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geant4/source/geometry/magneticfield/src/G4EqGravityField.cc
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2016-06-09 16:46:55 +02:00

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//
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//
//
// This is the right-hand side for equation of motion for a
// massive particle in a gravitational field.
//
// History:
// - 14.06.11 P.Gumplinger, Created.
// -------------------------------------------------------------------
// Adopted from G4EqMagElectricField.hh
//
// Thanks to Peter Fierlinger (PSI) and
// A. Capra and A. Fontana (INFN Pavia)
// -------------------------------------------------------------------
#include "G4EqGravityField.hh"
#include "globals.hh"
void
G4EqGravityField::SetChargeMomentumMass(G4double,
G4double,
G4double particleMass )
{
fMass = particleMass;
}
void
G4EqGravityField::EvaluateRhsGivenB(const G4double y[],
const G4double G[],
G4double dydx[] ) const
{
// Components of y:
// 0-2 dr/ds,
// 3-5 dp/ds - momentum derivatives
G4double momentum_mag_square = y[3]*y[3] + y[4]*y[4] + y[5]*y[5];
G4double inv_momentum_magnitude = 1.0 / std::sqrt( momentum_mag_square );
G4double Energy = std::sqrt(momentum_mag_square + fMass*fMass);
G4double cof2 = Energy/c_light;
G4double cof1 = inv_momentum_magnitude*fMass;
G4double inverse_velocity = Energy*inv_momentum_magnitude/c_light;
dydx[0] = y[3]*inv_momentum_magnitude; // (d/ds)x = Vx/V
dydx[1] = y[4]*inv_momentum_magnitude; // (d/ds)y = Vy/V
dydx[2] = y[5]*inv_momentum_magnitude; // (d/ds)z = Vz/V
dydx[3] = G[0]*cof1*cof2;
dydx[4] = G[1]*cof1*cof2; // m*g
dydx[5] = G[2]*cof1*cof2;
// Lab Time of flight
dydx[7] = inverse_velocity;
return;
}