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0001 // 0002 // ******************************************************************** 0003 // * License and Disclaimer * 0004 // * * 0005 // * The Geant4 software is copyright of the Copyright Holders of * 0006 // * the Geant4 Collaboration. It is provided under the terms and * 0007 // * conditions of the Geant4 Software License, included in the file * 0008 // * LICENSE and available at http://cern.ch/geant4/license . These * 0009 // * include a list of copyright holders. * 0010 // * * 0011 // * Neither the authors of this software system, nor their employing * 0012 // * institutes,nor the agencies providing financial support for this * 0013 // * work make any representation or warranty, express or implied, * 0014 // * regarding this software system or assume any liability for its * 0015 // * use. Please see the license in the file LICENSE and URL above * 0016 // * for the full disclaimer and the limitation of liability. * 0017 // * * 0018 // * This code implementation is the result of the scientific and * 0019 // * technical work of the GEANT4 collaboration. * 0020 // * By using, copying, modifying or distributing the software (or * 0021 // * any work based on the software) you agree to acknowledge its * 0022 // * use in resulting scientific publications, and indicate your * 0023 // * acceptance of all terms of the Geant4 Software license. * 0024 // ******************************************************************** 0025 // 0026 // G4TExplicitEuler 0027 // 0028 // Class description: 0029 // 0030 // Templated version of G4ExplicitEuler 0031 // 0032 // 0033 // Created: Josh Xie, June 2014 (supported by Google Summer of Code 2014 ) 0034 // 0035 // Supervisors: Sandro Wenzel, John Apostolakis (CERN) 0036 // Adapted from G4G4TExplicitEuler class 0037 // ------------------------------------------------------------------- 0038 // 0039 // Information from G4Explicit Euler: 0040 // ---------------------------------- 0041 // Explicit Euler stepper for magnetic field: x_1 = x_0 + h * dx_0. 0042 // The simplistic approach to solving linear differential equations. 0043 // Take the current derivative and add it to the current position. 0044 // 0045 // Created: W.Wander <wwc@mit.edu>, 12.09.1997 0046 // ------------------------------------------------------------------- 0047 0048 // -------------------------------------------------------------------- 0049 #ifndef G4TExplicitEuler_HH 0050 #define G4TExplicitEuler_HH 0051 0052 #include "G4TMagErrorStepper.hh" 0053 #include "G4ThreeVector.hh" 0054 0055 template <class T_Equation, int N> 0056 class G4TExplicitEuler 0057 : public G4TMagErrorStepper<G4TExplicitEuler<T_Equation, N>, T_Equation, N> 0058 { 0059 public: // with description 0060 static constexpr double IntegratorCorrection = 1.; 0061 0062 G4TExplicitEuler(T_Equation* EqRhs, G4int numberOfVariables = N) 0063 : G4TMagErrorStepper<G4TExplicitEuler<T_Equation, N>, T_Equation, N>( 0064 EqRhs, numberOfVariables) 0065 , fEquation_Rhs(EqRhs) 0066 { 0067 if( numberOfVariables != N ){ 0068 G4ExceptionDescription msg; 0069 msg << "Equation has an incompatible number of variables." ; 0070 msg << " template N = " << N << " equation-Nvar= " 0071 << numberOfVariables; 0072 G4Exception("G4TExplicitEuler: constructor", "GeomField0003", 0073 FatalErrorInArgument, msg ); 0074 } 0075 } 0076 0077 ~G4TExplicitEuler() { ; } 0078 0079 inline void DumbStepper(const G4double yIn[], 0080 const G4double dydx[], 0081 G4double h, G4double yOut[]) // override final 0082 { 0083 // Initialise time to t0, needed when it is not updated by the integration. 0084 // yOut[7] = yIn[7]; // Better to set it to NaN; // TODO 0085 0086 for(G4int i = 0; i < N; ++i) 0087 { 0088 yOut[i] = yIn[i] + h * dydx[i]; // 1st and only Step 0089 } 0090 0091 return; 0092 } 0093 0094 public: // without description 0095 G4int IntegratorOrder() const { return 1; } 0096 0097 private: 0098 T_Equation* fEquation_Rhs; 0099 }; 0100 0101 #endif /* G4TExplicitEuler_HH */
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