The theory developed in Part I is applied to a number of typical deflection fields such as the fields produced by parallel plates, parallel cylinders, semi‐infinite co‐planar sheets, and bent‐plates. Graphs for the magnitude of deflection are given. An electrolytic tank potential‐plotting device is described which was used for the determination of the potential distribution of some of the deflection fields.The theory shows that the deflection is a function of the initial conditions of the electron beam before entering the field and that it is a slightly non‐linear function of the field strength. It follows that the fluorescent spot and the pattern produced on the screen of cathode‐ray tubes will show distortions. These distortions were calculated for several deflection fields and electron beam shapes; the results are shown graphically.The problem of the reduction of these distortion effects is discussed.