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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 // G4ConstRK4 0027 // 0028 // Class description: 0029 // 0030 // G4ConstRK4 performs the integration of one step with error calculation 0031 // in constant magnetic field. The integration method is the same as in 0032 // ClassicalRK4. The field value is assumed constant for the step. 0033 // This field evaluation is called only once per step. 0034 // G4ConstRK4 can be used only for magnetic fields. 0035 0036 // Authors: J.Apostolakis, T.Nikitina (CERN), 18.09.2008 0037 // ------------------------------------------------------------------- 0038 #ifndef G4CONSTRK4_HH 0039 #define G4CONSTRK4_HH 0040 0041 #include "G4MagErrorStepper.hh" 0042 #include "G4EquationOfMotion.hh" 0043 #include "G4Mag_EqRhs.hh" 0044 0045 /** 0046 * @brief G4ConstRK4 performs the integration of one step with error 0047 * calculation in constant magnetic field. The integration method is the 0048 * same as in ClassicalRK4. The field value is assumed constant for the step. 0049 * This field evaluation is called only once per step. 0050 * G4ConstRK4 can be used only for magnetic fields. 0051 */ 0052 0053 class G4ConstRK4 : public G4MagErrorStepper 0054 { 0055 public: 0056 0057 /** 0058 * Constructor for G4ConstRK4. 0059 * @param[in] EqRhs Pointer to the provided equation of motion. 0060 * @param[in] numberOfVariables The number of integration variables. 0061 */ 0062 G4ConstRK4(G4Mag_EqRhs* EquationMotion, 0063 G4int numberOfStateVariables=8); 0064 0065 /** 0066 * Destructor. 0067 */ 0068 ~G4ConstRK4() override; 0069 0070 /** 0071 * Copy constructor and assignment operator not allowed. 0072 */ 0073 G4ConstRK4(const G4ConstRK4&) = delete; 0074 G4ConstRK4& operator=(const G4ConstRK4&) = delete; 0075 0076 /** 0077 * The stepper for the Runge Kutta integration. 0078 * The stepsize is fixed, with the step size given by 'h'. 0079 * Integrates ODE starting values y[0 to 6]. 0080 * Outputs yout[] and its estimated error yerr[]. 0081 * @param[in] y Starting values array of integration variables. 0082 * @param[in] dydx Derivatives array. 0083 * @param[in] h The given step size. 0084 * @param[out] yout Integration output. 0085 * @param[out] yerr The estimated error. 0086 */ 0087 void Stepper( const G4double y[], 0088 const G4double dydx[], 0089 G4double h, 0090 G4double yout[], 0091 G4double yerr[] ) override; 0092 0093 /** 0094 * Given values for the variables y[0,..,n-1] and their derivatives 0095 * dydx[0,...,n-1] known at x, uses the classical 4th Runge-Kutta 0096 * method to advance the solution over an interval h and returns the 0097 * incremented variables as yout[0,...,n-1]. The user supplies the 0098 * function RightHandSide(x,y,dydx), which returns derivatives dydx at x. 0099 * The source is routine rk4 from NRC p.712-713. 0100 * @param[in] y Starting values array of integration variables. 0101 * @param[in] dydx Derivatives array. 0102 * @param[in] h The given step size. 0103 * @param[out] yout Integration output. 0104 */ 0105 void DumbStepper( const G4double yIn[], 0106 const G4double dydx[], 0107 G4double h, 0108 G4double yOut[] ) override ; 0109 0110 /** 0111 * Returns the distance from chord line. 0112 */ 0113 G4double DistChord() const override; 0114 0115 /** 0116 * Returns the derivatives value, at position and time 'y'. 0117 * @param[in] y The position vector plus time (x,y,z,t). 0118 * @param[out] dydx The derivatives array. 0119 */ 0120 inline void RightHandSideConst(const G4double y[], G4double dydx[] ) const; 0121 0122 /** 0123 * Returns the field values, at position and time 'y'. 0124 * @param[in] y The position vector plus time (x,y,z,t). 0125 * @param[out] Field The field value in output. 0126 */ 0127 inline void GetConstField(const G4double y[], G4double Field[]); 0128 0129 /** 0130 * Returns the order, 4, of integration. 0131 */ 0132 inline G4int IntegratorOrder() const override { return 4; } 0133 0134 /** 0135 * Returns the stepper type-ID, "kConstRK4". 0136 */ 0137 inline G4StepperType StepperType() const override { return kConstRK4; } 0138 0139 private: 0140 0141 G4ThreeVector fInitialPoint, fMidPoint, fFinalPoint; 0142 // Data stored in order to find the chord 0143 G4double *dydxm, *dydxt, *yt; // scratch space - not state 0144 G4double *yInitial, *yMiddle, *dydxMid, *yOneStep; 0145 G4Mag_EqRhs* fEq = nullptr; 0146 G4double Field[3]; 0147 }; 0148 0149 // Inline methods 0150 0151 inline void G4ConstRK4::RightHandSideConst(const G4double y[], 0152 G4double dydx[] ) const 0153 { 0154 0155 G4double momentum_mag_square = y[3]*y[3] + y[4]*y[4] + y[5]*y[5]; 0156 G4double inv_momentum_magnitude = 1.0 / std::sqrt( momentum_mag_square ); 0157 0158 G4double cof = fEq->FCof()*inv_momentum_magnitude; 0159 0160 dydx[0] = y[3]*inv_momentum_magnitude; // (d/ds)x = Vx/V 0161 dydx[1] = y[4]*inv_momentum_magnitude; // (d/ds)y = Vy/V 0162 dydx[2] = y[5]*inv_momentum_magnitude; // (d/ds)z = Vz/V 0163 0164 dydx[3] = cof*(y[4]*Field[2] - y[5]*Field[1]) ; // Ax = a*(Vy*Bz - Vz*By) 0165 dydx[4] = cof*(y[5]*Field[0] - y[3]*Field[2]) ; // Ay = a*(Vz*Bx - Vx*Bz) 0166 dydx[5] = cof*(y[3]*Field[1] - y[4]*Field[0]) ; // Az = a*(Vx*By - Vy*Bx) 0167 } 0168 0169 inline void G4ConstRK4::GetConstField(const G4double y[], G4double B[]) 0170 { 0171 G4double PositionAndTime[4]; 0172 0173 PositionAndTime[0] = y[0]; 0174 PositionAndTime[1] = y[1]; 0175 PositionAndTime[2] = y[2]; 0176 // Global Time 0177 PositionAndTime[3] = y[7]; 0178 fEq -> GetFieldValue(PositionAndTime, B); 0179 } 0180 0181 #endif
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