudspeakers includes crosstalk!
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Panning results in amplitude and phase difference!
Consider sine waves! a t a t L R a t a t Panning results in amplitude and phase difference!
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+ = Consider sine waves! L sin (2p f t) R sin (2p f t)
k (<1) and ø are constant for fixed loudspeaker & listener locations L sin (2p f t) + kR sin (2p f t + ø) L * R --- delayed (ø ) and reduced in gain (k) * t + t = t
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Consider sine waves! a t a t L R R sin (2p f t) + kL sin (2p f t + ø)
kR sin (2p f t + ø) What about the resulting IID and ITD?
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Consider sine waves! R and L affect the IID and interaural phase! a t
( L2 + k2R2 + 2 kLR cos (- ø) ) IID(in decibels) = 10 log (k2L2 + R2 + 2 kLR cos (- ø) ) L sin(2pft) + R sin(2pft+ ø) L cos(2pft) + R cos(2pft+ ø) Interaural phase = arctan R and L affect the IID and interaural phase!
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Panning Methods 0.5 amp Amplitude Panning L (C) R position 0.7
Intensity or Power Panning amp L (C) R position
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Panning Methods Near-field Monitoring: Large-space Monitoring:
Greatest accuracy: Low Frequencies: amplitude panning High Frequencies: power panning Large-space Monitoring: power panning
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Panning Inaccuracy High Low L (C) R position
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How well does panning work in typical multichannel settings like 5.1?
L C R S1 S2 S1 S2 S1 S2 S1 S2
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ITD / IID HRTF For side locations the only change is a cross fading of HRTFs! Cross fading does not produce proper HRTFs in the middle! HRTF only HRTF ITD / IID
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