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geant4/source/geometry/magneticfield/src/G4ClassicalRK4.cc
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//
// ********************************************************************
// * DISCLAIMER *
// * *
// * The following disclaimer summarizes all the specific disclaimers *
// * of contributors to this software. The specific disclaimers,which *
// * govern, are listed with their locations in: *
// * http://cern.ch/geant4/license *
// * *
// * 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. *
// * *
// * This code implementation is the intellectual property of the *
// * GEANT4 collaboration. *
// * By copying, distributing or modifying the Program (or any work *
// * based on the Program) you indicate your acceptance of this *
// * statement, and all its terms. *
// ********************************************************************
//
//
// $Id: G4ClassicalRK4.cc,v 1.8 2003/06/16 16:51:11 gunter Exp $
// GEANT4 tag $Name: geant4-05-02 $
//
#include "G4ClassicalRK4.hh"
#include "G4ThreeVector.hh"
//////////////////////////////////////////////////////////////////
//
// Constructor sets the number of variables (default = 6)
G4ClassicalRK4::G4ClassicalRK4(G4Mag_EqRhs *EqRhs, G4int numberOfVariables)
: G4MagErrorStepper(EqRhs, numberOfVariables)
// fNumberOfVariables(numberOfVariables)
{
unsigned int noVariables= std::max(numberOfVariables,8); // For Time .. 7+1
dydxm = new G4double[noVariables];
dydxt = new G4double[noVariables];
yt = new G4double[noVariables];
}
////////////////////////////////////////////////////////////////
//
// Destructor
G4ClassicalRK4::~G4ClassicalRK4()
{
delete[] dydxm;
delete[] dydxt;
delete[] yt;
}
//////////////////////////////////////////////////////////////////////
//
// Given values for the variables y[0,..,n-1] and their derivatives
// dydx[0,...,n-1] known at x, use the classical 4th Runge-Kutta
// method to advance the solution over an interval h and return the
// incremented variables as yout[0,...,n-1], which not be a distinct
// array from y. The user supplies the routine RightHandSide(x,y,dydx),
// which returns derivatives dydx at x. The source is routine rk4 from
// NRC p. 712-713 .
void
G4ClassicalRK4::DumbStepper( const G4double yIn[],
const G4double dydx[],
G4double h,
G4double yOut[])
{
const G4int nvar = this->GetNumberOfVariables(); // fNumberOfVariables();
G4int i;
G4double hh = h*0.5 , h6 = h/6.0 ;
// Initialise time to t0, needed when it is not updated by the integration.
// [ Note: Only for time dependent fields (usually electric)
// is it neccessary to integrate the time.]
yt[7] = yIn[7];
yOut[7] = yIn[7];
for(i=0;i<nvar;i++)
{
yt[i] = yIn[i] + hh*dydx[i] ; // 1st Step K1=h*dydx
}
RightHandSide(yt,dydxt) ; // 2nd Step K2=h*dydxt
for(i=0;i<nvar;i++)
{
yt[i] = yIn[i] + hh*dydxt[i] ;
}
RightHandSide(yt,dydxm) ; // 3rd Step K3=h*dydxm
for(i=0;i<nvar;i++)
{
yt[i] = yIn[i] + h*dydxm[i] ;
dydxm[i] += dydxt[i] ; // now dydxm=(K2+K3)/h
}
RightHandSide(yt,dydxt) ; // 4th Step K4=h*dydxt
for(i=0;i<nvar;i++) // Final RK4 output
{
yOut[i] = yIn[i]+h6*(dydx[i]+dydxt[i]+2.0*dydxm[i]); //+K1/6+K4/6+(K2+K3)/3
}
// NormaliseTangentVector( yOut );
return ;
} // end of DumbStepper ....................................................
////////////////////////////////////////////////////////////////////
//
//
void
G4ClassicalRK4::StepWithEst( const G4double*,
const G4double*,
G4double,
G4double*,
G4double&,
G4double&,
const G4double*,
G4double* )
{
G4Exception("ERROR - G4ClassicalRK4::StepWithEst(): method no longer used.");
return ;
} // end of StepWithEst ......................................................