205 lines
6.5 KiB
Rust
205 lines
6.5 KiB
Rust
//! Tests for D3Q19 Lattice Boltzmann Method implementation
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use approx::assert_relative_eq;
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use nalgebra::Vector3;
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use rtx_cfd::solvers::lbm::{D3Q19Parameters, D3Q19Solver};
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#[test]
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fn test_d3q19_lattice_velocities() {
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let solver = D3Q19Solver::new(10, 10, 10, D3Q19Parameters::default());
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let velocities = solver.lattice_velocities();
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// D3Q19 should have 19 velocities
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assert_eq!(velocities.len(), 19);
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// Check specific velocity directions
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assert_eq!(velocities[0], Vector3::new(0, 0, 0)); // Rest
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assert_eq!(velocities[1], Vector3::new(1, 0, 0)); // +X
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assert_eq!(velocities[2], Vector3::new(-1, 0, 0)); // -X
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assert_eq!(velocities[3], Vector3::new(0, 1, 0)); // +Y
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assert_eq!(velocities[4], Vector3::new(0, -1, 0)); // -Y
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assert_eq!(velocities[5], Vector3::new(0, 0, 1)); // +Z
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assert_eq!(velocities[6], Vector3::new(0, 0, -1)); // -Z
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}
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#[test]
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fn test_d3q19_weights() {
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let solver = D3Q19Solver::new(10, 10, 10, D3Q19Parameters::default());
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let weights = solver.weights();
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// D3Q19 should have 19 weights
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assert_eq!(weights.len(), 19);
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// Check weight values
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assert_relative_eq!(weights[0], 1.0 / 3.0, epsilon = 1e-12); // Rest particle
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assert_relative_eq!(weights[1], 1.0 / 18.0, epsilon = 1e-12); // Face neighbors
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assert_relative_eq!(weights[7], 1.0 / 36.0, epsilon = 1e-12); // Edge neighbors
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// Weights should sum to 1
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let sum: f64 = weights.iter().sum();
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assert_relative_eq!(sum, 1.0, epsilon = 1e-12);
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}
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#[test]
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fn test_d3q19_equilibrium_distribution() {
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let solver = D3Q19Solver::new(10, 10, 10, D3Q19Parameters::default());
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let density = 1.0;
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let velocity = Vector3::new(0.1, 0.05, 0.02);
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let f_eq = solver.equilibrium_distribution(density, &velocity);
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// Should have 19 components
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assert_eq!(f_eq.len(), 19);
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// All components should be positive
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for &val in &f_eq {
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assert!(
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val > 0.0,
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"Equilibrium distribution component should be positive"
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);
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}
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// Sum should equal density
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let sum: f64 = f_eq.iter().sum();
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assert_relative_eq!(sum, density, epsilon = 1e-12);
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}
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#[test]
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fn test_d3q19_equilibrium_at_rest() {
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let solver = D3Q19Solver::new(10, 10, 10, D3Q19Parameters::default());
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let density = 1.0;
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let velocity = Vector3::zeros();
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let f_eq = solver.equilibrium_distribution(density, &velocity);
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let weights = solver.weights();
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// For zero velocity, equilibrium should be density * weight
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for i in 0..19 {
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assert_relative_eq!(f_eq[i], density * weights[i], epsilon = 1e-12);
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}
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}
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#[test]
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fn test_d3q19_macroscopic_variables() {
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let mut solver = D3Q19Solver::new(10, 10, 10, D3Q19Parameters::default());
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// Initialize with known state
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let density = 1.2;
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let velocity = Vector3::new(0.1, -0.05, 0.03);
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// Set distribution functions to equilibrium
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let f_eq = solver.equilibrium_distribution(density, &velocity);
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solver.set_distribution_at(5, 5, 5, &f_eq);
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// Extract macroscopic variables
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let macro_vars = solver.macroscopic_variables_at(5, 5, 5);
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assert_relative_eq!(macro_vars.density, density, epsilon = 1e-12);
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assert_relative_eq!(macro_vars.velocity.x, velocity.x, epsilon = 1e-12);
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assert_relative_eq!(macro_vars.velocity.y, velocity.y, epsilon = 1e-12);
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assert_relative_eq!(macro_vars.velocity.z, velocity.z, epsilon = 1e-12);
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}
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#[test]
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fn test_d3q19_bgk_collision() {
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let mut solver = D3Q19Solver::new(10, 10, 10, D3Q19Parameters::new(0.6));
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// Initialize all cells with equilibrium
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let density = 1.0;
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let velocity = Vector3::new(0.1, 0.0, 0.0);
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solver.initialize_uniform(density, velocity);
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// Get original equilibrium distribution
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let f_eq = solver.equilibrium_distribution(density, &velocity);
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// Perturb from equilibrium by reducing a component
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let mut f = f_eq.clone();
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f[1] *= 0.8; // Reduce from equilibrium (80% of equilibrium value)
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solver.set_distribution_at(5, 5, 5, &f);
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let initial_value = f[1];
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// Apply collision step
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solver.collision_step();
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// Check that distribution moves toward equilibrium
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let f_after = solver.distribution_at(5, 5, 5);
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// With BGK collision: f_new = f - omega * (f - f_eq)
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// Since f[1] < f_eq[1], (f - f_eq) is negative, so f_new should increase
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assert!(
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f_after[1] > initial_value,
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"BGK should move towards equilibrium: {} > {}",
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f_after[1],
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initial_value
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);
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// Check that it's moving in the right direction (don't check exact value due to neighboring cell effects)
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let direction_to_equilibrium = f_eq[1] - initial_value;
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let actual_change = f_after[1] - initial_value;
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assert!(
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direction_to_equilibrium > 0.0 && actual_change > 0.0,
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"Should move towards equilibrium"
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);
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}
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#[test]
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fn test_d3q19_streaming_step() {
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let mut solver = D3Q19Solver::new(5, 5, 5, D3Q19Parameters::default());
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// Initialize central cell with specific distribution
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let mut f = vec![0.0; 19];
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f[1] = 1.0; // Only +X component
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solver.set_distribution_at(2, 2, 2, &f);
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// Apply streaming step
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solver.streaming_step();
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// Check that the distribution has moved in +X direction
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let f_east = solver.distribution_at(3, 2, 2);
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assert_relative_eq!(f_east[1], 1.0, epsilon = 1e-12);
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// Original cell should have zero +X component
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let f_original = solver.distribution_at(2, 2, 2);
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assert_relative_eq!(f_original[1], 0.0, epsilon = 1e-12);
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}
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#[test]
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fn test_d3q19_mass_conservation() {
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let nx = 8;
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let ny = 8;
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let nz = 8;
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let mut solver = D3Q19Solver::new(nx, ny, nz, D3Q19Parameters::default());
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// Initialize with uniform density
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solver.initialize_uniform(1.0, Vector3::new(0.05, 0.02, 0.01));
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let initial_mass = solver.total_mass();
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// Run simulation for several steps with periodic boundaries
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for _ in 0..50 {
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solver.step_periodic();
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}
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let final_mass = solver.total_mass();
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// Mass should be conserved
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assert_relative_eq!(final_mass, initial_mass, epsilon = 1e-12);
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}
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#[test]
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fn test_d3q19_parameters_validation() {
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// Valid parameters
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let valid_params = D3Q19Parameters::new(0.6);
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assert!(valid_params.validate().is_ok());
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// Invalid relaxation time (too small)
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let invalid_params = D3Q19Parameters::new(0.4);
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assert!(invalid_params.validate().is_err());
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// Invalid relaxation time (too large)
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let invalid_params = D3Q19Parameters::new(2.1);
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assert!(invalid_params.validate().is_err());
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}
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