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geant4/source/geometry/magneticfield/include/G4BogackiShampine45.hh
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//
// ********************************************************************
// * License and Disclaimer *
// * *
// * The Geant4 software is copyright of the Copyright Holders of *
// * the Geant4 Collaboration. It is provided under the terms and *
// * conditions of the Geant4 Software License, included in the file *
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// * *
// * Neither the authors of this software system, nor their employing *
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// * work make any representation or warranty, express or implied, *
// * regarding this software system or assume any liability for its *
// * use. Please see the license in the file LICENSE and URL above *
// * for the full disclaimer and the limitation of liability. *
// * *
// * This code implementation is the result of the scientific and *
// * technical work of the GEANT4 collaboration. *
// * By using, copying, modifying or distributing the software (or *
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// ********************************************************************
//
// An implementation of the embedded RK method from the following paper
// by P. Bogacki and L. F. Shampine:
// “An efficient Runge-Kutta (4,5) pair,”
// Comput. Math. with Appl., vol. 32, no. 6, pp. 1528, Sep. 1996.
//
// An interpolation method provides the value of an intermediate
// point in a step -- if a step was sucessful.
//
// This version can provide the FSAL property of the method,
// which allows the reuse of the last derivative in the next step.
// but only by using the additional method GetLastDyDx.
// (Alternative interface for simpler use of FSAL is under development.)
//
// Design & Implementation by Somnath Banerjee
// Supervision & code review: John Apostolakis
//
// Work supported by the Google Summer of Code 2015.
//
///////////////////////////////////////////////////////////////////////////////
#ifndef Bogacki_Shampine_45
#define Bogacki_Shampine_45
#include "G4MagIntegratorStepper.hh"
class G4BogackiShampine45 : public G4MagIntegratorStepper
{
public:
G4BogackiShampine45(G4EquationOfMotion *EqRhs,
G4int numberOfVariables = 6,
G4bool primary = true);
~G4BogackiShampine45();
void Stepper( const G4double y[],
const G4double dydx[],
G4double h,
G4double yout[],
G4double yerr[] ) ;
// This Stepper provides 'dense output'. After a successful
// step, it is possible to obtain an estimate of the value
// of the function at an intermediate point of the interval.
// This requires only two additional evaluations of the
// derivative (and thus the field).
inline void SetupInterpolation()
// const G4double yInput[], const G4double dydx[], const G4double Step )
{
SetupInterpolationHigh(); // ( yInput, dydx, Step);
}
//For calculating the output at the tau fraction of Step
inline void Interpolate( // const G4double yInput[],
// const G4double dydx[],
// const G4double Step,
G4double tau,
G4double yOut[]) // Output value
{
InterpolateHigh( tau, yOut);
// InterpolateHigh( yInput, dydx, Step, yOut, tau);
}
void SetupInterpolationHigh();
// Was: ( const G4double yInput[], const G4double, const G4double Step );
// For calculating the output at the tau fraction of Step
void InterpolateHigh( // const G4double yInput[],
// const G4double dydx[],
// const G4double Step,
G4double tau,
G4double yOut[] ) const;
G4double DistChord() const;
G4int IntegratorOrder() const { return 4; }
void GetLastDydx( G4double dyDxLast[] );
void PrepareConstants(); // Initialise the values of the bi[][] array
private :
G4BogackiShampine45(const G4BogackiShampine45&);
G4BogackiShampine45& operator=(const G4BogackiShampine45&);
G4double *ak2, *ak3, *ak4, *ak5, *ak6, *ak7, *ak8,
*ak9, *ak10, *ak11, *yTemp, *yIn;
G4double *p[6];
G4double fLastStepLength;
G4double *fLastInitialVector, *fLastFinalVector, *fLastDyDx,
*fMidVector, *fMidError;
// for DistChord calculations
G4BogackiShampine45* fAuxStepper; // For chord - until interpolation is proven
bool fPreparedInterpolation;
// Class constants
static bool fPreparedConstants;
static G4double bi[12][7];
};
#endif /* defined(__Geant4__G4BogackiShampine45__) */