Geant4 Cross Reference |
>> 1 // This code implementation is the intellectual property of >> 2 // the GEANT4 collaboration. 1 // 3 // 2 // ******************************************* << 4 // By copying, distributing or modifying the Program (or any work 3 // * License and Disclaimer << 5 // based on the Program) you indicate your acceptance of this statement, 4 // * << 6 // and all its terms. 5 // * The Geant4 software is copyright of th << 6 // * the Geant4 Collaboration. It is provided << 7 // * conditions of the Geant4 Software License << 8 // * LICENSE and available at http://cern.ch/ << 9 // * include a list of copyright holders. << 10 // * << 11 // * Neither the authors of this software syst << 12 // * institutes,nor the agencies providing fin << 13 // * work make any representation or warran << 14 // * regarding this software system or assum << 15 // * use. Please see the license in the file << 16 // * for the full disclaimer and the limitatio << 17 // * << 18 // * This code implementation is the result << 19 // * technical work of the GEANT4 collaboratio << 20 // * By using, copying, modifying or distri << 21 // * any work based on the software) you ag << 22 // * use in resulting scientific publicati << 23 // * acceptance of all terms of the Geant4 Sof << 24 // ******************************************* << 25 // 7 // 26 // G4EqMagElectricField << 8 // $Id: G4EqMagElectricField.hh,v 1.1.10.1 1999/12/07 20:47:59 gunter Exp $ >> 9 // GEANT4 tag $Name: geant4-01-00 $ 27 // 10 // 28 // Class description: << 11 // This is the right-hand side of equation of motion in a combined >> 12 // electric and magnetic field. >> 13 //// >> 14 // 10.11.98 V.Grichine 29 // 15 // 30 // This is the right-hand side of equation of << 16 #ifndef G4EQMAGELECTRICFIELD_hh 31 // electric and magnetic field. << 17 #define G4EQMAGELECTRICFIELD_hh 32 18 33 // Created: V.Grichine, 10.11.1998 << 19 #include "G4Mag_EqRhs.hh" 34 // ------------------------------------------- << 35 #ifndef G4EQMAGELECTRICFIELD_HH << 36 #define G4EQMAGELECTRICFIELD_HH << 37 << 38 #include "G4ChargeState.hh" << 39 #include "G4EquationOfMotion.hh" << 40 #include "G4ElectroMagneticField.hh" 20 #include "G4ElectroMagneticField.hh" 41 21 42 class G4EqMagElectricField : public G4Equation << 22 class G4EqMagElectricField : public G4Mag_EqRhs 43 { 23 { 44 public: 24 public: >> 25 G4EqMagElectricField( G4ElectroMagneticField *emField ) : >> 26 G4Mag_EqRhs( emField ) {}; >> 27 >> 28 ~G4EqMagElectricField() {} ; 45 29 46 G4EqMagElectricField(G4ElectroMagneticFiel << 30 // Given the value of the electromagnetic field, this function 47 ~G4EqMagElectricField() override; << 31 // calculates the value of the derivative dydx. 48 32 49 void SetChargeMomentumMass(G4ChargeState << 33 void SetChargeMomentumMass( const G4double particleCharge, // in e+ units 50 G4double Momen << 34 const G4double MomentumXc, 51 G4double mass) << 35 const G4double mass); 52 << 36 53 void EvaluateRhsGivenB(const G4double y[], << 37 void EvaluateRhsGivenB( const G4double y[], 54 const G4double Fiel << 38 const G4double Field[], 55 G4double dydx << 39 G4double dydx[] ) const; 56 // Given the value of the electromagneti << 57 // calculates the value of the derivativ << 58 40 59 private: << 41 private: 60 42 61 G4double fElectroMagCof = 0.0; << 43 G4double fElectroMagCof ; 62 G4double fMassCof = 0.0; << 63 }; 44 }; 64 45 65 #endif 46 #endif 66 47