Added stabilisation for constraints
Note: necessary for arbitrary DAE systems
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6b422ec286
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8bdb557b93
8 changed files with 173 additions and 24 deletions
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@ -536,35 +536,52 @@ void Foam::geometricSixDOF::update(const scalar delta)
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{
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// Translation
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// Update displacement
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// Get displacement
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const vector Xold = Xrel_.value();
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vector& Xval = Xrel_.value();
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Xval.x() = coeffs_[0];
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Xval.y() = coeffs_[1];
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Xval.z() = coeffs_[2];
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// Update velocity
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Uaverage_.value() = (Xval - Xold)/delta;
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// Get velocity
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vector& Uval = U_.value();
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Uval.x() = coeffs_[3];
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Uval.y() = coeffs_[4];
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Uval.z() = coeffs_[5];
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// Stabilise translational constraints if necessary
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forAll(translationalConstraints(), tcI)
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{
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// Note: get end time for this ODE step from mesh, assuming that the top
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// level solves this ode from [t - deltaT, t], yielding solution at
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// t. Done this way to preserve the interface of ODE class.
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// VV, 10/Mar/2017.
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const scalar t = dict().time().value();
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translationalConstraints()[tcI].stabilise(t, Xval, Uval);
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}
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// Update (possibly constrained) displacement
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coeffs_[0] = Xval.x();
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coeffs_[1] = Xval.y();
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coeffs_[2] = Xval.z();
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// Update (possibly constrained) velocity
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coeffs_[3] = Uval.x();
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coeffs_[4] = Uval.y();
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coeffs_[5] = Uval.z();
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// Update average velocity
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Uaverage_.value() = (Xval - Xold)/delta;
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// Rotation
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// Update omega
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// Get angular velocity
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const vector omegaOld = omega_.value();
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vector& omegaVal = omega_.value();
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omegaVal.x() = coeffs_[6];
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omegaVal.y() = coeffs_[7];
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omegaVal.z() = coeffs_[8];
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@ -575,11 +592,29 @@ void Foam::geometricSixDOF::update(const scalar delta)
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// Update rotational tensor
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rotation_ = (rotation_ & rotIncrement_);
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// Stabilise rotational constraints if necessary
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forAll(rotationalConstraints(), rcI)
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{
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// Note: get end time for this ODE step from mesh, assuming that the top
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// level solves this ode from [t - deltaT, t], yielding solution at
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// t. Done this way to preserve the interface of ODE class.
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// VV, 10/Mar/2017.
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const scalar t = dict().time().value();
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rotationalConstraints()[rcI].stabilise(t, omegaVal);
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}
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// Update (possibly constrained) omega
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coeffs_[6] = omegaVal.x();
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coeffs_[7] = omegaVal.y();
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coeffs_[8] = omegaVal.z();
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// Reset increment vector in coefficients for the next step
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coeffs_[9] = 0;
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coeffs_[10] = 0;
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coeffs_[11] = 0;
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// Update average omega
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omegaAverage_.value() = 0.5*(omegaVal + omegaOld);
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}
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@ -447,40 +447,54 @@ void Foam::quaternionSixDOF::update(const scalar delta)
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{
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// Translation
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// Update displacement
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vector Xold = Xrel_.value();
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// Get displacement
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const vector Xold = Xrel_.value();
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vector& Xval = Xrel_.value();
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Xval.x() = coeffs_[0];
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Xval.y() = coeffs_[1];
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Xval.z() = coeffs_[2];
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// Update velocity
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Uaverage_.value() = (Xval - Xold)/delta;
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// Get velocity
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vector& Uval = U_.value();
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Uval.x() = coeffs_[3];
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Uval.y() = coeffs_[4];
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Uval.z() = coeffs_[5];
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// Stabilise translational constraints if necessary
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forAll(translationalConstraints(), tcI)
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{
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// Note: get end time for this ODE step from mesh, assuming that the top
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// level solves this ode from [t - deltaT, t], yielding solution at
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// t. Done this way to preserve the interface of ODE class.
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// VV, 10/Mar/2017.
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const scalar t = dict().time().value();
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translationalConstraints()[tcI].stabilise(t, Xval, Uval);
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}
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// Update (possibly constrained) displacement
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coeffs_[0] = Xval.x();
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coeffs_[1] = Xval.y();
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coeffs_[2] = Xval.z();
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// Update (possibly constrained) velocity
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coeffs_[3] = Uval.x();
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coeffs_[4] = Uval.y();
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coeffs_[5] = Uval.z();
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// Update average velocity
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Uaverage_.value() = (Xval - Xold)/delta;
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// Rotation
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// Update omega
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// Get angular velocity
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vector& omegaVal = omega_.value();
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omegaVal.x() = coeffs_[6];
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omegaVal.y() = coeffs_[7];
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omegaVal.z() = coeffs_[8];
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coeffs_[6] = omegaVal.x();
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coeffs_[7] = omegaVal.y();
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coeffs_[8] = omegaVal.z();
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rotation_.updateRotation
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(
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@ -493,6 +507,24 @@ void Foam::quaternionSixDOF::update(const scalar delta)
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)
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);
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// Stabilise rotational constraints if necessary
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forAll(rotationalConstraints(), rcI)
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{
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// Note: get end time for this ODE step from mesh, assuming that the top
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// level solves this ode from [t - deltaT, t], yielding solution at
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// t. Done this way to preserve the interface of ODE class.
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// VV, 10/Mar/2017.
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const scalar t = dict().time().value();
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rotationalConstraints()[rcI].stabilise(t, omegaVal);
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}
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// Update (possibly constrained) omega
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coeffs_[6] = omegaVal.x();
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coeffs_[7] = omegaVal.y();
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coeffs_[8] = omegaVal.z();
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// Update average omega
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omegaAverage_.value() = rotation_.omegaAverage(delta);
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}
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@ -113,6 +113,16 @@ public:
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const vector&
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) const;
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//- Stabilise the constraint
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virtual void stabilise
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(
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const scalar,
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vector&
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) const
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{
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// Does nothing: no need to stabilise this constraint
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}
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// I-O Functions
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@ -41,8 +41,12 @@ Description
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2. sourceContribution() - corresponding to a(t), to be inserted into right
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hand side vector.
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Note: constraints are usually used alongside appropriate initial
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conditions (rotational rate in a given direction).
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Notes:
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1. Constraints are usually used alongside appropriate initial
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conditions (rotational rate in a given direction),
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2. According to DAE theory, a stabilisation on orientation/angular velocity
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is necessary based on "differentiation index" used to obtain the final
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form of the constraint.
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Author
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Viktor Pandza, FSB Zagreb. All rights reserved.
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@ -167,6 +171,14 @@ public:
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const vector& omega
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) const = 0;
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//- Stabilise the constraint (necessary for constraints with
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// differentiation index higher than zero)
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virtual void stabilise
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(
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const scalar t,
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vector& omega
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) const = 0;
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// I-O Functions and Operators
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@ -111,6 +111,16 @@ public:
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const vector&
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) const;
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//- Stabilise the constraint
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virtual void stabilise
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(
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const scalar,
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vector&,
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vector&
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) const
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{
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// Does nothing: no need to stabilise this constraint
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};
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// I-O Functions
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@ -117,6 +117,32 @@ Foam::scalar Foam::periodicOscillation::sourceContribution
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}
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void Foam::periodicOscillation::stabilise
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(
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const scalar t,
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vector& x,
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vector& u
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) const
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{
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// Set the displacement according to periodic oscillation
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// First subtract calculated displacement...
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x -= (x & dir_)*dir_;
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// ... then add the correct displacement
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x += dir_*sin(omega_*t + phi_);
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// Set the velocity according to periodic oscillation
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// First subract calculated velocity...
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u -= (u & dir_)*dir_;
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// ... then add the correct velocity
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u += dir_*cos(omega_*t + phi_);
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}
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void Foam::periodicOscillation::write(Ostream& os) const
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{
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os.writeKeyword("type") << tab << type()
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@ -32,6 +32,10 @@ Description
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where a is the amplitude of oscillation, omega radial frequency and phi is
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the phase shift.
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Note: since this constraint is basically algebraic (dependent on
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displacement), the differentiation index is two so the stabilisation on
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displacement and velocity is necessary.
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Author
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Viktor Pandza, FSB Zagreb. All rights reserved.
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Vuko Vukcevic, FSB Zagreb. All rights reserved.
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@ -124,6 +128,13 @@ public:
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const vector&
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) const;
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//- Stabilise the constraint
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virtual void stabilise
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(
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const scalar t,
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vector& x,
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vector& u
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) const;
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// I-O Functions
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@ -41,8 +41,12 @@ Description
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2. sourceContribution() - corresponding to a(t), to be inserted into right
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hand side vector.
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Note: constraints are usually used alongside appropriate initial
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conditions (velocity in a given direction).
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Notes:
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1. Constraints are usually used alongside appropriate initial
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conditions (velocity in a given direction),
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2. According to DAE theory, a stabilisation on displacement/velocity is
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necessary based on "differentiation index" used to obtain the final form
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of the constraint.
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Author
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Viktor Pandza, FSB Zagreb. All rights reserved.
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@ -169,6 +173,15 @@ public:
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const vector& u
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) const = 0;
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//- Stabilise the constraint (necessary for constraints with
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// differentiation index higher than zero)
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virtual void stabilise
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(
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const scalar t,
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vector& x,
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vector& u
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) const = 0;
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// I-O Functions and Operators
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