Skip to content
New issue

Have a question about this project? Sign up for a free GitHub account to open an issue and contact its maintainers and the community.

Sign up for GitHub

By clicking “Sign up for GitHub”, you agree to our terms of service and privacy statement. We’ll occasionally send you account related emails.

Already on GitHub? Sign in to your account

Jump to bottom

Prediction of Aliasing Frequency #184

Open
wants to merge 3 commits into
base: master
Choose a base branch
from
Open

Prediction of Aliasing Frequency #184

Show file tree
Hide file tree
Changes from all commits
Commits
Show all changes
3 commits
Select commit Hold shift + click to select a range
74c7ad2
initial commit for aliasing model
Nov 6, 2018
e6a0965
add support for discretised virtual secondary source distribution and…
Nov 15, 2018
ea8cd4e
add test function for aliasing frequency
Nov 15, 2018
File filter

Filter by extension

Filter by extension
Conversations
Failed to load comments.
Loading
Jump to
Jump to file
Failed to load files.
Loading
Diff view
Diff view
161 changes: 161 additions & 0 deletions SFS_aliasing/aliasing_extended_sbl.m
View file
Open in desktop
Original file line number Diff line number Diff line change
@@ -0,0 +1,161 @@
function f = aliasing_extended_sbl(x0, kS, x, minmax_kGt_fun, xc, M, Npw, conf)
%ALIASING_EXTENDED_SBL aliasing frequency for an extended listening area for
%an circular control area at xc with R=M/k where synthesis is focused on.
%
% Usage: f = aliasing_extended_control(x0, kSx0, x, minmax_kGt_fun, minmax_kSt_fun, conf)
%
% Input options:
% x0 - position, direction, and sampling distance of
% secondary sources [N0x7] / m
% kSx0 - normalised local wavenumber vector of virtual sound
% field [N0x3]
% x - position for which aliasing frequency is calculated
% [Nx3]
% minmax_kGt_fun - function handle to determine the extremal value of
% the tangential component of k_G(x-x0)
% [kGtmin, kGtmax] = minmax_kGt_fun(x0)
% xc - center of circular control area
% M - modal order which defines the radius R=M/k
% Npw -
% conf - configuration struct (see SFS_config)
%
% Output parameters:
% f - aliasing frequency [Nx1]
%

%*****************************************************************************
% The MIT License (MIT) *
% *
% Copyright (c) 2010-2018 SFS Toolbox Developers *
% *
% Permission is hereby granted, free of charge, to any person obtaining a *
% copy of this software and associated documentation files (the "Software"), *
% to deal in the Software without restriction, including without limitation *
% the rights to use, copy, modify, merge, publish, distribute, sublicense, *
% and/or sell copies of the Software, and to permit persons to whom the *
% Software is furnished to do so, subject to the following conditions: *
% *
% The above copyright notice and this permission notice shall be included in *
% all copies or substantial portions of the Software. *
% *
% THE SOFTWARE IS PROVIDED "AS IS", WITHOUT WARRANTY OF ANY KIND, EXPRESS OR *
% IMPLIED, INCLUDING BUT NOT LIMITED TO THE WARRANTIES OF MERCHANTABILITY, *
% FITNESS FOR A PARTICULAR PURPOSE AND NONINFRINGEMENT. IN NO EVENT SHALL *
% THE AUTHORS OR COPYRIGHT HOLDERS BE LIABLE FOR ANY CLAIM, DAMAGES OR OTHER *
% LIABILITY, WHETHER IN AN ACTION OF CONTRACT, TORT OR OTHERWISE, ARISING *
% FROM, OUT OF OR IN CONNECTION WITH THE SOFTWARE OR THE USE OR OTHER *
% DEALINGS IN THE SOFTWARE. *
% *
% The SFS Toolbox allows to simulate and investigate sound field synthesis *
% methods like wave field synthesis or higher order ambisonics. *
% *
% http://sfstoolbox.org [email protected] *
%*****************************************************************************

% shift coordinates to expansion centre xc
x = bsxfun(@minus, x, xc);
x0(:,1:3) = bsxfun(@minus, x0(:,1:3), xc);

phin0 = cart2pol(x0(:,4),x0(:,5)); % azimuth angle of normal vector n0(x0)
deltax0 = abs(x0(:,7)); % sampling distance delta_x0(x0)
phik = cart2pol(kS(:,1),kS(:,2)); % azimuth angle of kS(x0)

select = cos(phin0 - phik) >= 0; % secondary source selection
gdx = find(select);

% quantities for selected secondary sources
x0select = x0(select,:);
[phix0select, rx0select] = cart2pol(x0select(:,1),x0select(:,2));
deltax0select = deltax0(select); % sampling distance
kSselect = kS(select,:);
phikselect = phik(select);
kStselect = sin(phin0(select) - phikselect); % tangential component of kS(x0)

% wavelength at which secondary source x0 turn inactive due to spatial
% bandwidth limitation
lambdaMselect = 2.*pi/M.*rx0select.*abs(sin(phix0select - phikselect));

f = inf(size(x,1), 1);
if Npw < M
f(:) = 0;
return
end

eps = 0.01;

for xdx = 1:size(x,1);

vectorxx0 = bsxfun(@minus, x(xdx,:), x0(:,1:3)); % vector x - x0
[phixx0,rxx0] = cart2pol(vectorxx0(:,1),vectorxx0(:,2)); % polar coordinates
% mininum and maximum values of k_Gt(x - x_0)
% (tangential component of k_G(x-x0))
[kGtmin, kGtmax] = minmax_kGt_fun(x0,x(xdx,:));
kGtminselect = kGtmin(gdx);
kGtmaxselect = kGtmax(gdx);

lambda = 0;

% aliasing wavelength for eta=1 and zeta=0
lambda10 = deltax0select.* ...
max(abs(kStselect-kGtminselect),abs(kStselect-kGtmaxselect));
% select all wavelengths, that above the limit of the spatial bandwidth
% limitation
select = lambda10 >= lambdaMselect;
if any(select)
lambda = max(lambda, max(lambda10(select)));
end

if isinf(Npw)
f(xdx) = conf.c./lambda;
continue;
end

% aliasing wavelength for eta=0 and zeta=1
lambda01 = 2.*pi./Npw.*rxx0(gdx).*abs(sin(phixx0(gdx)-phikselect));
% select all wavelengths, that above the limit of the spatial bandwidth
% limitation
select = lambda01 >= lambdaMselect;
if any(select)
lambda = max(lambda, max(lambda01(select)));
end

% aliasing wavelength for eta=1 and zeta=1
for sdx=1:size(x0select,1); % interate over all active x0'

% secondary source selection for ALL x0 with a single kS(x0')
active = x0(:,4:6)*kSselect(sdx,:).' >= 0;

% vector x0 - x0'
vectorx0x0p = bsxfun(@minus, x0(active,1:3), x0select(sdx,1:3));
% polar angle and radius of vector (x0-x0')
[phix0x0p,rx0x0p] = cart2pol(vectorx0x0p(:,1),vectorx0x0p(:,2));

% range for aliasing wavelength at x0' caused by Discrete SSD (eta = 1)
lambda10x0p1 = ...
abs(sin(phin0(active) - phikselect(sdx))-kGtmin(active)) ...
.*deltax0(active);
lambda10x0p2 = ...
abs(sin(phin0(active) - phikselect(sdx))-kGtmax(active)) ...
.*deltax0(active);
lambda10x0pmin = min(lambda10x0p1,lambda10x0p2);
lambda10x0pmax = max(lambda10x0p1,lambda10x0p2);

% aliasing wavelength at x0' caused by Plane Wave Decomposition (zeta = 1)
lambda01x0p = 2.*pi/Npw.*rx0x0p.*abs(sin(phix0x0p - phikselect(sdx)));

% select x0' where PWD wavelength is in the range of SSD wavelength
select = lambda01x0p < (1+eps).*lambda10x0pmax & ...
lambda10x0pmin < (1+eps).*lambda01x0p;
if any(select)
lambda11 = lambda01x0p(select);
% select all wavelengths, that above the limit of the spatial bandwidth
% limitation
select = lambda11 >= lambdaMselect(sdx);
if any(select)
lambda = max(lambda, max(lambda11(select)));
end
end
end

f(xdx) = conf.c./lambda;
end
122 changes: 122 additions & 0 deletions SFS_aliasing/aliasing_extended_vss.m
View file
Open in desktop
Original file line number Diff line number Diff line change
@@ -0,0 +1,122 @@
function f = aliasing_extended_vss(x0, xv, kSxv, x, minmax_kGt_fun, conf)
%ALIASING_EXTENDED_CONTROL aliasing frequency for an extended listening area
%with an defined control area where the sound field synthesis is prioritized
%
% Usage: f = aliasing_extended_control(x0, kSx0, x, minmax_kGt_fun, minmax_kSt_fun, conf)
%
% Input options:
% x0 - position, direction, and sampling distance of
% secondary sources [N0x7] / m
% kSx0 - normalised local wavenumber vector kS(x0)
% of virtual sound field at x0 [N0x3]
% x - position for which aliasing frequency is calculated
% [Nx3]
% minmax_kGt_fun - function handle to determine the extremal value of
% the tangential component of k_G(x-x0)
% [kGtmin, kGtmax] = minmax_kGt_fun(x0,x)
% minmax_kSt_fun - function handle to determine the extremal value of
% the tangential component of k_S(x0)
% [kStmin, kStmax] = minmax_kSt_fun(x0)
% conf - configuration struct (see SFS_config)
%
% Output parameters:
% f - aliasing frequency [Nx1]
%

%*****************************************************************************
% The MIT License (MIT) *
% *
% Copyright (c) 2010-2018 SFS Toolbox Developers *
% *
% Permission is hereby granted, free of charge, to any person obtaining a *
% copy of this software and associated documentation files (the "Software"), *
% to deal in the Software without restriction, including without limitation *
% the rights to use, copy, modify, merge, publish, distribute, sublicense, *
% and/or sell copies of the Software, and to permit persons to whom the *
% Software is furnished to do so, subject to the following conditions: *
% *
% The above copyright notice and this permission notice shall be included in *
% all copies or substantial portions of the Software. *
% *
% THE SOFTWARE IS PROVIDED "AS IS", WITHOUT WARRANTY OF ANY KIND, EXPRESS OR *
% IMPLIED, INCLUDING BUT NOT LIMITED TO THE WARRANTIES OF MERCHANTABILITY, *
% FITNESS FOR A PARTICULAR PURPOSE AND NONINFRINGEMENT. IN NO EVENT SHALL *
% THE AUTHORS OR COPYRIGHT HOLDERS BE LIABLE FOR ANY CLAIM, DAMAGES OR OTHER *
% LIABILITY, WHETHER IN AN ACTION OF CONTRACT, TORT OR OTHERWISE, ARISING *
% FROM, OUT OF OR IN CONNECTION WITH THE SOFTWARE OR THE USE OR OTHER *
% DEALINGS IN THE SOFTWARE. *
% *
% The SFS Toolbox allows to simulate and investigate sound field synthesis *
% methods like wave field synthesis or higher order ambisonics. *
% *
% http://sfstoolbox.org [email protected] *
%*****************************************************************************

phik = cart2pol(kSxv(:,1),kSxv(:,2)); % azimuth angle of kS(xv)
phinv = cart2pol(xv(:,4),xv(:,5)); % azimuth angle of normal vector nv(xv)
phin0 = cart2pol(x0(:,4),x0(:,5)); % azimuth angle of normal vector n0(x0)

% selection of virtual secondary source
select = cos(phinv - phik) >= 0;
xv = xv(select,:);
% k_S,tv(xv) (tangential component of kS(xv) at xv )
kStv = sin(phinv(select) - phik(select));

% sampling distance
deltax0 = abs(x0(:,7));
deltaxv = abs(xv(:,7));

f = inf(size(x,1), 1);

eps = 0.01;
for xdx = 1:size(x,1);

% mininum and maximum values of k_G,tv(x-xv)
% (tangential component of k_G(x-xv) at xv)
[kGtvmin, kGtvmax] = minmax_kGt_fun(xv,x(xdx,:));
lambda = max(deltaxv.*max(abs(kStv-kGtvmin),abs(kStv-kGtvmax)));

% mininum and maximum values of k_G,t0(x-x0)
% (tangential component of k_G(x-x0) at x0)
[kGt0min, kGt0max] = minmax_kGt_fun(x0,x(xdx,:));

for vdx=1:size(xv,1) % interate over all active xv

vectorxvx0 = bsxfun(@minus, xv(vdx,1:3), x0(:,1:3)); % vector xv - x0

% secondary source selection for ALL x0 and a single xv
active = vectorxvx0*xv(vdx,4:6).' >= 0;

% polar angle and radius of vector (xv-x0)
phixvx0 = cart2pol(vectorxvx0(active,1),vectorxvx0(active,2));

% k_FS,tv(xv-x0) (tangential component of k_FS(xv-x0) at xv)
kFStv = sin(phinv(vdx) - phixvx0);
% k_FS,t0(xv-x0) (tangential component of k_FS(xv-x0) at x0)
kFSt0 = sin(phin0(active) - phixvx0);

% range for aliasing wavelength at x0 caused by discrete SSD (eta = 1)
lambda10_1 = abs(kFSt0 - kGt0min(active)).*deltax0(active);
lambda10_2 = abs(kFSt0 - kGt0max(active)).*deltax0(active);

lambda10min = min(lambda10_1,lambda10_2);
lambda10max = max(lambda10_1,lambda10_2);

% aliasing wavelength at xv caused by discrete virtual SSD (zeta = 1)
lambda01 = abs((kStv(vdx) - kFStv).*deltaxv(vdx));

% select the x0 where the virtual SSD wavelength is in the range of SSD
% wavelength
select = lambda01 < (1+eps).*lambda10max & lambda10min < (1+eps).*lambda01;
if any(select)
lambda = max(lambda, max(lambda01(select)));
end

select = lambda01 < eps;
if any(select)
lambda = max(lambda, max(lambda10max(select)));
end
end

f(xdx) = conf.c./lambda;
end
Loading