// // ******************************************************************** // * 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. * // ******************************************************************** // // G4VFSALIntegrationStepper // // Class description: // // Class similar to G4VMagIntegratorStepper, for steppers which // estimate the value of the derivative at the projected endpoint // of integration - at each successful step. // This ability is known as 'First Same As Last' (FSAL). It // reduces the number of required calls to the equation's // RightHandSide method, and, as such the number of calls to the // (potentially expensive) field evaluation methods. // // Based on G4VMagIntegratorStepper // Author: Somnath Banerjee (CERN, Google Summer of Code 2015), 26.05.2016 // Supervision: John Apostolakis (CERN) // -------------------------------------------------------------------- #ifndef G4VFSALINTEGRATOR_STEPPER_HH #define G4VFSALINTEGRATOR_STEPPER_HH #include "G4Types.hh" #include "G4EquationOfMotion.hh" /** * @brief G4VFSALIntegrationStepper is a class similar to * G4VMagIntegratorStepper, but for steppers which estimate the value of * the derivative at the projected endpoint of integration, at each successful * step. This ability is known as 'First Same As Last' (FSAL). * It reduces the number of required calls to the equation's RightHandSide * method, and, as such the number of calls to the (potentially expensive) * field evaluation methods. */ class G4VFSALIntegrationStepper { public: /** * Constructor for G4VFSALIntegrationStepper. * @param[in] Equation Pointer to the provided equation of motion. * @param[in] numStateVariables The number of state variables. */ G4VFSALIntegrationStepper (G4EquationOfMotion* Equation, G4int numIntegrationVariables, G4int numStateVariables = 12); /** * Default Destructor. */ virtual ~G4VFSALIntegrationStepper() = default; /** * Copy constructor and assignment operator not allowed. */ G4VFSALIntegrationStepper(const G4VFSALIntegrationStepper&) = delete; G4VFSALIntegrationStepper& operator=(const G4VFSALIntegrationStepper&) = delete; /** * The stepper for the Runge Kutta integration. * The stepsize is fixed, with the step size given by 'h'. * Integrates ODE starting values yInput[0 to 6]. * Outputs yout[] and its estimated error yerr[]. * @param[in] y Starting values array of integration variables. * @param[in] dydx Derivatives array. * @param[in] h The given step size. * @param[out] yout Integration output. * @param[out] yerr The estimated error. * @param[out] lastDydx Last derivative. */ virtual void Stepper( const G4double y[], const G4double dydx[], G4double h, G4double yout[], G4double yerr[], G4double lastDydx[]) = 0; /** * Returns an estimate of the maximum distance of a chord from the * true path over the segment last integrated. */ virtual G4double DistChord() const = 0; /** * Simple utility function to (re)normalise 'unit velocity' vector. */ inline void NormaliseTangentVector( G4double vec[6] ); /** * Simple utility function to (re)normalise 'unit spin' vector. */ inline void NormalisePolarizationVector( G4double vec[12] ); /** * Utility method to supply the standard Evaluation of the * Right Hand side of the associated equation. */ void RightHandSide( const double y[], double dydx[] ); /** * Returns the number of variables that the stepper will integrate over. */ inline G4int GetNumberOfVariables() const; /** * Returns the number of variables of state variables (>= above, integration) */ inline G4int GetNumberOfStateVariables() const; /** * Returns the order of the integrator, i.e. its error behaviour * is of the order O(h^order). */ virtual G4int IntegratorOrder() const = 0; /** * Returns a pointer to the equation of motion. * As some steppers (e.g. RKG3) require other methods of Eq_Rhs, * this function allows for access to them. */ inline G4EquationOfMotion* GetEquationOfMotion(); /** * Setter for the equation of motion. */ inline void SetEquationOfMotion(G4EquationOfMotion* newEquation); /** * Methods for debug use. */ inline G4int GetfNoRHSCalls() { return fNoRHSCalls; } void increasefNORHSCalls(); inline void ResetfNORHSCalls() { fNoRHSCalls = 0; } private: G4EquationOfMotion* fEquation_Rhs = nullptr; /** Variables in integration. */ const G4int fNoIntegrationVariables = 0; /** Number required for FieldTrack. */ const G4int fNoStateVariables = 0; /** Used for debug. */ G4int fNoRHSCalls = 0; }; #include "G4VFSALIntegrationStepper.icc" #endif