Geant4 10.7.0
Toolkit for the simulation of the passage of particles through matter
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G4BogackiShampine45.hh
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1//
2// ********************************************************************
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4// * *
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6// * the Geant4 Collaboration. It is provided under the terms and *
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14// * regarding this software system or assume any liability for its *
15// * use. Please see the license in the file LICENSE and URL above *
16// * for the full disclaimer and the limitation of liability. *
17// * *
18// * This code implementation is the result of the scientific and *
19// * technical work of the GEANT4 collaboration. *
20// * By using, copying, modifying or distributing the software (or *
21// * any work based on the software) you agree to acknowledge its *
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24// ********************************************************************
25//
26// G4BogackiShampine45
27//
28// Class description:
29//
30// An implementation of the embedded RK method from the following paper
31// by P. Bogacki and L. F. Shampine:
32// "An efficient Runge-Kutta (4,5) pair"
33// Comput. Math. with Appl., vol. 32, no. 6, pp. 15-28, Sep. 1996.
34//
35// An interpolation method provides the value of an intermediate
36// point in a step -- if a step was sucessful.
37//
38// This version can provide the FSAL property of the method,
39// which allows the reuse of the last derivative in the next step,
40// but only by using the additional method GetLastDyDx() (an alternative
41// interface for simpler use of FSAL is under development).
42
43// Created: Somnath Banerjee, Google Summer of Code 2015, 25 May 2015
44// Supervision: John Apostolakis, CERN
45// --------------------------------------------------------------------
46#ifndef BOGACKI_SHAMPINE_45_HH
47#define BOGACKI_SHAMPINE_45_HH
48
50
52{
53 public:
54
56 G4int numberOfVariables = 6,
57 G4bool primary = true);
59
62
63 void Stepper( const G4double y[],
64 const G4double dydx[],
65 G4double h,
66 G4double yout[],
67 G4double yerr[] ) ;
68
69 // This Stepper provides 'dense output'. After a successful
70 // step, it is possible to obtain an estimate of the value
71 // of the function at an intermediate point of the interval.
72 // This requires only two additional evaluations of the
73 // derivative (and thus the field).
74
75 inline void SetupInterpolation()
76 {
77 SetupInterpolationHigh(); // ( yInput, dydx, Step);
78 }
79
80 // For calculating the output at the tau fraction of Step
81 //
82 inline void Interpolate( G4double tau,
83 G4double yOut[] ) // Output value
84 {
85 InterpolateHigh( tau, yOut);
86 // InterpolateHigh( yInput, dydx, Step, yOut, tau);
87 }
88
90
91 // For calculating the output at the tau fraction of Step
92 //
93 void InterpolateHigh( G4double tau,
94 G4double yOut[] ) const;
95
96 G4double DistChord() const;
97 G4int IntegratorOrder() const { return 4; }
98
99 void GetLastDydx( G4double dyDxLast[] );
100
101 void PrepareConstants(); // Initialise the values of the bi[][] array
102
103 private:
104
105 G4double *ak2, *ak3, *ak4, *ak5, *ak6, *ak7, *ak8,
106 *ak9, *ak10, *ak11, *yTemp, *yIn;
107
108 G4double *p[6];
109
110 G4double fLastStepLength = -1.0;
111 G4double *fLastInitialVector, *fLastFinalVector, *fLastDyDx,
112 *fMidVector, *fMidError;
113 // For DistChord calculations
114
115 G4BogackiShampine45* fAuxStepper = nullptr;
116 // For chord - until interpolation is proven
117 G4bool fPreparedInterpolation = false;
118
119 // Class constants
120 static G4bool fPreparedConstants;
121 static G4double bi[12][7];
122};
123
124#endif
double G4double
Definition: G4Types.hh:83
bool G4bool
Definition: G4Types.hh:86
int G4int
Definition: G4Types.hh:85
G4int IntegratorOrder() const
void Stepper(const G4double y[], const G4double dydx[], G4double h, G4double yout[], G4double yerr[])
G4BogackiShampine45(const G4BogackiShampine45 &)=delete
void GetLastDydx(G4double dyDxLast[])
void Interpolate(G4double tau, G4double yOut[])
G4double DistChord() const
void InterpolateHigh(G4double tau, G4double yOut[]) const
G4BogackiShampine45 & operator=(const G4BogackiShampine45 &)=delete