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geant4/source/geometry/magneticfield/include/G4RKG3_Stepper.hh
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// $Id: G4RKG3_Stepper.hh,v 1.13 2007/05/18 12:44:02 tnikitin Exp $
// GEANT4 tag $Name: geant4-09-01 $
//
//
//
// class G4RKG3_Stepper
//
// Class description:
//
// Integrator Runga-Kutta Stepper from Geant3.
//
// History:
// - Created. J.Apostolakis, V.Grichine - 30.01.97
// -------------------------------------------------------------------
#ifndef G4RKG3_Stepper_hh
#define G4RKG3_Stepper_hh
#include "G4Types.hh"
#include "G4MagIntegratorStepper.hh"
#include "G4ThreeVector.hh"
class G4Mag_EqRhs;
class G4RKG3_Stepper : public G4MagIntegratorStepper
{
public: // with description
G4RKG3_Stepper(G4Mag_EqRhs *EqRhs);
// Integrate over 6 variables only: position & velocity.
// Not implemented yet !
~G4RKG3_Stepper();
void Stepper( const G4double yIn[],
const G4double dydx[],
G4double h,
G4double yOut[],
G4double yErr[] );
// The method which must be provided, even if less efficient.
G4double DistChord() const ;
void StepNoErr( const G4double tIn[7],
const G4double dydx[7],
G4double Step,
G4double tOut[7],
G4double B[3] );
// Integrator RK Stepper from G3 with only two field evaluation per
// Step. It is used in propagation initial Step by small substeps
// after solution error and delta geometry considerations.
// B[3] is magnetic field which is passed from substep to substep.
void StepWithEst( const G4double tIn[7],
const G4double dydx[7],
G4double Step,
G4double tOut[7],
G4double& alpha2,
G4double& beta2,
const G4double B1[3],
G4double B2[3] );
// Integrator for RK from G3 with evaluation of error in solution and delta
// geometry based on naive similarity with the case of uniform magnetic field.
// B1[3] is input and is the first magnetic field values
// B2[3] is output and is the final magnetic field values.
public: // without description
G4int IntegratorOrder() const { return 4; }
private:
G4ThreeVector fyInitial,
fyMidPoint,
fyFinal;
G4ThreeVector fpInitial;
G4ThreeVector BfldIn;
G4double hStep;
G4Mag_EqRhs* fPtrMagEqOfMot;
};
#endif