// // ******************************************************************** // * 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. * // ******************************************************************** // // G4TMagFieldEquation // // Class description: // // Templated version of equation of motion of a particle in a pure // magnetic field. // Enables use of inlined code for field, equation, stepper, driver, // avoiding all virtual calls. // // Adapted from G4Mag_UsualEqRhs. // // Author: Josh Xie (CERN, Google Summer of Code 2014), June 2014 // Supervisors: Sandro Wenzel, John Apostolakis (CERN) // -------------------------------------------------------------------- #ifndef G4TMAGFIELD_EQUATION_HH #define G4TMAGFIELD_EQUATION_HH #include "G4Mag_UsualEqRhs.hh" /** * @brief G4TMagFieldEquation is a templated version of G4MagFieldEquation. */ template class G4TMagFieldEquation : public G4Mag_UsualEqRhs { public: G4TMagFieldEquation(T_Field* f) : G4Mag_UsualEqRhs(f) { itsField = f; } virtual ~G4TMagFieldEquation() = default; inline void GetFieldValue(const G4double Point[4], G4double Field[]) const { itsField->T_Field::GetFieldValue(Point, Field); } inline void TEvaluateRhsGivenB( const G4double y[], const G4double B[3], G4double dydx[] ) const { G4double momentum_mag_square = y[3]*y[3] + y[4]*y[4] + y[5]*y[5]; G4double inv_momentum_magnitude = 1.0 / std::sqrt( momentum_mag_square ); G4double cof = FCof()*inv_momentum_magnitude; dydx[0] = y[3]*inv_momentum_magnitude; // (d/ds)x = Vx/V dydx[1] = y[4]*inv_momentum_magnitude; // (d/ds)y = Vy/V dydx[2] = y[5]*inv_momentum_magnitude; // (d/ds)z = Vz/V dydx[3] = cof*(y[4]*B[2] - y[5]*B[1]) ; // Ax = a*(Vy*Bz - Vz*By) dydx[4] = cof*(y[5]*B[0] - y[3]*B[2]) ; // Ay = a*(Vz*Bx - Vx*Bz) dydx[5] = cof*(y[3]*B[1] - y[4]*B[0]) ; // Az = a*(Vx*By - Vy*Bx) return ; } __attribute__((always_inline)) void RightHandSide( const G4double y[], G4double dydx[] ) // const { G4double Field[G4maximum_number_of_field_components]; G4double PositionAndTime[4]; PositionAndTime[0] = y[0]; PositionAndTime[1] = y[1]; PositionAndTime[2] = y[2]; PositionAndTime[3] = y[7]; GetFieldValue(PositionAndTime, Field) ; TEvaluateRhsGivenB(y, Field, dydx); } private: enum { G4maximum_number_of_field_components = 24 }; // Dependent objects T_Field* itsField; }; #endif