With ψ(0)=ζ, ψ′(d)=0 and no slip at either wall, linear screening gives ψ/ζ=cosh[κ(d−x)]/cosh(κd). The velocity is v/U=1−(1−sechκd)x/d−cosh[κ(d−x)]/cosh(κd). This electrically neutral-wall boundary assumes no external normal field; it differs from a grounded wall.