dyna3/app-proto/src/engine.rs
2025-01-20 15:44:20 -08:00

642 lines
No EOL
23 KiB
Rust

use lazy_static::lazy_static;
use nalgebra::{Const, DMatrix, DVector, DVectorView, Dyn, SymmetricEigen};
use web_sys::{console, wasm_bindgen::JsValue}; /* DEBUG */
// --- elements ---
#[cfg(feature = "dev")]
pub fn point(x: f64, y: f64, z: f64) -> DVector<f64> {
DVector::from_column_slice(&[x, y, z, 0.5, 0.5*(x*x + y*y + z*z)])
}
// the sphere with the given center and radius, with inward-pointing normals
pub fn sphere(center_x: f64, center_y: f64, center_z: f64, radius: f64) -> DVector<f64> {
let center_norm_sq = center_x * center_x + center_y * center_y + center_z * center_z;
DVector::from_column_slice(&[
center_x / radius,
center_y / radius,
center_z / radius,
0.5 / radius,
0.5 * (center_norm_sq / radius - radius)
])
}
// the sphere of curvature `curv` whose closest point to the origin has position
// `off * dir` and normal `dir`, where `dir` is a unit vector. setting the
// curvature to zero gives a plane
pub fn sphere_with_offset(dir_x: f64, dir_y: f64, dir_z: f64, off: f64, curv: f64) -> DVector<f64> {
let norm_sp = 1.0 + off * curv;
DVector::from_column_slice(&[
norm_sp * dir_x,
norm_sp * dir_y,
norm_sp * dir_z,
0.5 * curv,
off * (1.0 + 0.5 * off * curv)
])
}
// --- partial matrices ---
struct MatrixEntry {
index: (usize, usize),
value: f64
}
pub struct PartialMatrix(Vec<MatrixEntry>);
impl PartialMatrix {
pub fn new() -> PartialMatrix {
PartialMatrix(Vec::<MatrixEntry>::new())
}
pub fn push_sym(&mut self, row: usize, col: usize, value: f64) {
let PartialMatrix(entries) = self;
entries.push(MatrixEntry { index: (row, col), value: value });
if row != col {
entries.push(MatrixEntry { index: (col, row), value: value });
}
}
/* DEBUG */
pub fn log_to_console(&self) {
let PartialMatrix(entries) = self;
for ent in entries {
let ent_str = format!(" {} {} {}", ent.index.0, ent.index.1, ent.value);
console::log_1(&JsValue::from(ent_str.as_str()));
}
}
fn proj(&self, a: &DMatrix<f64>) -> DMatrix<f64> {
let mut result = DMatrix::<f64>::zeros(a.nrows(), a.ncols());
let PartialMatrix(entries) = self;
for ent in entries {
result[ent.index] = a[ent.index];
}
result
}
fn sub_proj(&self, rhs: &DMatrix<f64>) -> DMatrix<f64> {
let mut result = DMatrix::<f64>::zeros(rhs.nrows(), rhs.ncols());
let PartialMatrix(entries) = self;
for ent in entries {
result[ent.index] = ent.value - rhs[ent.index];
}
result
}
}
// --- configuration subspaces ---
#[derive(Clone)]
pub struct ConfigSubspace {
assembly_dim: usize,
basis_std: Vec<DMatrix<f64>>,
basis_proj: Vec<DMatrix<f64>>
}
impl ConfigSubspace {
pub fn zero(assembly_dim: usize) -> ConfigSubspace {
ConfigSubspace {
assembly_dim: assembly_dim,
basis_proj: Vec::new(),
basis_std: Vec::new()
}
}
// approximate the kernel of a symmetric endomorphism of the configuration
// space for `assembly_dim` elements. we consider an eigenvector to be part
// of the kernel if its eigenvalue is smaller than the constant `THRESHOLD`
fn symmetric_kernel(a: DMatrix<f64>, proj_to_std: DMatrix<f64>, assembly_dim: usize) -> ConfigSubspace {
// find a basis for the kernel, expressed in the standard coordinates
const ELEMENT_DIM: usize = 5;
const THRESHOLD: f64 = 1.0e-4;
let eig = SymmetricEigen::new(a);
let eig_vecs = eig.eigenvectors.column_iter();
let eig_pairs = eig.eigenvalues.iter().zip(eig_vecs);
let basis_std = DMatrix::from_columns(
eig_pairs.filter_map(
|(λ, v)| (λ.abs() < THRESHOLD).then_some(v)
).collect::<Vec<_>>().as_slice()
);
/* DEBUG */
// print the eigenvalues
#[cfg(all(target_family = "wasm", target_os = "unknown"))]
console::log_1(&JsValue::from(
format!("Eigenvalues used to find kernel:{}", eig.eigenvalues)
));
// express the basis in the projection coordinates
let basis_proj = proj_to_std.clone().qr().solve(&basis_std).unwrap();
// orthonormalize the basis with respect to the projection inner product
let basis_proj_orth = basis_proj.qr().q();
let basis_std_orth = proj_to_std * &basis_proj_orth;
// print the projection basis in projection coordinates
#[cfg(all(target_family = "wasm", target_os = "unknown"))]
console::log_1(&JsValue::from(
format!("Basis in projection coordinates:{}", basis_proj_orth)
));
ConfigSubspace {
assembly_dim: assembly_dim,
basis_std: basis_std_orth.column_iter().map(
|v| Into::<DMatrix<f64>>::into(
v.reshape_generic(Dyn(ELEMENT_DIM), Dyn(assembly_dim))
)
).collect(),
basis_proj: basis_proj_orth.column_iter().map(
|v| Into::<DMatrix<f64>>::into(
v.reshape_generic(Dyn(ELEMENT_DIM), Dyn(assembly_dim))
)
).collect()
}
}
pub fn dim(&self) -> usize {
self.basis_std.len()
}
pub fn assembly_dim(&self) -> usize {
self.assembly_dim
}
// find the projection onto this subspace of the motion where the element
// with the given column index has velocity `v`. the velocity is given in
// projection coordinates, and the projection is done with respect to the
// projection inner product
pub fn proj(&self, v: &DVectorView<f64>, column_index: usize) -> DMatrix<f64> {
if self.dim() == 0 {
const ELEMENT_DIM: usize = 5;
DMatrix::zeros(ELEMENT_DIM, self.assembly_dim)
} else {
self.basis_proj.iter().zip(self.basis_std.iter()).map(
|(b_proj, b_std)| b_proj.column(column_index).dot(&v) * b_std
).sum()
}
}
}
// --- descent history ---
pub struct DescentHistory {
pub config: Vec<DMatrix<f64>>,
pub scaled_loss: Vec<f64>,
pub neg_grad: Vec<DMatrix<f64>>,
pub min_eigval: Vec<f64>,
pub base_step: Vec<DMatrix<f64>>,
pub backoff_steps: Vec<i32>
}
impl DescentHistory {
fn new() -> DescentHistory {
DescentHistory {
config: Vec::<DMatrix<f64>>::new(),
scaled_loss: Vec::<f64>::new(),
neg_grad: Vec::<DMatrix<f64>>::new(),
min_eigval: Vec::<f64>::new(),
base_step: Vec::<DMatrix<f64>>::new(),
backoff_steps: Vec::<i32>::new(),
}
}
}
// --- gram matrix realization ---
// the Lorentz form
lazy_static! {
pub static ref Q: DMatrix<f64> = DMatrix::from_row_slice(5, 5, &[
1.0, 0.0, 0.0, 0.0, 0.0,
0.0, 1.0, 0.0, 0.0, 0.0,
0.0, 0.0, 1.0, 0.0, 0.0,
0.0, 0.0, 0.0, 0.0, -2.0,
0.0, 0.0, 0.0, -2.0, 0.0
]);
}
struct SearchState {
config: DMatrix<f64>,
err_proj: DMatrix<f64>,
loss: f64
}
impl SearchState {
fn from_config(gram: &PartialMatrix, config: DMatrix<f64>) -> SearchState {
let err_proj = gram.sub_proj(&(config.tr_mul(&*Q) * &config));
let loss = err_proj.norm_squared();
SearchState {
config: config,
err_proj: err_proj,
loss: loss
}
}
}
fn basis_matrix(index: (usize, usize), nrows: usize, ncols: usize) -> DMatrix<f64> {
let mut result = DMatrix::<f64>::zeros(nrows, ncols);
result[index] = 1.0;
result
}
// given a normalized vector `v` representing an element, build a basis for the
// element's linear configuration space consisting of:
// - the unit translation motions of the element
// - the unit shrinking motion of the element, if it's a sphere
// - one or two vectors whose coefficients vanish on the tangent space of the
// normalization variety
pub fn local_unif_to_std(v: DVectorView<f64>) -> DMatrix<f64> {
const ELEMENT_DIM: usize = 5;
let curv = 2.0*v[3];
if v.dot(&(&*Q * v)) < 0.5 {
// `v` represents a point. the normalization condition says that the
// curvature component of `v` is 1/2
DMatrix::from_column_slice(ELEMENT_DIM, ELEMENT_DIM, &[
curv, 0.0, 0.0, 0.0, v[0],
0.0, curv, 0.0, 0.0, v[1],
0.0, 0.0, curv, 0.0, v[2],
v[0], v[1], v[2], v[3], v[4],
0.0, 0.0, 0.0, 0.0, 1.0
])
} else {
// `v` represents a sphere. the normalization condition says that the
// Lorentz product of `v` with itself is 1
DMatrix::from_column_slice(ELEMENT_DIM, ELEMENT_DIM, &[
curv, 0.0, 0.0, 0.0, v[0],
0.0, curv, 0.0, 0.0, v[1],
0.0, 0.0, curv, 0.0, v[2],
curv*v[0], curv*v[1], curv*v[2], curv*v[3], curv*v[4] + 1.0,
v[0], v[1], v[2], v[3], v[4]
])
}
}
// use backtracking line search to find a better configuration
fn seek_better_config(
gram: &PartialMatrix,
state: &SearchState,
base_step: &DMatrix<f64>,
base_target_improvement: f64,
min_efficiency: f64,
backoff: f64,
max_backoff_steps: i32
) -> Option<(SearchState, i32)> {
let mut rate = 1.0;
for backoff_steps in 0..max_backoff_steps {
let trial_config = &state.config + rate * base_step;
let trial_state = SearchState::from_config(gram, trial_config);
let improvement = state.loss - trial_state.loss;
if improvement >= min_efficiency * rate * base_target_improvement {
return Some((trial_state, backoff_steps));
}
rate *= backoff;
}
None
}
// seek a matrix `config` for which `config' * Q * config` matches the partial
// matrix `gram`. use gradient descent starting from `guess`
pub fn realize_gram(
gram: &PartialMatrix,
guess: DMatrix<f64>,
frozen: &[(usize, usize)],
scaled_tol: f64,
min_efficiency: f64,
backoff: f64,
reg_scale: f64,
max_descent_steps: i32,
max_backoff_steps: i32
) -> (DMatrix<f64>, ConfigSubspace, bool, DescentHistory) {
// start the descent history
let mut history = DescentHistory::new();
// find the dimension of the search space
let element_dim = guess.nrows();
let assembly_dim = guess.ncols();
let total_dim = element_dim * assembly_dim;
// scale the tolerance
let scale_adjustment = (gram.0.len() as f64).sqrt();
let tol = scale_adjustment * scaled_tol;
// convert the frozen indices to stacked format
let frozen_stacked: Vec<usize> = frozen.into_iter().map(
|index| index.1*element_dim + index.0
).collect();
// use Newton's method with backtracking and gradient descent backup
let mut state = SearchState::from_config(gram, guess);
let mut hess = DMatrix::zeros(element_dim, assembly_dim);
for _ in 0..max_descent_steps {
// find the negative gradient of the loss function
let neg_grad = 4.0 * &*Q * &state.config * &state.err_proj;
let mut neg_grad_stacked = neg_grad.clone().reshape_generic(Dyn(total_dim), Const::<1>);
history.neg_grad.push(neg_grad.clone());
// find the negative Hessian of the loss function
let mut hess_cols = Vec::<DVector<f64>>::with_capacity(total_dim);
for col in 0..assembly_dim {
for row in 0..element_dim {
let index = (row, col);
let basis_mat = basis_matrix(index, element_dim, assembly_dim);
let neg_d_err =
basis_mat.tr_mul(&*Q) * &state.config
+ state.config.tr_mul(&*Q) * &basis_mat;
let neg_d_err_proj = gram.proj(&neg_d_err);
let deriv_grad = 4.0 * &*Q * (
-&basis_mat * &state.err_proj
+ &state.config * &neg_d_err_proj
);
hess_cols.push(deriv_grad.reshape_generic(Dyn(total_dim), Const::<1>));
}
}
hess = DMatrix::from_columns(hess_cols.as_slice());
// regularize the Hessian
let min_eigval = hess.symmetric_eigenvalues().min();
if min_eigval <= 0.0 {
hess -= reg_scale * min_eigval * DMatrix::identity(total_dim, total_dim);
}
history.min_eigval.push(min_eigval);
// project the negative gradient and negative Hessian onto the
// orthogonal complement of the frozen subspace
let zero_col = DVector::zeros(total_dim);
let zero_row = zero_col.transpose();
for &k in &frozen_stacked {
neg_grad_stacked[k] = 0.0;
hess.set_row(k, &zero_row);
hess.set_column(k, &zero_col);
hess[(k, k)] = 1.0;
}
// stop if the loss is tolerably low
history.config.push(state.config.clone());
history.scaled_loss.push(state.loss / scale_adjustment);
if state.loss < tol { break; }
// compute the Newton step
/*
we need to either handle or eliminate the case where the minimum
eigenvalue of the Hessian is zero, so the regularized Hessian is
singular. right now, this causes the Cholesky decomposition to return
`None`, leading to a panic when we unrap
*/
let base_step_stacked = hess.clone().cholesky().unwrap().solve(&neg_grad_stacked);
let base_step = base_step_stacked.reshape_generic(Dyn(element_dim), Dyn(assembly_dim));
history.base_step.push(base_step.clone());
// use backtracking line search to find a better configuration
match seek_better_config(
gram, &state, &base_step, neg_grad.dot(&base_step),
min_efficiency, backoff, max_backoff_steps
) {
Some((better_state, backoff_steps)) => {
state = better_state;
history.backoff_steps.push(backoff_steps);
},
None => return (state.config, ConfigSubspace::zero(assembly_dim), false, history)
};
}
let success = state.loss < tol;
let tangent = if success {
// express the uniform basis in the standard basis
let mut unif_to_std = DMatrix::<f64>::zeros(total_dim, total_dim);
for n in 0..assembly_dim {
let block_start = element_dim * n;
unif_to_std
.view_mut((block_start, block_start), (element_dim, element_dim))
.copy_from(&local_unif_to_std(state.config.column(n)));
}
// find the kernel of the Hessian. give it the uniform inner product
ConfigSubspace::symmetric_kernel(hess, unif_to_std, assembly_dim)
} else {
ConfigSubspace::zero(assembly_dim)
};
(state.config, tangent, success, history)
}
// --- tests ---
// this problem is from a sangaku by Irisawa Shintarō Hiroatsu. the article
// below includes a nice translation of the problem statement, which was
// recorded in Uchida Itsumi's book _Kokon sankan_ (_Mathematics, Past and
// Present_)
//
// "Japan's 'Wasan' Mathematical Tradition", by Abe Haruki
// https://www.nippon.com/en/japan-topics/c12801/
//
#[cfg(feature = "dev")]
pub mod irisawa {
use std::{array, f64::consts::PI};
use super::*;
pub fn realize_irisawa_hexlet(scaled_tol: f64) -> (DMatrix<f64>, ConfigSubspace, bool, DescentHistory) {
let gram = {
let mut gram_to_be = PartialMatrix::new();
for s in 0..9 {
// each sphere is represented by a spacelike vector
gram_to_be.push_sym(s, s, 1.0);
// the circumscribing sphere is tangent to all of the other
// spheres, with matching orientation
if s > 0 {
gram_to_be.push_sym(0, s, 1.0);
}
if s > 2 {
// each chain sphere is tangent to the "sun" and "moon"
// spheres, with opposing orientation
for n in 1..3 {
gram_to_be.push_sym(s, n, -1.0);
}
// each chain sphere is tangent to the next chain sphere,
// with opposing orientation
let s_next = 3 + (s-2) % 6;
gram_to_be.push_sym(s, s_next, -1.0);
}
}
gram_to_be
};
let guess = DMatrix::from_columns(
[
sphere(0.0, 0.0, 0.0, 15.0),
sphere(0.0, 0.0, -9.0, 5.0),
sphere(0.0, 0.0, 11.0, 3.0)
].into_iter().chain(
(1..=6).map(
|k| {
let ang = (k as f64) * PI/3.0;
sphere(9.0 * ang.cos(), 9.0 * ang.sin(), 0.0, 2.5)
}
)
).collect::<Vec<_>>().as_slice()
);
// the frozen entries fix the radii of the circumscribing sphere, the
// "sun" and "moon" spheres, and one of the chain spheres
let frozen: [(usize, usize); 4] = array::from_fn(|k| (3, k));
realize_gram(
&gram, guess, &frozen,
scaled_tol, 0.5, 0.9, 1.1, 200, 110
)
}
}
#[cfg(test)]
mod tests {
use super::{*, irisawa::realize_irisawa_hexlet};
#[test]
fn sub_proj_test() {
let target = PartialMatrix(vec![
MatrixEntry { index: (0, 0), value: 19.0 },
MatrixEntry { index: (0, 2), value: 39.0 },
MatrixEntry { index: (1, 1), value: 59.0 },
MatrixEntry { index: (1, 2), value: 69.0 }
]);
let attempt = DMatrix::<f64>::from_row_slice(2, 3, &[
1.0, 2.0, 3.0,
4.0, 5.0, 6.0
]);
let expected_result = DMatrix::<f64>::from_row_slice(2, 3, &[
18.0, 0.0, 36.0,
0.0, 54.0, 63.0
]);
assert_eq!(target.sub_proj(&attempt), expected_result);
}
#[test]
fn zero_loss_test() {
let gram = PartialMatrix({
let mut entries = Vec::<MatrixEntry>::new();
for j in 0..3 {
for k in 0..3 {
entries.push(MatrixEntry {
index: (j, k),
value: if j == k { 1.0 } else { -1.0 }
});
}
}
entries
});
let config = {
let a: f64 = 0.75_f64.sqrt();
DMatrix::from_columns(&[
sphere(1.0, 0.0, 0.0, a),
sphere(-0.5, a, 0.0, a),
sphere(-0.5, -a, 0.0, a)
])
};
let state = SearchState::from_config(&gram, config);
assert!(state.loss.abs() < f64::EPSILON);
}
#[test]
fn irisawa_hexlet_test() {
// solve Irisawa's problem
const SCALED_TOL: f64 = 1.0e-12;
let (config, _, _, _) = realize_irisawa_hexlet(SCALED_TOL);
// check against Irisawa's solution
let entry_tol = SCALED_TOL.sqrt();
let solution_diams = [30.0, 10.0, 6.0, 5.0, 15.0, 10.0, 3.75, 2.5, 2.0 + 8.0/11.0];
for (k, diam) in solution_diams.into_iter().enumerate() {
assert!((config[(3, k)] - 1.0 / diam).abs() < entry_tol);
}
}
#[test]
fn tangent_test() {
const SCALED_TOL: f64 = 1.0e-12;
const ELEMENT_DIM: usize = 5;
const ASSEMBLY_DIM: usize = 3;
let gram = {
let mut gram_to_be = PartialMatrix::new();
for j in 0..3 {
for k in j..3 {
gram_to_be.push_sym(j, k, if j == k { 1.0 } else { -1.0 });
}
}
gram_to_be
};
let guess = DMatrix::from_columns(&[
sphere(0.0, 0.0, 0.0, -2.0),
sphere(0.0, 0.0, 1.0, 1.0),
sphere(0.0, 0.0, -1.0, 1.0)
]);
let frozen: [_; 5] = std::array::from_fn(|k| (k, 0));
let (config, tangent, success, history) = realize_gram(
&gram, guess.clone(), &frozen,
SCALED_TOL, 0.5, 0.9, 1.1, 200, 110
);
assert_eq!(config, guess);
assert_eq!(success, true);
assert_eq!(history.scaled_loss.len(), 1);
// confirm that the tangent space has dimension five or less
let ConfigSubspace(ref tangent_basis) = tangent;
assert_eq!(tangent_basis.len(), 5);
// confirm that the tangent space contains all the motions we expect it
// to. since we've already bounded the dimension of the tangent space,
// this confirms that the tangent space is what we expect it to be
let tangent_motions = vec![
basis_matrix((0, 1), ELEMENT_DIM, ASSEMBLY_DIM),
basis_matrix((1, 1), ELEMENT_DIM, ASSEMBLY_DIM),
basis_matrix((0, 2), ELEMENT_DIM, ASSEMBLY_DIM),
basis_matrix((1, 2), ELEMENT_DIM, ASSEMBLY_DIM),
DMatrix::<f64>::from_column_slice(ELEMENT_DIM, 3, &[
0.0, 0.0, 0.0, 0.0, 0.0,
0.0, 0.0, -1.0, -0.25, -1.0,
0.0, 0.0, -1.0, 0.25, 1.0
])
];
let tol_sq = ((ELEMENT_DIM * ASSEMBLY_DIM) as f64) * SCALED_TOL * SCALED_TOL;
for motion in tangent_motions {
let motion_proj: DMatrix<_> = motion.column_iter().enumerate().map(
|(k, v)| tangent.proj(&v, k)
).sum();
assert!((motion - motion_proj).norm_squared() < tol_sq);
}
}
// at the frozen indices, the optimization steps should have exact zeros,
// and the realized configuration should match the initial guess
#[test]
fn frozen_entry_test() {
let gram = {
let mut gram_to_be = PartialMatrix::new();
for j in 0..2 {
for k in j..2 {
gram_to_be.push_sym(j, k, if (j, k) == (1, 1) { 1.0 } else { 0.0 });
}
}
gram_to_be
};
let guess = DMatrix::from_columns(&[
point(0.0, 0.0, 2.0),
sphere(0.0, 0.0, 0.0, 1.0)
]);
let frozen = [(3, 0), (3, 1)];
println!();
let (config, _, success, history) = realize_gram(
&gram, guess.clone(), &frozen,
1.0e-12, 0.5, 0.9, 1.1, 200, 110
);
assert_eq!(success, true);
for base_step in history.base_step.into_iter() {
for index in frozen {
assert_eq!(base_step[index], 0.0);
}
}
for index in frozen {
assert_eq!(config[index], guess[index]);
}
}
}