This document discusses the Lorentz force experienced by a current-carrying conductor in a magnetic field. It states that the force (F) is proportional to the current (I), length of the conductor (l), and the sine of the angle between the conductor and the magnetic field (θ). It also provides examples of calculating the force on charges moving at various angles to a magnetic field, as well as the repulsive force between two parallel current-carrying conductors. Finally, it notes that a galvanometer can be converted to an ammeter by connecting a low resistance in parallel, and to a voltmeter by connecting a high resistance in series.