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geant4/source/geometry/magneticfield/include/G4VFSALIntegrationStepper.icc
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// G4VFSALIntegrationStepper inline methods implementation
//
// Author: Somnath Banerjee (CERN, Google Summer of Code 2015), 26.05.2016
// Supervision: John Apostolakis (CERN)
// --------------------------------------------------------------------
inline
G4EquationOfMotion* G4VFSALIntegrationStepper::GetEquationOfMotion()
{
return fEquation_Rhs;
}
inline void
G4VFSALIntegrationStepper::SetEquationOfMotion(G4EquationOfMotion* newEquation)
{
if( newEquation != nullptr )
{
fEquation_Rhs = newEquation;
}
}
inline
G4int G4VFSALIntegrationStepper::GetNumberOfVariables() const
{
return fNoIntegrationVariables;
}
inline
G4int G4VFSALIntegrationStepper::GetNumberOfStateVariables() const
{
return fNoStateVariables;
}
inline
void G4VFSALIntegrationStepper::NormaliseTangentVector( G4double vec[6] )
{
G4double drds2 = vec[3]*vec[3]+vec[4]*vec[4]+vec[5]*vec[5];
if( std::fabs(drds2 - 1.0) > 1.e-14 )
{
G4double normx = 1.0 / std::sqrt(drds2);
for(auto i=3; i<6; ++i) { vec[i] *= normx; }
}
}
inline
void G4VFSALIntegrationStepper::NormalisePolarizationVector( G4double vec[12] )
{
G4double drds2 = vec[9]*vec[9]+vec[10]*vec[10]+vec[11]*vec[11];
if( drds2 > 0. )
{
if( std::fabs(drds2 - 1.0) > 1.e-14 )
{
G4double normx = 1.0 / std::sqrt(drds2);
for(auto i=9; i<12; ++i) { vec[i] *= normx; }
}
}
}