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geant4/source/geometry/magneticfield/src/G4EqMagElectricField.cc
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2016-06-10 11:51:14 +02:00

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// $Id: G4EqMagElectricField.cc 69699 2013-05-13 08:50:30Z gcosmo $
//
//
// This is the standard right-hand side for equation of motion.
//
// The only case another is required is when using a moving reference
// frame ... or extending the class to include additional Forces,
// eg an electric field
//
// 10.11.98 V.Grichine
//
// -------------------------------------------------------------------
#include "G4EqMagElectricField.hh"
#include "globals.hh"
#include "G4PhysicalConstants.hh"
#include "G4SystemOfUnits.hh"
void
G4EqMagElectricField::SetChargeMomentumMass(G4ChargeState particleCharge,
G4double,
G4double particleMass)
{
G4double pcharge = particleCharge.GetCharge();
fElectroMagCof = eplus*pcharge*c_light ;
fMassCof = particleMass*particleMass ;
}
void
G4EqMagElectricField::EvaluateRhsGivenB(const G4double y[],
const G4double Field[],
G4double dydx[] ) const
{
// Components of y:
// 0-2 dr/ds,
// 3-5 dp/ds - momentum derivatives
G4double pSquared = y[3]*y[3] + y[4]*y[4] + y[5]*y[5] ;
G4double Energy = std::sqrt( pSquared + fMassCof );
G4double cof2 = Energy/c_light ;
G4double pModuleInverse = 1.0/std::sqrt(pSquared) ;
// G4double inverse_velocity = Energy * c_light * pModuleInverse;
G4double inverse_velocity = Energy * pModuleInverse / c_light;
G4double cof1 = fElectroMagCof*pModuleInverse ;
// G4double vDotE = y[3]*Field[3] + y[4]*Field[4] + y[5]*Field[5] ;
dydx[0] = y[3]*pModuleInverse ;
dydx[1] = y[4]*pModuleInverse ;
dydx[2] = y[5]*pModuleInverse ;
dydx[3] = cof1*(cof2*Field[3] + (y[4]*Field[2] - y[5]*Field[1])) ;
dydx[4] = cof1*(cof2*Field[4] + (y[5]*Field[0] - y[3]*Field[2])) ;
dydx[5] = cof1*(cof2*Field[5] + (y[3]*Field[1] - y[4]*Field[0])) ;
dydx[6] = 0.;//not used
// Lab Time of flight
dydx[7] = inverse_velocity;
return ;
}