Main [.m]

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Lisa Pizzo 2026-01-27 09:49:10 +01:00
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% Axisymmetric mug
% rz plane, rotation around r = 0
clear; clc; close all;
%% General values that we use in the entire script
%Task 3) Thermal conductivity
lambda_wall = 30; % ceramic
lambda_fluid = 0.6089; % water
lambda_air = 0.026; % air
%Task 4)
alpha = 10; % heat transfer coefficient
u_out = 18; % ambient air temperature (°C)
%Task 6) Volumetric heat capacities: rho * c_p
% Densities [kg/m^3]
rho_wall = 2400; % ceramic
rho_fluid = 1000; % water
rho_air = 1.2; % air
% Specific heats [J/(kg*K)]
cp_wall = 900;
cp_fluid = 4184;
cp_air = 1005;
% Volumetric heat capacities [J/(m^3*K)]
c_wall = rho_wall * cp_wall;
c_fluid = rho_fluid * cp_fluid;
c_air = rho_air * cp_air;
%% Task 1: Mesh definition
% Create PDE model
model = createpde();
% Points (meters)
A = [0, 0]; B = [0.055, 0];
C = [0.083, 0.105]; H = [0.078, 0.105];
F = [0.050, 0.005]; E = [0, 0.005];
G = [0.067, 0.066]; I = [0, 0.066];
D = [0, 0.105];
% Geometry matrix (edges)
g1 = [2; A(1); E(1); A(2); E(2); 1; 0]; % Axis - ceramic
g2 = [2; E(1); I(1); E(2); I(2); 2; 0]; % Axis - fluid
g3 = [2; I(1); D(1); I(2); D(2); 3; 0]; % Axis - air
g4 = [2; A(1); B(1); A(2); B(2); 1; 0]; % Outer ceramic
g5 = [2; B(1); C(1); B(2); C(2); 1; 0]; % Outer ceramic
g6 = [2; C(1); H(1); C(2); H(2); 1; 3]; % Top rim: (C-H) ceramic-air
g7 = [2; H(1); F(1); H(2); F(2); 1; 3]; % Inner ceramic wall (H-F) ceramic-air
g8 = [2; F(1); E(1); F(2); E(2); 1; 2]; % Inner ceramic bottom (F-E) ceramic-fluid
g9 = [2; F(1); G(1); F(2); G(2); 2; 3]; % Fluid surface (F-G) fluid-air
g10 = [2; G(1); I(1); G(2); I(2); 2; 3]; % Fluid surface (G-I) fluid-air
g11 = [2; D(1); H(1); D(2); H(2); 3; 0]; % Air top boundary: (D-H) air-outside
% Assemble geometry
g = [g1 g2 g3 g4 g5 g6 g7 g8 g9 g10 g11];
geometryFromEdges(model, g);
% figure(1);
% pdegplot(model, 'EdgeLabels','on', 'FaceLabels','on');
% axis equal;
% title('Geometry with edge and face labels');
% Generate mesh, linear and 3 nodes per element
mesh = generateMesh(model, 'Hmax', 0.002, 'GeometricOrder','linear');
% figure(2);
% pdemesh(model);
% axis equal;
% title('Generated mesh');
%% Task 2: Direct solver with constant lambda
nodes = mesh.Nodes; % coordinates of all mesh nodes
elements = mesh.Elements; % which nodes make up each triangle element
Nnodes = size(nodes,2);
Nelems = size(elements,2);
% Define material properties (for simplicity, lambda = 1 everywhere)
lambda = ones(Nelems,1); % thermal conductivity
% Initialize global stiffness matrix and RHS
K = sparse(Nnodes, Nnodes);
F = zeros(Nnodes,1);
% Assemble K and F
for e = 1:Nelems %Loop over each triangle element
vert = elements(:,e); %nodes of element
x = nodes(1,vert);
y = nodes(2,vert);
Ae = polyarea(x,y); % Compute area of the triangle
% Linear triangle gradients
b = [y(2)-y(3); y(3)-y(1); y(1)-y(2)]; % derivative with respect to x
c = [x(3)-x(2); x(1)-x(3); x(2)-x(1)]; % derivative with respect to y
% Element stiffness matrix
Ke = (lambda(e)/(4*Ae)) * (b*b.' + c*c.');
% Assemble
K(vert,vert) = K(vert,vert) + Ke;
% Element load vector (f=0)
F(vert) = F(vert) + zeros(3,1);
end
% Find boundary nodes (couldn't find a better way)
edgesAll = [elements([1 2],:), elements([2 3],:), elements([3 1],:)]; % all edges -> 2x(3*Nelems) awway since each triangle has 3 edges
edgesSorted = sort(edgesAll,1); % sort nodes of each edge, ensure that [i,j] and [j,i] are the same
[~,~,ic] = unique(edgesSorted','rows'); % identifies unique edges and assignes indices ic
counts = accumarray(ic,1); % counts how many times each edge appears in the mesh
boundaryEdges = find(counts==1); %edges belonging to only 1 element: hence on the boundary
boundaryNodes = unique(edgesSorted(:,boundaryEdges)); % nodes belonging to these boundary edges
% Direct solver
% Enforce Dirichlet BC strongly
K(boundaryNodes,:) = 0;
K(:,boundaryNodes) = 0;
K(boundaryNodes,boundaryNodes) = speye(length(boundaryNodes));
F(boundaryNodes) = 0;
% Direct solve
u = K \ F;
% figure(3)
% pdeplot(model, 'XYData', u, 'Mesh','on');
% axis equal;
% title('Stationary Dirichlet solution');
% colorbar;
%% Task 3: Laplace with multiple lambdas
[K, F] = CalculateLaplace_mult(model, lambda_wall, lambda_fluid, lambda_air);
% Enforce Dirichlet BC strongly
K(boundaryNodes,:) = 0;
K(:,boundaryNodes) = 0;
K(boundaryNodes,boundaryNodes) = speye(length(boundaryNodes));
F(boundaryNodes) = 0;
% Direct solve
u = K \ F;
% % Plot solution
% figure(4)
% pdeplot(model,'XYData',u, 'Mesh','on');
% axis equal
% title('Task 3: Stationary solution with multiple conductivities');
% colorbar
%% Task 4: Robin boundary condition
[K, F] = CalculateLaplace_mult(model, lambda_wall, lambda_fluid, lambda_air);
[K, F] = ApplyRobinBC_mult(model, K, F, alpha, u_out);
% Direct solve
u = K \ F;
% figure(5)
% pdeplot(model, 'XYData', u, 'Mesh','on');
% axis equal
% title('Task 4: Stationary solution with Robin BC');
% colorbar
%% Task 5: Axisymmetric Laplace + Robin BC
[K, F] = CalculateLaplace_mult_rot(model, lambda_wall, lambda_fluid, lambda_air);
[K, F] = ApplyRobinBC_mult_rot(model, K, F, alpha, u_out);
% Direct solve
u = K \ F;
% figure(6)
% pdeplot(model, 'XYData', u, 'Mesh','on');
% axis equal
% title('Task 5: Axisymmetric stationary solution with Robin BC');
% colorbar
%To see it in 3D paste here the code in "AdditionalPlotCodes.txt".
%% Task 6: Axisymmetric mass matrix
M = sparse(Nnodes, Nnodes);
M = AddMass_mult_rot(model, M, c_wall, c_fluid, c_air);
%% Task 7: Initial solution
u0 = Init_Solution_mult(model, 18, 80, 18);
% figure(7)
% pdeplot(model, 'XYData', u0, 'Mesh','on');
% axis equal
% title('Initial temperature distribution');
% colorbar
%% Task 8: Time-dependent simulation (explicit scheme)
tau = 0.5; % time step in seconds
T_end = 400; % total simulation time (seconds)
Nt = ceil(T_end/tau); % number of time steps
A = (1/tau)*M+K; % Left-hand side matrix
u = u0;
for k = 1:Nt
b = (1/tau)*M*u + F; % F is the load vector, F=0
u_next = A\b;
u = u_next; % Update
if mod(k,20) == 0
% figure(8)
% pdeplot(model, 'XYData', u, 'Mesh','on');
% axis equal
% title(['Temperature at t = ', num2str(k*tau), ' s']);
% colorbar
% drawnow
end
end
%To see the 9 snapshots paste here the codes in "AdditionalPlotCodes.txt"
%% Task 9 (i): Heating time using inner ceramic wall temperature
T_target = 67; % [°C]
[K, F] = CalculateLaplace_mult_rot(model, lambda_wall, lambda_fluid, lambda_air);
[K, F] = ApplyRobinBC_mult_rot(model, K, F, alpha, u_out);
A = (1/tau)*M+K; % Left-hand side matrix
innerWallNodes = findNodes(model.Mesh,'region','Edge',8); % Edge 8 = ceramicfluid interface
u = u0;
% Storage
timeVec = (0:Nt-1)' * tau;
innerWallTemp = zeros(Nt,1);
Twarm = NaN;
for k = 1:Nt
b = (1/tau)*M*u + F;
u = A\b;
% Average inner wall temperature
innerWallTemp(k) = mean(u(innerWallNodes));
% Check heating criterion
if innerWallTemp(k) >= T_target
Twarm = k * tau;
fprintf('Task 9 (i): Inner wall reaches %.1f°C at T = %.1f s\n', ...
T_target, Twarm);
break
end
end
% figure(9)
% plot(timeVec(1:k), innerWallTemp(1:k), 'LineWidth', 2)
% hold on
% yline(T_target,'r--','67°C','LineWidth',1.5)
% xlabel('Time [s]')
% ylabel('Average inner wall temperature [°C]')
% title('Heating of the inner ceramic wall')
% grid on
%% CHECK: Insulated mug transient redistribution
[K_neu, F_neu] = CalculateLaplace_mult_rot(model,lambda_wall,lambda_fluid,lambda_air);
M_neu = sparse(Nnodes, Nnodes);
M_neu = AddMass_mult_rot(model,M_neu,c_wall,c_fluid,c_air);
% Time stepping parameters
tau = 0.5;
T_end = 400;
Nt = ceil(T_end / tau);
A_neu = (1/tau) * M_neu + K_neu;
% Initial condition
u = u0;
for k = 1:Nt
b = (1/tau) * M_neu * u + F_neu;
u = A_neu \ b;
if mod(k,20) == 0
% figure(10)
% pdeplot(model, 'XYData', u, 'Mesh','on');
% axis equal
% title(['Insulated mug, t = ', num2str(k*tau), ' s']);
% colorbar
% drawnow
end
end