Joseph John Thomson,
Rays of Positive Electricity and Their Application to Chemical Analyses…
(1913)
“ If b is the length of the plates measured parallel to the axis of x, and if one end of the plates just comes up to the point from which the particle is projected, putting Z=Z from x=0 to x=b, and Z=0 fromx= b to x=l, we find that so that If z is the deflection when x=l The electric field Is not absolutely constant between the plates, It is greater close to the edges than in other parts of the field, nor it absolutely vanish at all places outside the plates ”
