CCD: take angular motion and penetration depth into account in various thresholds.
This commit is contained in:
@@ -113,6 +113,7 @@ pub struct RigidBody {
|
||||
/// User-defined data associated to this rigid-body.
|
||||
pub user_data: u128,
|
||||
pub(crate) ccd_thickness: Real,
|
||||
pub(crate) ccd_max_dist: Real,
|
||||
}
|
||||
|
||||
impl RigidBody {
|
||||
@@ -146,6 +147,7 @@ impl RigidBody {
|
||||
dominance_group: 0,
|
||||
user_data: 0,
|
||||
ccd_thickness: Real::MAX,
|
||||
ccd_max_dist: 0.0,
|
||||
}
|
||||
}
|
||||
|
||||
@@ -172,8 +174,6 @@ impl RigidBody {
|
||||
|
||||
self.linvel += linear_acc * dt;
|
||||
self.angvel += angular_acc * dt;
|
||||
self.force = na::zero();
|
||||
self.torque = na::zero();
|
||||
}
|
||||
|
||||
/// The mass properties of this rigid-body.
|
||||
@@ -208,17 +208,56 @@ impl RigidBody {
|
||||
// This is different from `is_ccd_enabled`. This checks that CCD
|
||||
// is active for this rigid-body, i.e., if it was seen to move fast
|
||||
// enough to justify a CCD run.
|
||||
pub(crate) fn is_ccd_active(&self) -> bool {
|
||||
/// Is CCD active for this rigid-body?
|
||||
///
|
||||
/// The CCD is considered active if the rigid-body is moving at
|
||||
/// a velocity greater than an automatically-computed threshold.
|
||||
///
|
||||
/// This is not the same as `self.is_ccd_enabled` which only
|
||||
/// checks if CCD is allowed to run for this rigid-body or if
|
||||
/// it is completely disabled (independently from its velocity).
|
||||
pub fn is_ccd_active(&self) -> bool {
|
||||
self.flags.contains(RigidBodyFlags::CCD_ACTIVE)
|
||||
}
|
||||
|
||||
pub(crate) fn update_ccd_active_flag(&mut self, dt: Real) {
|
||||
let ccd_active = self.is_ccd_enabled() && self.is_moving_fast(dt);
|
||||
pub(crate) fn update_ccd_active_flag(&mut self, dt: Real, include_forces: bool) {
|
||||
let ccd_active = self.is_ccd_enabled() && self.is_moving_fast(dt, include_forces);
|
||||
self.flags.set(RigidBodyFlags::CCD_ACTIVE, ccd_active);
|
||||
}
|
||||
|
||||
pub(crate) fn is_moving_fast(&self, dt: Real) -> bool {
|
||||
self.is_dynamic() && self.linvel.norm() * dt > self.ccd_thickness
|
||||
pub(crate) fn is_moving_fast(&self, dt: Real, include_forces: bool) -> bool {
|
||||
if self.is_dynamic() {
|
||||
// NOTE: for the threshold we don't use the exact CCD thickness. Theoretically, we
|
||||
// should use `self.ccd_thickness - smallest_contact_dist` where `smallest_contact_dist`
|
||||
// is the deepest contact (the contact with the largest penetration depth, i.e., the
|
||||
// negative `dist` with the largest absolute value.
|
||||
// However, getting this penetration depth assumes querying the contact graph from
|
||||
// the narrow-phase, which can be pretty expensive. So we use the CCD thickness
|
||||
// divided by 10 right now. We will see in practice if this value is OK or if we
|
||||
// should use a smaller (to be less conservative) or larger divisor (to be more conservative).
|
||||
let threshold = self.ccd_thickness / 10.0;
|
||||
|
||||
if include_forces {
|
||||
let linear_part = (self.linvel + self.force * dt).norm();
|
||||
#[cfg(feature = "dim2")]
|
||||
let angular_part = (self.angvel + self.torque * dt).abs() * self.ccd_max_dist;
|
||||
#[cfg(feature = "dim3")]
|
||||
let angular_part = (self.angvel + self.torque * dt).norm() * self.ccd_max_dist;
|
||||
let vel_with_forces = linear_part + angular_part;
|
||||
vel_with_forces > threshold
|
||||
} else {
|
||||
self.max_point_velocity() * dt > threshold
|
||||
}
|
||||
} else {
|
||||
false
|
||||
}
|
||||
}
|
||||
|
||||
pub(crate) fn max_point_velocity(&self) -> Real {
|
||||
#[cfg(feature = "dim2")]
|
||||
return self.linvel.norm() + self.angvel.abs() * self.ccd_max_dist;
|
||||
#[cfg(feature = "dim3")]
|
||||
return self.linvel.norm() + self.angvel.norm() * self.ccd_max_dist;
|
||||
}
|
||||
|
||||
/// Sets the rigid-body's mass properties.
|
||||
@@ -301,6 +340,13 @@ impl RigidBody {
|
||||
|
||||
self.ccd_thickness = self.ccd_thickness.min(coll.shape().ccd_thickness());
|
||||
|
||||
let shape_bsphere = coll
|
||||
.shape()
|
||||
.compute_bounding_sphere(coll.position_wrt_parent());
|
||||
self.ccd_max_dist = self
|
||||
.ccd_max_dist
|
||||
.max(shape_bsphere.center.coords.norm() + shape_bsphere.radius);
|
||||
|
||||
let mass_properties = coll
|
||||
.mass_properties()
|
||||
.transform_by(coll.position_wrt_parent());
|
||||
@@ -311,7 +357,7 @@ impl RigidBody {
|
||||
|
||||
pub(crate) fn update_colliders_positions(&mut self, colliders: &mut ColliderSet) {
|
||||
for handle in &self.colliders {
|
||||
// NOTE: we don't use `get_mut_internal` here because we want to
|
||||
// NOTE: we use `get_mut_internal_with_modification_tracking` here because we want to
|
||||
// benefit from the modification tracking to know the colliders
|
||||
// we need to update the broad-phase and narrow-phase for.
|
||||
let collider = colliders
|
||||
@@ -382,7 +428,9 @@ impl RigidBody {
|
||||
!self.linvel.is_zero() || !self.angvel.is_zero()
|
||||
}
|
||||
|
||||
pub(crate) fn predict_position_using_velocity_and_forces(&self, dt: Real) -> Isometry<Real> {
|
||||
/// Computes the predict position of this rigid-body after `dt` seconds, taking
|
||||
/// into account its velocities and external forces applied to it.
|
||||
pub fn predict_position_using_velocity_and_forces(&self, dt: Real) -> Isometry<Real> {
|
||||
let dlinvel = self.force * (self.effective_inv_mass * dt);
|
||||
let dangvel = self
|
||||
.effective_world_inv_inertia_sqrt
|
||||
|
||||
Reference in New Issue
Block a user