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geant4/source/geometry/magneticfield/src/G4BogackiShampine23.cc
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//
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//
// G4BogackiShampine23 implementation
//
// Bogacki-Shampine - 4 - 3(2) non-FSAL implementation
//
// Implementation of the method proposed in the publication
// "A 3(2) pair of Runge - Kutta formulas"
// by P. Bogacki and L. F. Shampine,
// Appl. Math. Lett., vol. 2, no. 4, pp. 321-325, Jan. 1989.
//
// The Bogacki shampine method has the following Butcher's tableau
//
// 0 |
// 1/2|1/2
// 3/4|0 3/4
// 1 |2/9 1/3 4/9
// -------------------
// |2/9 1/3 4/9 0
// |7/24 1/4 1/3 1/8
//
// Created: Somnath Banerjee, Google Summer of Code 2015, 20 May 2015
// Supervision: John Apostolakis, CERN
// --------------------------------------------------------------------
#include "G4BogackiShampine23.hh"
#include "G4LineSection.hh"
#include "G4FieldUtils.hh"
using namespace field_utils;
G4BogackiShampine23::G4BogackiShampine23(G4EquationOfMotion* EqRhs,
G4int integrationVariables)
: G4MagIntegratorStepper(EqRhs, integrationVariables)
{
SetIntegrationOrder(3);
SetFSAL(true);
}
void G4BogackiShampine23::makeStep(const G4double yInput[],
const G4double dydx[],
const G4double hstep,
G4double yOutput[],
G4double* dydxOutput,
G4double* yError) const
{
G4double yTemp[G4FieldTrack::ncompSVEC];
for(G4int i = GetNumberOfVariables(); i < GetNumberOfStateVariables(); ++i)
{
yOutput[i] = yTemp[i] = yInput[i];
}
G4double ak2[G4FieldTrack::ncompSVEC],
ak3[G4FieldTrack::ncompSVEC];
const G4double b21 = 0.5 ,
b31 = 0., b32 = 3.0 / 4.0,
b41 = 2.0 / 9.0, b42 = 1.0 / 3.0, b43 = 4.0 / 9.0;
const G4double dc1 = b41 - 7.0 / 24.0, dc2 = b42 - 1.0 / 4.0,
dc3 = b43 - 1.0 / 3.0, dc4 = - 1.0 / 8.0;
// RightHandSide(yInput, dydx);
for(G4int i = 0; i < GetNumberOfVariables(); ++i)
{
yTemp[i] = yInput[i] + b21 * hstep * dydx[i];
}
RightHandSide(yTemp, ak2);
for(G4int i = 0; i < GetNumberOfVariables(); ++i)
{
yTemp[i] = yInput[i] + hstep * (b31 * dydx[i] + b32 * ak2[i]);
}
RightHandSide(yTemp, ak3);
for(G4int i = 0; i < GetNumberOfVariables(); ++i)
{
yOutput[i] = yInput[i] + hstep * (b41*dydx[i] + b42*ak2[i] + b43*ak3[i]);
}
if ((dydxOutput != nullptr) && (yError != nullptr))
{
RightHandSide(yOutput, dydxOutput);
for(G4int i = 0; i < GetNumberOfVariables(); ++i)
{
yError[i] = hstep * (dc1 * dydx[i] + dc2 * ak2[i] +
dc3 * ak3[i] + dc4 * dydxOutput[i]);
}
}
}
void G4BogackiShampine23::Stepper(const G4double yInput[],
const G4double dydx[],
G4double hstep,
G4double yOutput[],
G4double yError[])
{
copy(fyIn, yInput);
copy(fdydx, dydx);
fhstep = hstep;
makeStep(fyIn, fdydx, fhstep, fyOut, fdydxOut, yError);
copy(yOutput, fyOut);
}
void G4BogackiShampine23::Stepper(const G4double yInput[],
const G4double dydx[],
G4double hstep,
G4double yOutput[],
G4double yError[],
G4double dydxOutput[])
{
copy(fyIn, yInput);
copy(fdydx, dydx);
fhstep = hstep;
makeStep(fyIn, fdydx, fhstep, fyOut, fdydxOut, yError);
copy(yOutput, fyOut);
copy(dydxOutput, fdydxOut);
}
G4double G4BogackiShampine23::DistChord() const
{
G4double yMid[G4FieldTrack::ncompSVEC];
makeStep(fyIn, fdydx, fhstep / 2., yMid);
const G4ThreeVector begin = makeVector(fyIn, Value3D::Position);
const G4ThreeVector mid = makeVector(yMid, Value3D::Position);
const G4ThreeVector end = makeVector(fyOut, Value3D::Position);
return G4LineSection::Distline(mid, begin, end);
}