// // ******************************************************************** // * 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. * // ******************************************************************** // // // // // class G4BFieldIntegrationDriver // // Class description: // // Specialized integration driver for pure magnetic field // History: // - Created. D.Sorokin // -------------------------------------------------------------------- #include "globals.hh" #include "G4GeometryTolerance.hh" #include "G4FieldTrack.hh" #include "G4FieldUtils.hh" namespace internal { G4Mag_EqRhs* toMagneticEquation(G4EquationOfMotion* equation) { auto e = dynamic_cast(equation); if (!e) { G4Exception("G4BFieldIntegrationDriver::G4BFieldIntegrationDriver", "GeomField0003", FatalErrorInArgument, "Works only with G4Mag_EqRhs"); } return e; } } // internal template G4BFieldIntegrationDriver::G4BFieldIntegrationDriver(G4double hminimum, T* pStepper, G4int numComponents, G4int statisticsVerbose) : G4IntegrationDriver(hminimum, pStepper, numComponents, statisticsVerbose) , fallbackThreshold(pi / 3.) , fequation(internal::toMagneticEquation(pStepper->GetEquationOfMotion())) , fallbackStepper(fequation) { } template bool G4BFieldIntegrationDriver::QuickAdvance(G4FieldTrack& fieldTrack, const G4double dydx[], G4double hstep, G4double inverseCurvatureRadius, G4double& dchord_step, G4double& dyerr) { if (hstep * inverseCurvatureRadius < fallbackThreshold) { return G4IntegrationDriver::QuickAdvance( fieldTrack, dydx, hstep, inverseCurvatureRadius, dchord_step, dyerr); } G4IntegrationDriver::IncrementQuickAdvanceCalls(); G4double yError[G4FieldTrack::ncompSVEC], yIn[G4FieldTrack::ncompSVEC], yOut[G4FieldTrack::ncompSVEC]; fieldTrack.DumpToArray(yIn); fallbackStepper.Stepper(yIn, dydx, hstep, yOut, yError); dchord_step = fallbackStepper.DistChord(); dyerr = field_utils::absoluteError(yOut, yError, hstep); fieldTrack.LoadFromArray(yOut, fallbackStepper.GetNumberOfVariables()); fieldTrack.SetCurveLength(fieldTrack.GetCurveLength() + hstep); return true; } template void G4BFieldIntegrationDriver::SetEquationOfMotion(G4EquationOfMotion* equation) { G4IntegrationDriver::SetEquationOfMotion(equation); fequation = internal::toMagneticEquation(equation); } template G4double G4BFieldIntegrationDriver::GetInverseCurvatureRadius(const G4FieldTrack& track, G4double field[]) const { const G4double Bmag = std::sqrt(field[0] * field[0] + field[1] * field[1] + field[2] * field[2]); const G4double momentum = track.GetMomentum().mag(); const G4double particleCharge = fequation->FCof() / (CLHEP::eplus * CLHEP::c_light); return std::abs(field_utils::inverseCurvatureRadius(particleCharge, momentum, Bmag)); }