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geant4/source/geometry/magneticfield/include/G4CashKarpRKF45.hh
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2016-06-08 15:55:53 +02:00

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// This code implementation is the intellectual property of
// the GEANT4 collaboration.
//
// By copying, distributing or modifying the Program (or any work
// based on the Program) you indicate your acceptance of this statement,
// and all its terms.
//
// $Id: G4CashKarpRKF45.hh,v 1.4 2000/11/01 15:15:48 gcosmo Exp $
// GEANT4 tag $Name: geant4-03-00 $
//
//
// class G4CashKarpRKF45
//
// Class description:
//
// The Cash-Karp Runge-Kutta-Fehlberg 4/5 method is an embedded fourth
// order method (giving fifth-order accuracy) for the solution of an ODE.
// Two different fourth order estimates are calculated; their difference
// gives an error estimate. [ref. Numerical Recipes in C, 2nd Edition]
// It is used to integrate the equations of the motion of a particle
// in a magnetic field.
// History:
// - Created. J.Apostolakis, V.Grichine - 30.1.97
#ifndef G4CashKARP_RKF45
#define G4CashKARP_RKF45
#include "G4MagIntegratorStepper.hh"
class G4CashKarpRKF45 : public G4MagIntegratorStepper
{
public: // with description
G4CashKarpRKF45(G4Mag_EqRhs *EqRhs, G4int numberOfVariables = 6) ;
~G4CashKarpRKF45() ;
void Stepper( const G4double y[],
const G4double dydx[],
G4double h,
G4double yout[],
G4double yerr[] ) ;
void StepWithEst( const G4double yIn[],
const G4double dydx[],
G4double Step,
G4double yOut[],
G4double& alpha2,
G4double& beta2,
const G4double B1[],
G4double B2[] ) ;
public: // without description
G4double DistChord() const = 0 ; // This is not IMPLEMENTED yet.
// It must be done before it can work.
G4int IntegratorOrder() const { return 4; }
private:
G4CashKarpRKF45(const G4CashKarpRKF45&);
G4CashKarpRKF45& operator=(const G4CashKarpRKF45&);
// Private copy constructor and assignment operator.
private:
G4int fNumberOfVariables ;
G4double *ak2, *ak3, *ak4, *ak5, *ak6, *ak7, *yTemp, *yIn; // scratch space
};
#endif /* G4CashKARP_RKF45 */