Geant4 10.7.0
Toolkit for the simulation of the passage of particles through matter
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G4VFSALIntegrationStepper.hh
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1//
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25//
26// G4VFSALIntegrationStepper
27//
28// Class description:
29//
30// Class similar to G4VMagIntegratorStepper, for steppers which
31// estimate the value of the derivative at the projected endpoint
32// of integration - at each successful step.
33// This ability is known as 'First Same As Last' (FSAL). It
34// reduces the number of required calls to the equation's
35// RightHandSide method, and, as such the number of calls to the
36// (potentially expensive) field evaluation methods.
37//
38// Based on G4VMagIntegratorStepper
39
40// Author: Somnath Banerjee, Google Summer of Code 2015
41// Supervision: John Apostolakis, CERN
42// --------------------------------------------------------------------
43#ifndef G4VFSALINTEGRATOR_STEPPER_HH
44#define G4VFSALINTEGRATOR_STEPPER_HH
45
46#include "G4Types.hh"
47#include "G4EquationOfMotion.hh"
48
50{
51 public: // with description
52
54 G4int numIntegrationVariables,
55 G4int numStateVariables = 12);
56 virtual ~G4VFSALIntegrationStepper() = default;
57 // Constructor and destructor. No actions.
58
61
62 virtual void Stepper( const G4double y[],
63 const G4double dydx[],
64 G4double h,
65 G4double yout[],
66 G4double yerr[],
67 G4double lastDydx[]) = 0;
68 // The stepper for the Runge Kutta integration.
69 // The stepsize is fixed, with the Step size given by h.
70 // Integrates ODE starting values y[0 to 6].
71 // Outputs yout[] and its estimated error yerr[].
72
73 virtual G4double DistChord() const = 0;
74 // Estimate the maximum distance of a chord from the true path
75 // over the segment last integrated.
76
77 inline void NormaliseTangentVector( G4double vec[6] );
78 // Simple utility function to (re)normalise 'unit velocity' vector.
79
80 inline void NormalisePolarizationVector( G4double vec[12] );
81 // Simple utility function to (re)normalise 'unit spin' vector.
82
83 void RightHandSide( const double y[], double dydx[] );
84 // Utility method to supply the standard Evaluation of the
85 // Right Hand side of the associated equation.
86
88 // Get the number of variables that the stepper will integrate over.
89
91 // Get the number of variables of state variables (>= above, integration)
92
93 virtual G4int IntegratorOrder() const = 0;
94 // Returns the order of the integrator
95 // i.e. its error behaviour is of the order O(h^order).
96
98 // As some steppers (eg RKG3) require other methods of Eq_Rhs
99 // this function allows for access to them.
100 inline void SetEquationOfMotion(G4EquationOfMotion* newEquation);
101
102 public: // without description
103
104 // Debug functions...
105
106 inline G4int GetfNoRHSCalls() { return fNoRHSCalls; }
107 void increasefNORHSCalls();
108 inline void ResetfNORHSCalls() { fNoRHSCalls = 0; }
109
110 private:
111
112 G4EquationOfMotion* fEquation_Rhs = nullptr;
113 const G4int fNoIntegrationVariables = 0; // Variables in integration
114 const G4int fNoStateVariables = 0; // Number required for FieldTrack
115
116 G4int fNoRHSCalls = 0;
117 // Debug...
118};
119
120#include "G4VFSALIntegrationStepper.icc"
121
122#endif
double G4double
Definition: G4Types.hh:83
int G4int
Definition: G4Types.hh:85
G4VFSALIntegrationStepper & operator=(const G4VFSALIntegrationStepper &)=delete
G4int GetNumberOfVariables() const
virtual ~G4VFSALIntegrationStepper()=default
virtual G4double DistChord() const =0
G4EquationOfMotion * GetEquationOfMotion()
G4VFSALIntegrationStepper(const G4VFSALIntegrationStepper &)=delete
void NormalisePolarizationVector(G4double vec[12])
void NormaliseTangentVector(G4double vec[6])
void SetEquationOfMotion(G4EquationOfMotion *newEquation)
virtual G4int IntegratorOrder() const =0
void RightHandSide(const double y[], double dydx[])
G4int GetNumberOfStateVariables() const
virtual void Stepper(const G4double y[], const G4double dydx[], G4double h, G4double yout[], G4double yerr[], G4double lastDydx[])=0