// // ******************************************************************** // * 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. * // ******************************************************************** // // G4ClassicalRK4 // // Class description: // // Integrate the equations of the motion of a particle in a magnetic field // using the classical 4th Runge-Kutta method. // Authors: J.Apostolakis, V.Grichine (CERN), 30.01.1997 // ------------------------------------------------------------------- #ifndef G4CLASSICALRK4_HH #define G4CLASSICALRK4_HH #include "G4MagErrorStepper.hh" /** * @brief G4ClassicalRK4 integrates the equations of the motion of a particle * in a magnetic field using the classical 4th Runge-Kutta method. */ class G4ClassicalRK4 : public G4MagErrorStepper { public: /** * Constructor for G4ClassicalRK4. * @param[in] EquationMotion Pointer to the provided equation of motion. * @param[in] numberOfVariables The number of integration variables. */ G4ClassicalRK4(G4EquationOfMotion* EquationMotion, G4int numberOfVariables = 6) ; /** * Destructor. */ ~G4ClassicalRK4() override ; /** * Copy constructor and assignment operator not allowed. */ G4ClassicalRK4(const G4ClassicalRK4&) = delete; G4ClassicalRK4& operator=(const G4ClassicalRK4&) = delete; // A stepper that does not know about errors. // It is used by the MagErrorStepper stepper. /** * Given values for the variables y[0,..,n-1] and their derivatives * dydx[0,...,n-1] known at x, uses the classical 4th Runge-Kutta * method to advance the solution over an interval h and returns the * incremented variables as yout[0,...,n-1]. The user supplies the * function RightHandSide(x,y,dydx), which returns derivatives dydx at x. * The source is routine rk4 from NRC p.712-713. * @param[in] yIn Starting values array of integration variables. * @param[in] dydx Derivatives array. * @param[in] h The given step size. * @param[out] yOut Integration output. */ void DumbStepper( const G4double yIn[], const G4double dydx[], G4double h, G4double yOut[] ) override ; /** * Returns the order, 4, of integration. */ G4int IntegratorOrder() const override { return 4; } /** * Returns the stepper type-ID, "kClassicalRK4". */ G4StepperType StepperType() const override { return kClassicalRK4; } private: G4double *dydxm, *dydxt, *yt; // scratch space - not state }; #endif