Geant4 Cross Reference |
1 // 1 // 2 // ******************************************* 2 // ******************************************************************** 3 // * License and Disclaimer << 3 // * DISCLAIMER * 4 // * 4 // * * 5 // * The Geant4 software is copyright of th << 5 // * The following disclaimer summarizes all the specific disclaimers * 6 // * the Geant4 Collaboration. It is provided << 6 // * of contributors to this software. The specific disclaimers,which * 7 // * conditions of the Geant4 Software License << 7 // * govern, are listed with their locations in: * 8 // * LICENSE and available at http://cern.ch/ << 8 // * http://cern.ch/geant4/license * 9 // * include a list of copyright holders. << 10 // * 9 // * * 11 // * Neither the authors of this software syst 10 // * Neither the authors of this software system, nor their employing * 12 // * institutes,nor the agencies providing fin 11 // * institutes,nor the agencies providing financial support for this * 13 // * work make any representation or warran 12 // * work make any representation or warranty, express or implied, * 14 // * regarding this software system or assum 13 // * regarding this software system or assume any liability for its * 15 // * use. Please see the license in the file << 14 // * use. * 16 // * for the full disclaimer and the limitatio << 17 // * 15 // * * 18 // * This code implementation is the result << 16 // * This code implementation is the intellectual property of the * 19 // * technical work of the GEANT4 collaboratio << 17 // * GEANT4 collaboration. * 20 // * By using, copying, modifying or distri << 18 // * By copying, distributing or modifying the Program (or any work * 21 // * any work based on the software) you ag << 19 // * based on the Program) you indicate your acceptance of this * 22 // * use in resulting scientific publicati << 20 // * statement, and all its terms. * 23 // * acceptance of all terms of the Geant4 Sof << 24 // ******************************************* 21 // ******************************************************************** 25 // 22 // 26 // G4Field << 23 // >> 24 // $Id: G4Field.hh,v 1.9 2004/09/01 09:59:06 japost Exp $ >> 25 // GEANT4 tag $Name: geant4-07-00-cand-03 $ >> 26 // >> 27 // >> 28 // class G4Field 27 // 29 // 28 // Class description: 30 // Class description: 29 // 31 // 30 // Abstract class for any kind of Field. 32 // Abstract class for any kind of Field. 31 // It allows any kind of field (vector, scalar 33 // It allows any kind of field (vector, scalar, tensor and any set of them) 32 // to be defined by implementing the inquiry f 34 // to be defined by implementing the inquiry function interface. 33 // 35 // 34 // The key method is GetFieldValue( const do 36 // The key method is GetFieldValue( const double Point[4], 35 // ************* do 37 // ************* double *fieldArr ) 36 // Given an input position/time vector 'Point' 38 // Given an input position/time vector 'Point', 37 // this method must return the value of the fi 39 // this method must return the value of the field in "fieldArr". 38 // 40 // 39 // A field must also specify whether it change 41 // A field must also specify whether it changes a track's energy: 40 // DoesFieldChangeEnergy() 42 // DoesFieldChangeEnergy() 41 // ********************* 43 // ********************* 42 // A field must co-work with a corresponding E 44 // A field must co-work with a corresponding Equation of Motion, to 43 // enable the integration of a particle's posi 45 // enable the integration of a particle's position, momentum and, optionally, 44 // spin. For this a field and its equation of 46 // spin. For this a field and its equation of motion must follow the 45 // same convention for the order of field comp 47 // same convention for the order of field components in the array "fieldArr" 46 << 47 // Created: John Apostolakis, 10.03.1997 << 48 // ------------------------------------------- 48 // ------------------------------------------------------------------- >> 49 // History: >> 50 // - Created: John Apostolakis, 10.03.1997 >> 51 // - Modified: >> 52 // V. Grichine 8 Nov 2001: Extended "Point" arg to [4] array to add time >> 53 // J. Apostolakis 5 Nov 2003: Added virtual method DoesFieldChangeEnergy() >> 54 // J. Apostolakis 31 Aug 2004: Information on convention for components >> 55 // ------------------------------------------------------------------- >> 56 49 #ifndef G4FIELD_HH 57 #ifndef G4FIELD_HH 50 #define G4FIELD_HH 58 #define G4FIELD_HH 51 59 52 #include "G4Types.hh" 60 #include "G4Types.hh" 53 #include "globals.hh" << 54 61 55 class G4Field 62 class G4Field 56 { 63 { 57 public: // with description 64 public: // with description 58 65 59 G4Field( G4bool gravityOn = false); << 66 virtual void GetFieldValue( const double Point[4], 60 G4Field( const G4Field& ); << 67 double *fieldArr ) const = 0; 61 virtual ~G4Field(); << 62 G4Field& operator = (const G4Field& p); << 63 << 64 virtual void GetFieldValue( const G4doub << 65 G4doub << 66 // Given the position time vector 'Poin 68 // Given the position time vector 'Point', 67 // return the value of the field in the 69 // return the value of the field in the array fieldArr. 68 // Notes: 70 // Notes: 69 // 1) The 'Point' vector has the foll 71 // 1) The 'Point' vector has the following structure: 70 // Point[0] is x ( position, 72 // Point[0] is x ( position, in Geant4 units ) 71 // Point[1] is y 73 // Point[1] is y 72 // Point[2] is z 74 // Point[2] is z 73 // Point[3] is t ( time, in 75 // Point[3] is t ( time, in Geant4 units ) 74 // 2) The convention for the componen 76 // 2) The convention for the components of the field 75 // array 'fieldArr' are determined 77 // array 'fieldArr' are determined by the type of field. 76 // See for example the class G4Ele 78 // See for example the class G4ElectroMagneticField. 77 79 78 virtual G4bool DoesFieldChangeEnergy() c << 80 G4Field(){;} 79 // Each type/class of field should res << 81 virtual ~G4Field(){;} 80 // For example: << 82 inline G4Field& operator = (const G4Field &p); 81 // - an electric field should re << 83 82 // - a pure magnetic field should re << 84 // A field signature function that can be used to insure 83 << 85 // that the Equation of motion object and the G4Field object 84 inline G4bool IsGravityActive() const; << 86 // have the same "field signature"? 85 // Does this field include gravity? << 87 86 << 88 virtual G4bool DoesFieldChangeEnergy() const= 0 ; 87 inline void SetGravityActive( G4bool OnO << 89 // Each type/class of field should respond this accordingly 88 << 90 // For example: 89 virtual G4Field* Clone() const; << 91 // - an electric field should return "true" 90 // Implements cloning, needed by multi << 92 // - a pure magnetic field should return "false" 91 << 92 static constexpr G4int MAX_NUMBER_OF_COM << 93 << 94 private: << 95 93 96 G4bool fGravityActive = false; << 97 }; 94 }; 98 95 99 // Inline methods ... << 96 inline G4Field& G4Field::operator = (const G4Field &p) 100 << 101 inline G4bool G4Field::IsGravityActive() const << 102 { 97 { 103 return fGravityActive; << 98 if (&p != this) { *this = p; } >> 99 return *this; 104 } 100 } 105 101 106 inline void G4Field::SetGravityActive( G4bool << 102 #endif /* G4FIELD_HH */ 107 { << 108 fGravityActive = OnOffFlag; << 109 } << 110 << 111 #endif << 112 103