In Fig. 23-48a, an electron is shot directly away from a uniformly charged plastic sheet, at speed v_s = 2.0 × 10^5 m/s. The sheet is nonconducting, flat, and very large. Figure 23-48b gives the electron’s vertical velocity component v versus time t until the return to the launch point. What is the sheet’s surface charge density?
The field due to the sheet is E=\frac{\sigma}{2 \varepsilon_0} . The force (in magnitude) on the electron (due to that field) is F = eE, and assuming it’s the only force then the acceleration is
a=\frac{e \sigma}{2 \varepsilon_0 m}=\text { slope of the graph }\left(=2.0 \times 10^5 \,m / s \text { divided by } 7.0 \times 10^{-12}\, s \right) \text {. }
Thus we obtain \sigma=2.9 \times 10^{-6}\, C / m ^2 .