source: trunk/source/geometry/magneticfield/src/G4ConstRK4.cc@ 1347

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1//
2// ********************************************************************
3// * License and Disclaimer *
4// * *
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6// * the Geant4 Collaboration. It is provided under the terms and *
7// * conditions of the Geant4 Software License, included in the file *
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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 *
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23// * acceptance of all terms of the Geant4 Software license. *
24// ********************************************************************
25//
26//
27// $Id: G4ConstRK4.cc,v 1.5 2010/09/10 15:51:10 japost Exp $
28// GEANT4 tag $Name: field-V09-03-03 $
29//
30//
31// - 18.09.2008 - J.Apostolakis, T.Nikitina - Created
32// -------------------------------------------------------------------
33
34#include "G4ConstRK4.hh"
35#include "G4ThreeVector.hh"
36#include "G4LineSection.hh"
37
38//////////////////////////////////////////////////////////////////
39//
40// Constructor sets the number of *State* variables (default = 8)
41// The number of variables integrated is always 6
42
43G4ConstRK4::G4ConstRK4(G4Mag_EqRhs* EqRhs, G4int numStateVariables)
44 : G4MagErrorStepper(EqRhs, 6, numStateVariables)
45{
46 // const G4int numberOfVariables= 6;
47 if( numStateVariables < 8 )
48 {
49 G4cerr << "ERROR in G4ConstRK4::G4ConstRK4 "
50 << " The number of State variables at least 8 " << G4endl;
51 G4cerr << " Instead it is numStateVariables= " << numStateVariables << G4endl;
52 G4Exception("G4ConstRK4::G4ConstRK4()", "InvalidSetup", FatalException,
53 "Valid only for number of state variables of 8 or more. Use another Stepper!");
54 }
55
56 fEq = EqRhs;
57 yMiddle = new G4double[8];
58 dydxMid = new G4double[8];
59 yInitial = new G4double[8];
60 yOneStep = new G4double[8];
61
62 dydxm = new G4double[8];
63 dydxt = new G4double[8];
64 yt = new G4double[8];
65 Field[0]=0.; Field[1]=0.; Field[2]=0.;
66}
67
68////////////////////////////////////////////////////////////////
69//
70// Destructor
71
72G4ConstRK4::~G4ConstRK4()
73{
74 delete [] yMiddle;
75 delete [] dydxMid;
76 delete [] yInitial;
77 delete [] yOneStep;
78 delete [] dydxm;
79 delete [] dydxt;
80 delete [] yt;
81}
82
83//////////////////////////////////////////////////////////////////////
84//
85// Given values for the variables y[0,..,n-1] and their derivatives
86// dydx[0,...,n-1] known at x, use the classical 4th Runge-Kutta
87// method to advance the solution over an interval h and return the
88// incremented variables as yout[0,...,n-1], which is not a distinct
89// array from y. The user supplies the routine RightHandSide(x,y,dydx),
90// which returns derivatives dydx at x. The source is routine rk4 from
91// NRC p. 712-713 .
92
93void G4ConstRK4::DumbStepper( const G4double yIn[],
94 const G4double dydx[],
95 G4double h,
96 G4double yOut[])
97{
98 G4double hh = h*0.5 , h6 = h/6.0 ;
99
100 // 1st Step K1=h*dydx
101 yt[5] = yIn[5] + hh*dydx[5] ;
102 yt[4] = yIn[4] + hh*dydx[4] ;
103 yt[3] = yIn[3] + hh*dydx[3] ;
104 yt[2] = yIn[2] + hh*dydx[2] ;
105 yt[1] = yIn[1] + hh*dydx[1] ;
106 yt[0] = yIn[0] + hh*dydx[0] ;
107 RightHandSideConst(yt,dydxt) ;
108
109 // 2nd Step K2=h*dydxt
110 yt[5] = yIn[5] + hh*dydxt[5] ;
111 yt[4] = yIn[4] + hh*dydxt[4] ;
112 yt[3] = yIn[3] + hh*dydxt[3] ;
113 yt[2] = yIn[2] + hh*dydxt[2] ;
114 yt[1] = yIn[1] + hh*dydxt[1] ;
115 yt[0] = yIn[0] + hh*dydxt[0] ;
116 RightHandSideConst(yt,dydxm) ;
117
118 // 3rd Step K3=h*dydxm
119 // now dydxm=(K2+K3)/h
120 yt[5] = yIn[5] + h*dydxm[5] ;
121 dydxm[5] += dydxt[5] ;
122 yt[4] = yIn[4] + h*dydxm[4] ;
123 dydxm[4] += dydxt[4] ;
124 yt[3] = yIn[3] + h*dydxm[3] ;
125 dydxm[3] += dydxt[3] ;
126 yt[2] = yIn[2] + h*dydxm[2] ;
127 dydxm[2] += dydxt[2] ;
128 yt[1] = yIn[1] + h*dydxm[1] ;
129 dydxm[1] += dydxt[1] ;
130 yt[0] = yIn[0] + h*dydxm[0] ;
131 dydxm[0] += dydxt[0] ;
132 RightHandSideConst(yt,dydxt) ;
133
134 // 4th Step K4=h*dydxt
135 yOut[5] = yIn[5]+h6*(dydx[5]+dydxt[5]+2.0*dydxm[5]);
136 yOut[4] = yIn[4]+h6*(dydx[4]+dydxt[4]+2.0*dydxm[4]);
137 yOut[3] = yIn[3]+h6*(dydx[3]+dydxt[3]+2.0*dydxm[3]);
138 yOut[2] = yIn[2]+h6*(dydx[2]+dydxt[2]+2.0*dydxm[2]);
139 yOut[1] = yIn[1]+h6*(dydx[1]+dydxt[1]+2.0*dydxm[1]);
140 yOut[0] = yIn[0]+h6*(dydx[0]+dydxt[0]+2.0*dydxm[0]);
141
142} // end of DumbStepper ....................................................
143
144////////////////////////////////////////////////////////////////
145//
146// Stepper
147
148void
149G4ConstRK4::Stepper( const G4double yInput[],
150 const G4double dydx[],
151 G4double hstep,
152 G4double yOutput[],
153 G4double yError [] )
154{
155 const G4int nvar = 6; // number of variables integrated
156 const G4int maxvar= GetNumberOfStateVariables();
157
158 // Correction for Richardson extrapolation
159 G4double correction = 1. / ( (1 << IntegratorOrder()) -1 );
160
161 G4int i;
162
163 // Saving yInput because yInput and yOutput can be aliases for same array
164 for (i=0; i<maxvar; i++) { yInitial[i]= yInput[i]; }
165
166 // Must copy the part of the state *not* integrated to the output
167 for (i=nvar; i<maxvar; i++) { yOutput[i]= yInput[i]; }
168
169 // yInitial[7]= yInput[7]; // The time is typically needed
170 yMiddle[7] = yInput[7]; // Copy the time from initial value
171 yOneStep[7] = yInput[7]; // As it contributes to final value of yOutput ?
172 // yOutput[7] = yInput[7]; // -> dumb stepper does it too for RK4
173 yError[7] = 0.0;
174
175 G4double halfStep = hstep * 0.5;
176
177 // Do two half steps
178 //
179 GetConstField(yInitial,Field);
180 DumbStepper (yInitial, dydx, halfStep, yMiddle);
181 RightHandSideConst(yMiddle, dydxMid);
182 DumbStepper (yMiddle, dydxMid, halfStep, yOutput);
183
184 // Store midpoint, chord calculation
185 //
186 fMidPoint = G4ThreeVector( yMiddle[0], yMiddle[1], yMiddle[2]);
187
188 // Do a full Step
189 //
190 DumbStepper(yInitial, dydx, hstep, yOneStep);
191 for(i=0;i<nvar;i++)
192 {
193 yError [i] = yOutput[i] - yOneStep[i] ;
194 yOutput[i] += yError[i]*correction ;
195 // Provides accuracy increased by 1 order via the
196 // Richardson extrapolation
197 }
198
199 fInitialPoint = G4ThreeVector( yInitial[0], yInitial[1], yInitial[2]);
200 fFinalPoint = G4ThreeVector( yOutput[0], yOutput[1], yOutput[2]);
201
202 return;
203}
204
205////////////////////////////////////////////////////////////////
206//
207// Estimate the maximum distance from the curve to the chord
208//
209// We estimate this using the distance of the midpoint to chord.
210// The method below is good only for angle deviations < 2 pi;
211// this restriction should not be a problem for the Runge Kutta methods,
212// which generally cannot integrate accurately for large angle deviations
213
214G4double G4ConstRK4::DistChord() const
215{
216 G4double distLine, distChord;
217
218 if (fInitialPoint != fFinalPoint)
219 {
220 distLine= G4LineSection::Distline( fMidPoint, fInitialPoint, fFinalPoint );
221 // This is a class method that gives distance of Mid
222 // from the Chord between the Initial and Final points
223 distChord = distLine;
224 }
225 else
226 {
227 distChord = (fMidPoint-fInitialPoint).mag();
228 }
229 return distChord;
230}
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