Assume for the directions and parametrizations; the boost formulas retain their signed meaning for reversed fields. A Lorentz boost with velocity along transforms the transverse electric field and magnetic field as
In the electric-dominated case choose
The inequality ensures , so this is an inertial frame. The field-removing boosts for perpendicular electric and magnetic fields are governed by the electromagnetic field invariants and explain why a purely electric inertial frame exists and a purely magnetic one does not.
The electron is not initially at rest in this convenient inertial frame: its initial velocity is and its initial three-momentum is . Thereafter , while stays constant. The electric field accelerates it toward ; as its relativistic energy increases, its negative transverse velocity decreases in magnitude. Defining and gives a useful parametric world line:
Here is the proper time. These formulas follow by integrating , , and constant . Its projection onto the plane is a hyperbola, but the spatial trajectory includes the initial transverse motion and is not a straight line.
Transforming back with , gives
The laboratory trajectory starts from rest toward , then bends toward . It is unbounded in and ultimately has and . Thus the late velocity has magnitude as a limit, consistent with the relativistic energy-momentum relation, rather than undergoing a closed cyclotron orbit.
Figure 1.
Electron trajectories in electric-dominated and magnetic-dominated crossed fields
. Original parametric spatial trajectories in the convenient inertial frame and laboratory, with dimensionless units . Arrows show increasing time. The initial transverse motion in the purely electric frame and the laboratory cusps in the purely magnetic case are visible. Details.

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