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* Radial weight function (`circ_radial_weights', `circular_pw`, `circular_ls') now returns a vector of length 2*N+1 with N being the maximum modal order * The ordering is consistant with the previous implementation: 0,1,...,N,-N,...-1 * In `circ_diagonal_modal_mat`, mirroring of the radial weights is no longer necessary. So `mirror_vec` will be depricated
* The modal bandwidth of the incident sound field `Nsf` may differ from that of the modal beamforming `N` * For open circular arrays, the incident sound can have either a finite or an infinite modal bandwidth
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Example for modal analysis and sound field extrapolation
capture the sound field of a monochromatic plane wave by an open circular array
compute the circular harmonics expansion coefficients up to order
N. As shown below, The CHT coefficientspmis obtained by multiplying the regularized radial weightsdnwith the IDFT of the captured signalp. No matrix computation is needed. The reason for using IDFT (not DFT) is due to our choice of the circular harmonics asnp.exp(-1j*n*phi).sfa-numpy/examples/sound_field_extrapolation_open_circular_array_mono.py
Lines 36 to 38 in 3da5e01
extrapolate the sound field on 2-dimensional grid points
sfa-numpy/examples/sound_field_extrapolation_open_circular_array_mono.py
Lines 40 to 43 in 3da5e01
results


CAUTION
One line in
regularizewas commented out so that it works for mono-frequency cases. This issue is being handled in #4.sfa-numpy/micarray/modal/radial.py
Lines 179 to 183 in 3da5e01