feat: add exact mlcp solver for pais of 2 constraints

This commit is contained in:
Sébastien Crozet
2024-04-14 15:53:35 +02:00
committed by Sébastien Crozet
parent 15c07cfeb3
commit 3ddf2441ea
11 changed files with 460 additions and 22 deletions

View File

@@ -1,6 +1,13 @@
use crate::dynamics::integration_parameters::{
BLOCK_SOLVER_ENABLED, DISABLE_FRICTION_LIMIT_REAPPLY,
};
use crate::dynamics::solver::contact_constraint::OneBodyConstraintNormalPart;
use crate::dynamics::solver::SolverVel;
use crate::math::{AngVector, Vector, DIM};
use crate::utils::{SimdBasis, SimdDot, SimdRealCopy};
use na::{Matrix2, Vector2};
use num::Zero;
use simba::simd::{SimdPartialOrd, SimdValue};
#[derive(Copy, Clone, Debug)]
pub(crate) struct TwoBodyConstraintTangentPart<N: SimdRealCopy> {
@@ -64,6 +71,10 @@ impl<N: SimdRealCopy> TwoBodyConstraintTangentPart<N> {
) where
AngVector<N>: SimdDot<AngVector<N>, Result = N>,
{
if DISABLE_FRICTION_LIMIT_REAPPLY {
return;
}
#[cfg(feature = "dim2")]
{
let new_impulse = self.impulse[0].simd_clamp(-limit, limit);
@@ -182,6 +193,11 @@ pub(crate) struct TwoBodyConstraintNormalPart<N: SimdRealCopy> {
pub impulse: N,
pub impulse_accumulator: N,
pub r: N,
// For coupled constraint pairs, even constraints store the
// diagonal of the projected mass matrix. Odd constraints
// store the off-diagonal element of the projected mass matrix,
// as well as the off-diagonal element of the inverse projected mass matrix.
pub r_mat_elts: [N; 2],
}
impl<N: SimdRealCopy> TwoBodyConstraintNormalPart<N> {
@@ -194,6 +210,7 @@ impl<N: SimdRealCopy> TwoBodyConstraintNormalPart<N> {
impulse: na::zero(),
impulse_accumulator: na::zero(),
r: na::zero(),
r_mat_elts: [N::zero(); 2],
}
}
@@ -229,6 +246,83 @@ impl<N: SimdRealCopy> TwoBodyConstraintNormalPart<N> {
solver_vel2.linear += dir1.component_mul(im2) * -dlambda;
solver_vel2.angular += self.gcross2 * dlambda;
}
#[inline(always)]
pub(crate) fn solve_mlcp_two_constraints(
dvel: Vector2<N>,
prev_impulse: Vector2<N>,
r_a: N,
r_b: N,
[r_mat11, r_mat22]: [N; 2],
[r_mat12, r_mat_inv12]: [N; 2],
cfm_factor: N,
) -> Vector2<N> {
let r_dvel = Vector2::new(
r_mat11 * dvel.x + r_mat12 * dvel.y,
r_mat12 * dvel.x + r_mat22 * dvel.y,
);
let new_impulse0 = prev_impulse - r_dvel;
let new_impulse1 = Vector2::new(prev_impulse.x - r_a * dvel.x, N::zero());
let new_impulse2 = Vector2::new(N::zero(), prev_impulse.y - r_b * dvel.y);
let new_impulse3 = Vector2::new(N::zero(), N::zero());
let keep0 = new_impulse0.x.simd_ge(N::zero()) & new_impulse0.y.simd_ge(N::zero());
let keep1 = new_impulse1.x.simd_ge(N::zero())
& (dvel.y + r_mat_inv12 * new_impulse1.x).simd_ge(N::zero());
let keep2 = new_impulse2.y.simd_ge(N::zero())
& (dvel.x + r_mat_inv12 * new_impulse2.y).simd_ge(N::zero());
let keep3 = dvel.x.simd_ge(N::zero()) & dvel.y.simd_ge(N::zero());
let selected3 = (new_impulse3 * cfm_factor).select(keep3, prev_impulse);
let selected2 = (new_impulse2 * cfm_factor).select(keep2, selected3);
let selected1 = (new_impulse1 * cfm_factor).select(keep1, selected2);
(new_impulse0 * cfm_factor).select(keep0, selected1)
}
#[inline]
pub fn solve_pair(
constraint_a: &mut Self,
constraint_b: &mut Self,
cfm_factor: N,
dir1: &Vector<N>,
im1: &Vector<N>,
im2: &Vector<N>,
solver_vel1: &mut SolverVel<N>,
solver_vel2: &mut SolverVel<N>,
) where
AngVector<N>: SimdDot<AngVector<N>, Result = N>,
{
let dvel_lin = dir1.dot(&solver_vel1.linear) - dir1.dot(&solver_vel2.linear);
let dvel_a = dvel_lin
+ constraint_a.gcross1.gdot(solver_vel1.angular)
+ constraint_a.gcross2.gdot(solver_vel2.angular)
+ constraint_a.rhs;
let dvel_b = dvel_lin
+ constraint_b.gcross1.gdot(solver_vel1.angular)
+ constraint_b.gcross2.gdot(solver_vel2.angular)
+ constraint_b.rhs;
let prev_impulse = Vector2::new(constraint_a.impulse, constraint_b.impulse);
let new_impulse = Self::solve_mlcp_two_constraints(
Vector2::new(dvel_a, dvel_b),
prev_impulse,
constraint_a.r,
constraint_b.r,
constraint_a.r_mat_elts,
constraint_b.r_mat_elts,
cfm_factor,
);
let dlambda = new_impulse - prev_impulse;
constraint_a.impulse = new_impulse.x;
constraint_b.impulse = new_impulse.y;
solver_vel1.linear += dir1.component_mul(im1) * (dlambda.x + dlambda.y);
solver_vel1.angular += constraint_a.gcross1 * dlambda.x + constraint_b.gcross1 * dlambda.y;
solver_vel2.linear += dir1.component_mul(im2) * (-dlambda.x - dlambda.y);
solver_vel2.angular += constraint_a.gcross2 * dlambda.x + constraint_b.gcross2 * dlambda.y;
}
}
#[derive(Copy, Clone, Debug)]
@@ -269,13 +363,49 @@ impl<N: SimdRealCopy> TwoBodyConstraintElement<N> {
// Solve penetration.
if solve_normal {
for element in elements.iter_mut() {
element
.normal_part
.solve(cfm_factor, dir1, im1, im2, solver_vel1, solver_vel2);
let limit = limit * element.normal_part.impulse;
let part = &mut element.tangent_part;
part.apply_limit(tangents1, im1, im2, limit, solver_vel1, solver_vel2);
if BLOCK_SOLVER_ENABLED {
for elements in elements.chunks_exact_mut(2) {
let [element_a, element_b] = elements else {
unreachable!()
};
TwoBodyConstraintNormalPart::solve_pair(
&mut element_a.normal_part,
&mut element_b.normal_part,
cfm_factor,
dir1,
im1,
im2,
solver_vel1,
solver_vel2,
);
for i in 0..2 {
let limit = limit * elements[i].normal_part.impulse;
let part = &mut elements[i].tangent_part;
part.apply_limit(tangents1, im1, im2, limit, solver_vel1, solver_vel2);
}
}
// There is one constraint left to solve if there isnt an even number.
if elements.len() % 2 == 1 {
let element = elements.last_mut().unwrap();
element
.normal_part
.solve(cfm_factor, dir1, im1, im2, solver_vel1, solver_vel2);
let limit = limit * element.normal_part.impulse;
let part = &mut element.tangent_part;
part.apply_limit(tangents1, im1, im2, limit, solver_vel1, solver_vel2);
}
} else {
for element in elements.iter_mut() {
element
.normal_part
.solve(cfm_factor, dir1, im1, im2, solver_vel1, solver_vel2);
let limit = limit * element.normal_part.impulse;
let part = &mut element.tangent_part;
part.apply_limit(tangents1, im1, im2, limit, solver_vel1, solver_vel2);
}
}
}