// 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: G4Mag_EqRhs.hh,v 1.5 2000/11/01 15:15:50 gcosmo Exp $ // GEANT4 tag $Name: geant4-03-00 $ // // // class G4Mag_EqRhs // // Class description: // // The "standard" right-hand side for the equation of motion of a particle // in a pure magnetic field. // Others that might be required are: // i) when using a moving reference frame ... or // ii) extending for other forces, eg an electric field. // History: // - Created. J.Apostolakis, January 13th 1996 #ifndef G4_MAG_EQRHS_DEF #define G4_MAG_EQRHS_DEF #include "globals.hh" #include "G4EquationOfMotion.hh" #include "G4MagneticField.hh" // class G4MagneticField; not enough ?? class G4Mag_EqRhs : public G4EquationOfMotion { public: // with description G4Mag_EqRhs( G4MagneticField *magField ); virtual ~G4Mag_EqRhs(); // Constructor and destructor. No actions. virtual void EvaluateRhsGivenB( const G4double y[], const G4double B[3], G4double dydx[] ) const = 0; // Given the value of the field "B", this function // calculates the value of the derivative dydx. // This is the _only_ function a subclass must define. // The other two functions use Rhs_givenB. inline G4double FCof() const; virtual void SetChargeMomentumMass( G4double particleCharge, // in e+ units G4double MomentumXc, G4double mass); private: G4double fCof_val; static const G4double fUnitConstant; // Set in G4Mag_EqRhs.cc // to 0.299792458 // Coefficient in the Lorentz motion equation (Lorentz force), if the // magnetic field B is in Tesla, the particle charge in units of the // elementary (positron?) charge, the momentum P in MeV/c, and the // space coordinates and path along the trajectory in mm . }; inline G4double G4Mag_EqRhs::FCof() const { return fCof_val; } #endif /* G4_MAG_EQRHS_DEF */