G4ClassicalRK4.cc

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00026 //
00027 // $Id: G4ClassicalRK4.cc 69786 2013-05-15 09:38:51Z gcosmo $
00028 //
00029 // -------------------------------------------------------------------
00030 
00031 #include "G4ClassicalRK4.hh"
00032 #include "G4ThreeVector.hh"
00033 
00035 //
00036 // Constructor sets the number of variables (default = 6)
00037 
00038 G4ClassicalRK4::
00039 G4ClassicalRK4(G4EquationOfMotion* EqRhs, G4int numberOfVariables)
00040   : G4MagErrorStepper(EqRhs, numberOfVariables)
00041 {
00042    unsigned int noVariables= std::max(numberOfVariables,8); // For Time .. 7+1
00043  
00044    dydxm = new G4double[noVariables];
00045    dydxt = new G4double[noVariables]; 
00046    yt    = new G4double[noVariables]; 
00047 }
00048 
00050 //
00051 // Destructor
00052 
00053 G4ClassicalRK4::~G4ClassicalRK4()
00054 {
00055   delete[] dydxm;
00056   delete[] dydxt;
00057   delete[] yt;
00058 }
00059 
00061 //
00062 // Given values for the variables y[0,..,n-1] and their derivatives
00063 // dydx[0,...,n-1] known at x, use the classical 4th Runge-Kutta
00064 // method to advance the solution over an interval h and return the
00065 // incremented variables as yout[0,...,n-1], which not be a distinct
00066 // array from y. The user supplies the routine RightHandSide(x,y,dydx),
00067 // which returns derivatives dydx at x. The source is routine rk4 from
00068 // NRC p. 712-713 .
00069 
00070 void
00071 G4ClassicalRK4::DumbStepper( const G4double  yIn[],
00072                              const G4double  dydx[],
00073                                    G4double  h,
00074                                    G4double  yOut[])
00075 {
00076   const G4int nvar = this->GetNumberOfVariables();   //  fNumberOfVariables(); 
00077   G4int i;
00078   G4double  hh = h*0.5 , h6 = h/6.0  ;
00079 
00080   // Initialise time to t0, needed when it is not updated by the integration.
00081   //        [ Note: Only for time dependent fields (usually electric) 
00082   //                  is it neccessary to integrate the time.] 
00083   yt[7]   = yIn[7]; 
00084   yOut[7] = yIn[7];
00085 
00086   for(i=0;i<nvar;i++)
00087   {
00088     yt[i] = yIn[i] + hh*dydx[i] ;             // 1st Step K1=h*dydx
00089   }
00090   RightHandSide(yt,dydxt) ;                   // 2nd Step K2=h*dydxt
00091 
00092   for(i=0;i<nvar;i++)
00093   { 
00094     yt[i] = yIn[i] + hh*dydxt[i] ;
00095   }
00096   RightHandSide(yt,dydxm) ;                   // 3rd Step K3=h*dydxm
00097 
00098   for(i=0;i<nvar;i++)
00099   {
00100     yt[i]   = yIn[i] + h*dydxm[i] ;
00101     dydxm[i] += dydxt[i] ;                    // now dydxm=(K2+K3)/h
00102   }
00103   RightHandSide(yt,dydxt) ;                   // 4th Step K4=h*dydxt
00104  
00105   for(i=0;i<nvar;i++)    // Final RK4 output
00106   {
00107     yOut[i] = yIn[i]+h6*(dydx[i]+dydxt[i]+2.0*dydxm[i]); //+K1/6+K4/6+(K2+K3)/3
00108   }
00109   if ( nvar == 12 )  { NormalisePolarizationVector ( yOut ); }
00110   
00111 }  // end of DumbStepper ....................................................
00112 
00114 //
00115 // StepWithEst
00116 
00117 void
00118 G4ClassicalRK4::StepWithEst( const G4double*,
00119                              const G4double*,
00120                                    G4double,
00121                                    G4double*,
00122                                    G4double&,
00123                                    G4double&,
00124                              const G4double*,
00125                                    G4double*  ) 
00126 {
00127   G4Exception("G4ClassicalRK4::StepWithEst()", "GeomField0001",
00128               FatalException, "Method no longer used.");
00129 
00130 }  // end of StepWithEst ......................................................
00131 

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