-
Notifications
You must be signed in to change notification settings - Fork 3
Meshfree Shallow Water on a Sphere #25
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.
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
base: master
Are you sure you want to change the base?
Changes from 10 commits
ea7b64e
b03be54
8348d67
b0a239d
ed87c83
0fb67d0
1fd08f0
d22bd67
f881d62
5a75ff9
e991917
4dce007
9175541
e362c46
File filter
Filter by extension
Conversations
Jump to
Diff view
Diff view
There are no files selected for viewing
Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,78 @@ | ||
classdef Canonical < otp.mfshallowwatersphere.MFShallowWaterSphereProblem | ||
methods | ||
function obj = Canonical(varargin) | ||
|
||
load('nodes500.mat', 'x', 'y', 'z'); | ||
|
||
% mean water height | ||
H = 5.768e4; | ||
% earth gravity | ||
g = otp.utils.PhysicalConstants.EarthGravity; | ||
% radius of the earth | ||
a = otp.utils.PhysicalConstants.EarthRadius; | ||
% initial velocity for the perturbation | ||
u0 = 20; | ||
% Angular velocity of the earth | ||
Omega = otp.utils.PhysicalConstants.EarthAngularVelocity; | ||
|
||
coriolisForce = 2*Omega*z; | ||
|
||
params = struct; | ||
params.gravity = otp.utils.PhysicalConstants.EarthGravity; | ||
params.radius = a; | ||
params.angularSpeed = Omega; | ||
params.coriolisForce = coriolisForce; | ||
|
||
params.x = x; | ||
params.y = y; | ||
params.z = z; | ||
|
||
params.rbfradius = 1.5; | ||
params.rbf = @otp.utils.rbf.buhmann3; | ||
|
||
% convert from Cartesian to spherical coordinates | ||
theta = atan2(z, sqrt(x.^2 + y.^2)); | ||
There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. Can use hypot function |
||
lambda = atan2(y, x); | ||
|
||
%% Define the initial conditions | ||
% first get a stableish Rossby-Haurwitz wave with a wave number | ||
% of R = 7 | ||
R = 7; | ||
[h, zonalwind, meridionalwind] = getrossbyhaurwitzwave(x, y, z, Omega, a, g, R); | ||
|
||
% then, define perturbations to this wave in terms of the T-Z | ||
% initial condition. | ||
hpert = (1/g)*(H + 2*Omega*a*u0*( sin(theta).^3 ).*cos(theta).*sin(lambda)); | ||
zonalwindpert = (-3*u0*sin(theta).*( cos(theta).^2 ).*sin(lambda) + u0*( sin(theta).^3 ).*sin(lambda)); | ||
meridionalwindpert = (u0*( sin(theta).^2 ).*cos(lambda)); | ||
|
||
% remove the excess height and velocity | ||
%hpert = hpert - mean(hpert); | ||
%zonalwindpert = zonalwindpert - mean(zonalwindpert); | ||
%meridionalwindpert = meridionalwindpert - mean(meridionalwindpert); | ||
|
||
% mixing coefficient | ||
alpha = 0.5; | ||
|
||
% perturb the R-H wave | ||
h = alpha*h + (1 - alpha)*hpert; | ||
zonalwind = alpha*zonalwind + (1 - alpha)*zonalwindpert; | ||
meridionalwind = alpha*meridionalwind + (1 - alpha)*meridionalwindpert; | ||
|
||
% finally, convert to Cartesian coordinates | ||
[u, v, w] = velocitytocartesian(x, y, z, zonalwind, meridionalwind); | ||
|
||
huv0 = [h; u; v; w]; | ||
|
||
%% Do the rest | ||
|
||
oneday = 24*60*60; | ||
There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. Can use |
||
|
||
tspan = [0, oneday]; | ||
|
||
obj = [email protected](tspan, ... | ||
huv0, params); | ||
|
||
end | ||
end | ||
end |
Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,33 @@ | ||
% See | ||
% Williamson, David L., John B. Drake, James J. Hack, Rüdiger Jakob, and Paul N. Swarztrauber. | ||
% "A standard test set for numerical approximations to the shallow water equations in spherical geometry." | ||
% Journal of Computational Physics 102, no. 1 (1992): 211-224. | ||
function [h, zonalwind, meridionalwind] = getrossbyhaurwitzwave(x, y, z, Omega, a, g, wavenumber) | ||
|
||
if nargin < 7 | ||
wavenumber = 4; | ||
end | ||
|
||
omega = 7.848e-6; | ||
K = omega; | ||
h0 = 8.0e3; | ||
R = wavenumber; | ||
|
||
% convert from Cartesian to spherical coordinates | ||
theta = atan2(z, sqrt(x.^2 + y.^2)); | ||
lambda = atan2(y, x); | ||
|
||
zonalwind = a*omega*cos(theta) + a*K*( cos(theta).^(R-1) ).*( R*(sin(theta).^2) - (cos(theta).^2)).*cos(R*lambda); | ||
meridionalwind = -a*K*R*( cos(theta).^(R-1) ).*sin(theta).*sin(R*lambda); | ||
|
||
At = (R + 1)*( cos(theta).^2 ) + (2*(R^2) - R - 2) - (2*(R^2))./( cos(theta).^2 ); | ||
A = (omega/2)*(2*Omega + omega)*( cos(theta).^2 ) + ((K^2)/4)*( cos(theta).^(2*R) ).*At; | ||
|
||
Bt = R^2 + 2*R + 2 - ((R + 1).^2).*( cos(theta).^2 ); | ||
B = (2*(Omega + omega)*K)/((R+1)*(R+2)).*( cos(theta).^R ).*Bt; | ||
|
||
C = ((K^2)/4)*( cos(theta).^(2*R) ).*( (R+1)*( cos(theta).^2 ) - (R+2)); | ||
|
||
h = (1/g)*(h0 + (a^2)*( A + B.*cos(R*lambda) + C.*cos(2*R*lambda) )); | ||
|
||
end |
Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,12 @@ | ||
function [u, v, w] = velocitytocartesian(x, y, z, zonalwind, meridionalwind) | ||
|
||
% convert from Cartesian to spherical coordinates | ||
theta = atan2(z, sqrt(x.^2 + y.^2)); | ||
lambda = atan2(y, x); | ||
|
||
% convert from spherical to Cartesian velocity | ||
u = (-zonalwind.*sin(lambda).*cos(theta) - meridionalwind.*cos(lambda).*sin(theta)); | ||
v = (zonalwind.*cos(lambda).*cos(theta) - meridionalwind.*sin(lambda).*sin(theta)); | ||
w = (meridionalwind.*cos(theta)); | ||
|
||
end |
Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,173 @@ | ||
classdef MFShallowWaterSphereProblem < otp.Problem | ||
|
||
methods | ||
function obj = MFShallowWaterSphereProblem(timeSpan, y0, parameters) | ||
|
||
[email protected]('Meshfree Shallow Water on a Sphere', [], ... | ||
timeSpan, y0, parameters); | ||
|
||
end | ||
end | ||
|
||
properties (SetAccess = private) | ||
DistanceFunction | ||
end | ||
|
||
methods | ||
|
||
function plotSphere(obj, huv, projection) | ||
There was a problem hiding this comment. Choose a reason for hiding this commentThe reason will be displayed to describe this comment to others. Learn more. Inconsistent passing of axes to plotting functions |
||
if nargin < 3 | ||
projection = 'eqaazim'; | ||
end | ||
|
||
|
||
x = obj.Parameters.x; | ||
y = obj.Parameters.y; | ||
z = obj.Parameters.z; | ||
rbf = obj.Parameters.rbf; | ||
|
||
Nplot = 50; | ||
lambdaplot = linspace(-pi, pi, Nplot); | ||
thetaplot = linspace(-pi/2, pi/2, Nplot); | ||
[lambdainterpgrid, thetainterpgrid] = meshgrid(lambdaplot, thetaplot); | ||
|
||
% get the cartesian coordinates for the uniform mesh | ||
[x2, y2, z2] = sph2cart(lambdainterpgrid(:), thetainterpgrid(:), ones(numel(lambdainterpgrid), 1)); | ||
radiusplot = 0.5; | ||
|
||
% | ||
Winterp = rbfinterp(x, y, z, x2, y2, z2, radiusplot, rbf); | ||
Winterp = Winterp./sum(Winterp, 2); | ||
|
||
lon = 360*(lambdainterpgrid/pi + 1)/2; | ||
lat = 180*(thetainterpgrid/(pi/2))/2; | ||
|
||
|
||
load('coastlines', 'coastlat', 'coastlon'); | ||
|
||
n = size(huv, 1)/4; | ||
h = huv(1:n); | ||
%u = huv((n+1):(2*n)); | ||
%v = huv((2*n+1):end); | ||
|
||
Nplot = sqrt(size(Winterp, 1)); | ||
|
||
cmap = interp1([0; 0.5; 1], [1, 0, 0; 1, 1, 1; 0, 0.3, 0.8], linspace(0, 1, 500)); | ||
levels = 20; | ||
|
||
%colormap(cmap); | ||
|
||
%subplot(1, 3, 1); | ||
cla; | ||
axesm(projection); | ||
contourfm(lat, lon, reshape(Winterp*h, Nplot, Nplot), levels, 'LineStyle','none'); | ||
colorbar; | ||
ax = gca; | ||
setm(ax,'FLineWidth', 3, 'Grid','on') | ||
l = plotm(coastlat, coastlon, '-k'); | ||
l.Color = [l.Color, 0.5]; | ||
|
||
% subplot(1, 3, 2); cla; | ||
% axesm(projection); | ||
% contourfm(lat, lon, reshape(Winterp*u, Nplot, Nplot), levels, 'LineStyle','none'); | ||
% colorbar; | ||
% ax = gca; | ||
% setm(ax,'FLineWidth', 3, 'Grid','on') | ||
% l = plotm(coastlat, coastlon, '-k'); | ||
% l.Color = [l.Color, 0.5]; | ||
% | ||
% subplot(1, 3, 3); cla; | ||
% axesm(projection); | ||
% contourfm(lat, lon, reshape(Winterp*v, Nplot, Nplot), levels, 'LineStyle','none'); | ||
% colorbar; | ||
% ax = gca; | ||
% setm(ax,'FLineWidth', 3, 'Grid','on') | ||
% l = plotm(coastlat, coastlon, '-k'); | ||
% l.Color = [l.Color, 0.5]; | ||
|
||
drawnow; | ||
|
||
|
||
end | ||
|
||
|
||
end | ||
|
||
|
||
methods (Access = protected) | ||
|
||
function onSettingsChanged(obj) | ||
x = obj.Parameters.x; | ||
y = obj.Parameters.y; | ||
z = obj.Parameters.z; | ||
g = obj.Parameters.gravity; | ||
a = obj.Parameters.radius; | ||
rbf = obj.Parameters.rbf; | ||
rbfradius = obj.Parameters.rbfradius; | ||
f = obj.Parameters.coriolisForce; | ||
|
||
% create the interpolation matrix and derivatives | ||
[W, dWdx, dWdy, dWdz] = rbfinterp(x, y, z, x, y, z, rbfradius, rbf); | ||
|
||
Bx = dWdx.*(1 - x.^2) + dWdy.*(-x.*y) + dWdz.*(-x.*z); | ||
By = dWdx.*(-x.*y) + dWdy.*(1 - y.^2) + dWdz.*(-y.*z); | ||
Bz = dWdx.*(-x.*z) + dWdy.*(-y.*z) + dWdz.*(1 - z.^2); | ||
|
||
Bx = Bx/a; | ||
By = By/a; | ||
Bz = Bz/a; | ||
|
||
try | ||
Wdecomp = decomposition(W, 'chol'); | ||
catch | ||
error('The selected compination of RBF, radius, and nodes did not result in a SPD collocation matrix.') | ||
end | ||
|
||
% build Shepard interpolation matrix | ||
S = W./sum(W, 2); | ||
|
||
% set the right hand side | ||
obj.Rhs = otp.Rhs(@(t, huvw) ... | ||
otp.mfshallowwatersphere.f(huvw, S, Wdecomp, Bx, By, Bz, f, g, x, y, z)); | ||
|
||
|
||
%% Distance function | ||
|
||
theta = atan2(z, sqrt(x.^2 + y.^2)); | ||
lambda = atan2(y, x); | ||
|
||
obj.DistanceFunction = @(t, huv, i, j) otp.mfshallowwatersphere.distfn(t, huv, i, j, theta, lambda); | ||
|
||
end | ||
|
||
function validateNewState(obj, newTimeSpan, newY0, newParameters) | ||
|
||
[email protected](obj, ... | ||
newTimeSpan, newY0, newParameters) | ||
|
||
%otp.utils.StructParser(newParameters) ... | ||
% .checkField('nx', 'finite', 'scalar', 'integer', 'positive') ... | ||
% .checkField('ny', 'finite', 'scalar', 'integer', 'positive') ... | ||
% .checkField('Re', 'finite', 'scalar', 'real', 'positive') ... | ||
% .checkField('Ro', 'finite', 'scalar', 'real'); | ||
|
||
end | ||
|
||
function label = internalIndex2label(obj, index) | ||
|
||
|
||
label = []; | ||
|
||
%[i, j] = ind2sub([obj.Parameters.nx, obj.Parameters.ny], index); | ||
|
||
%label = sprintf('(%d, %d)', i, j); | ||
|
||
end | ||
|
||
function sol = internalSolve(obj, varargin) | ||
% This really requires an SSP method | ||
sol = [email protected](obj, 'Method', @ode45, varargin{:}); | ||
end | ||
|
||
end | ||
end |
Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,20 @@ | ||
function d = distfn(~, ~, i, j, theta, lambda) | ||
|
||
n = numel(lambda); | ||
|
||
i = mod(i - 1, n) + 1; | ||
j = mod(j - 1, n) + 1; | ||
|
||
li = lambda(i); | ||
pi = theta(i); | ||
|
||
lj = lambda(j); | ||
pj = theta(j); | ||
|
||
dell = li - lj; | ||
|
||
nom = sqrt( ( cos(pj).*sin(dell) ).^2 + ( cos(pi).*sin(pj) - sin(pi).*cos(pj).*cos(dell) ).^2 ); | ||
den = sin(pi).*sin(pj) + cos(pi).*cos(pj).*cos(dell); | ||
d = atan2( nom, den ).'; | ||
|
||
end |
Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,47 @@ | ||
% See | ||
% Flyer, Natasha, and Grady B. Wright. | ||
% "A radial basis function method for the shallow water equations on a sphere." | ||
% Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences 465, no. 2106 (2009): 1949-1976. | ||
|
||
function dhuvwdt = f(huvw, S, Wdecomp, Bx, By, Bz, f, g, x, y, z) | ||
|
||
n = size(huvw, 1)/4; | ||
|
||
h = huvw(1:n, :); | ||
u = huvw((n+1):(2*n), :); | ||
v = huvw((2*n+1):(3*n), :); | ||
w = huvw((3*n+1):end, :); | ||
|
||
ch = Wdecomp\h; | ||
cu = Wdecomp\u; | ||
cv = Wdecomp\v; | ||
cw = Wdecomp\w; | ||
|
||
Bxch = Bx*ch; | ||
Bych = By*ch; | ||
Bzch = Bz*ch; | ||
|
||
Bxcu = Bx*cu; | ||
Bycv = By*cv; | ||
Bzcw = Bz*cw; | ||
|
||
rhsDx = u.*(Bxcu) + v.*(By*cu) + w.*(Bz*cu) + f.*(y.*w - z.*v) + g*Bxch; | ||
rhsDy = u.*(Bx*cv) + v.*(Bycv) + w.*(Bz*cv) + f.*(z.*u - x.*w) + g*Bych; | ||
rhsDz = u.*(Bx*cw) + v.*(By*cw) + w.*(Bzcw) + f.*(x.*v - y.*u) + g*Bzch; | ||
|
||
dudt = -( rhsDx.*(1 - x.^2) + rhsDy.*(-x.*y) + rhsDz.*(-x.*z) ); | ||
dvdt = -( rhsDx.*(-x.*y) + rhsDy.*(1 - y.^2) + rhsDz.*(-y.*z) ); | ||
dwdt = -( rhsDx.*(-x.*z) + rhsDy.*(-y.*z) + rhsDz.*(1 - z.^2) ); | ||
|
||
dhdt = -( u.*Bxch + v.*Bych + w.*Bzch + h.*(Bxcu + Bycv + Bzcw) ); | ||
|
||
% Shepard interpolation for stability | ||
dhdt = S*dhdt; | ||
dudt = S*dudt; | ||
dvdt = S*dvdt; | ||
dwdt = S*dwdt; | ||
|
||
dhuvwdt = [dhdt; dudt; dvdt; dwdt]; | ||
|
||
end | ||
|
There was a problem hiding this comment.
Choose a reason for hiding this comment
The reason will be displayed to describe this comment to others. Learn more.
Unnecessary line