// // ******************************************************************** // * 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 * // * LICENSE and available at http://cern.ch/geant4/license . These * // * include a list of copyright holders. * // * * // * Neither the authors of this software system, nor their employing * // * institutes,nor the agencies providing financial support for this * // * 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 * // * any work based on the software) you agree to acknowledge its * // * use in resulting scientific publications, and indicate your * // * acceptance of all terms of the Geant4 Software license. * // ******************************************************************** // // // $Id: G4ElectroMagneticField.hh,v 1.11 2006-06-29 18:22:01 gunter Exp $ // GEANT4 tag $Name: not supported by cvs2svn $ // // // class G4ElectroMagneticField // // Class description: // // A full Electromagnetic field, containing both electric and magnetic fields. // It is an abstract class, and a derived type of this field must be // created by the user to describe his/her field configuration. // We have established a convention for the electromagnetic field components: // In the GetValue method, the return values of Bfield will have // the following meaning // - Components 0, 1 and 2 are the Magnetic Field (x, y, z respectively); // - Components 3, 4 and 5 are the Electric field (x, y, z respectively). // // Note 1: one or the other field could optional, depending on the Equation // Note 2: such a convention is required between any field and its // corresponding equation of motion. // // History: // - Created: J. Apostolakis, November 12th, 1998 // - Modified: // V. Grichine 8 Nov 2001: Extended "Point" arg to [4] array to add time // G. Cosmo 2 Apr 2003: Reorgansised, moved inline methods to .cc // J. Apostolakis 5 Nov 2003: Derive directly from G4Field // J. Apostolakis 31 Aug 2004: Information on convention for components // ------------------------------------------------------------------- #ifndef G4ELECTROMAGNETIC_FIELD_DEF #define G4ELECTROMAGNETIC_FIELD_DEF #include "G4Field.hh" class G4ElectroMagneticField : public G4Field { public: // with description G4ElectroMagneticField(); virtual ~G4ElectroMagneticField(); G4ElectroMagneticField(const G4ElectroMagneticField &r); G4ElectroMagneticField& operator = (const G4ElectroMagneticField &p); // Copy constructor & assignment operators. virtual void GetFieldValue(const G4double Point[4], G4double *Bfield ) const = 0; // Return as Bfield[0], [1], [2] the magnetic field x, y & z components // and as Bfield[3], [4], [5] the electric field x, y & z components virtual G4bool DoesFieldChangeEnergy() const = 0; // For field with an electric component this should be true // For pure magnetic field this should be false // Alternative: default safe implementation { return true; } }; #endif /* G4ELECTROMAGNETIC_FIELD_DEF */