Geant4 11.1.1
Toolkit for the simulation of the passage of particles through matter
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G4ClassicalRK4.cc
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1//
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24// ********************************************************************
25//
26// G4ClassicalRK4 implementation
27//
28// Created: J.Apostolakis, V.Grichine - 30.01.1997
29// -------------------------------------------------------------------
30
31#include "G4ClassicalRK4.hh"
32#include "G4ThreeVector.hh"
33
34//////////////////////////////////////////////////////////////////
35//
36// Constructor sets the number of variables (default = 6)
37//
39G4ClassicalRK4(G4EquationOfMotion* EqRhs, G4int numberOfVariables)
40 : G4MagErrorStepper(EqRhs, numberOfVariables)
41{
42 unsigned int noVariables= std::max(numberOfVariables,8); // For Time .. 7+1
43
44 dydxm = new G4double[noVariables];
45 dydxt = new G4double[noVariables];
46 yt = new G4double[noVariables];
47}
48
49////////////////////////////////////////////////////////////////
50//
51// Destructor
52//
54{
55 delete [] dydxm;
56 delete [] dydxt;
57 delete [] yt;
58}
59
60//////////////////////////////////////////////////////////////////////
61//
62// Given values for the variables y[0,..,n-1] and their derivatives
63// dydx[0,...,n-1] known at x, use the classical 4th Runge-Kutta
64// method to advance the solution over an interval h and return the
65// incremented variables as yout[0,...,n-1], which not be a distinct
66// array from y. The user supplies the routine RightHandSide(x,y,dydx),
67// which returns derivatives dydx at x. The source is routine rk4 from
68// NRC p. 712-713 .
69//
70void
72 const G4double dydx[],
73 G4double h,
74 G4double yOut[])
75{
76 const G4int nvar = GetNumberOfVariables(); // fNumberOfVariables();
77 G4int i;
78 G4double hh = h*0.5, h6 = h/6.0;
79
80 // Initialise time to t0, needed when it is not updated by the integration.
81 // [ Note: Only for time dependent fields (usually electric)
82 // is it neccessary to integrate the time.]
83 yt[7] = yIn[7];
84 yOut[7] = yIn[7];
85
86 for(i=0; i<nvar; ++i)
87 {
88 yt[i] = yIn[i] + hh*dydx[i] ; // 1st Step K1=h*dydx
89 }
90 RightHandSide(yt,dydxt) ; // 2nd Step K2=h*dydxt
91
92 for(i=0; i<nvar; ++i)
93 {
94 yt[i] = yIn[i] + hh*dydxt[i] ;
95 }
96 RightHandSide(yt,dydxm) ; // 3rd Step K3=h*dydxm
97
98 for(i=0; i<nvar; ++i)
99 {
100 yt[i] = yIn[i] + h*dydxm[i] ;
101 dydxm[i] += dydxt[i] ; // now dydxm=(K2+K3)/h
102 }
103 RightHandSide(yt,dydxt) ; // 4th Step K4=h*dydxt
104
105 for(i=0; i<nvar; ++i) // Final RK4 output
106 {
107 yOut[i] = yIn[i]+h6*(dydx[i]+dydxt[i]+2.0*dydxm[i]); //+K1/6+K4/6+(K2+K3)/3
108 }
109 if ( nvar == 12 ) { NormalisePolarizationVector ( yOut ); }
110
111} // end of DumbStepper ....................................................
112
113////////////////////////////////////////////////////////////////////
114//
115// StepWithEst
116
117void
118G4ClassicalRK4::StepWithEst( const G4double*,
119 const G4double*,
120 G4double,
121 G4double*,
122 G4double&,
123 G4double&,
124 const G4double*,
125 G4double* )
126{
127 G4Exception("G4ClassicalRK4::StepWithEst()", "GeomField0001",
128 FatalException, "Method no longer used.");
129
130} // end of StepWithEst ......................................................
@ FatalException
void G4Exception(const char *originOfException, const char *exceptionCode, G4ExceptionSeverity severity, const char *description)
Definition: G4Exception.cc:59
double G4double
Definition: G4Types.hh:83
int G4int
Definition: G4Types.hh:85
void DumbStepper(const G4double yIn[], const G4double dydx[], G4double h, G4double yOut[])
G4ClassicalRK4(G4EquationOfMotion *EquationMotion, G4int numberOfVariables=6)
void NormalisePolarizationVector(G4double vec[12])
G4int GetNumberOfVariables() const
void RightHandSide(const G4double y[], G4double dydx[]) const