## 2. Analysis of forces in a rotating reference frameUsually the motion of a particle along rotating magnetic field lines is treated in the bead-on-the-wire approximation where a bead is assumed to follow the rotating field line and experiences centrifugal acceleration (or deceleration) while moving in the outward direction (e.g. Machabeli & Rogava 1994; Chedia et al. 1996; Cao 1997). This simple approach yields interesting results, though, as we will show further below, such an approximation breaks down in the region near the light cylinder. Let us consider the forces acting on a particle in a rotating frame
of reference (Gangadhara 1996; Gangadhara & Lesch 1997).
A particle with rest mass where is the Lorentz factor of the particle and is the angular velocity of the field. Additionally, there is also a relativistic Coriolis force in the noninertial frame governed by the equation which acts as a deviation-force in the azimuthal direction. In the inertial rest frame the particle sees the field line bending off from its initial injection position. Hence, it experiences a Lorentz force, which may be written as where is the relative velocity between the particle and the magnetic field line and where the convention is used. Due to the Lorentz force a charged particle tries to gyrate around the magnetic field line. Initially, the direction of the Lorentz force is perpendicular to the direction of the Coriolis force, but as a particle gyrates, it changes direction and eventually becomes antiparallel to the Coriolis force. Hence one expects that the bead-on-the-wire approximation holds, if the Lorentz force is not balanced by the Coriolis force. In this case, the accelerated motion of the particle's guiding center due to the centrifugal force is given by where © European Southern Observatory (ESO) 2000 Online publication: December 17, 1999 |