It has been shown that the approximate solutions of the Fredholm integral equation for the scattering amplitude obtained by demanding that ${f}_{\mathrm{out}={f}_{\mathrm{in}={\ensuremath{\lambda}}_{p}}}$,n${\mathrm{f}}_{\mathrm{Bn}}$ on the mass shell in the integral equation (where ${f}_{\mathrm{Bn}}$ is the scattering amplitude in the nth Born approximation, n and p are nonzero positive integers, and ${\ensuremath{\lambda}}_{p}$,n is a scattering-angle- and energy-dependent complex multiplying factor) are identical to those obtained from the Schwinger variational principle with incoming and outgoing trial wave functions which are correct to (p-1)th and (n-1)th order in the interaction potential in a Born approximation. Further, the scattering amplitude obtained from the Schwinger variational principle, with outgoing and incoming scattering waves correct up to first order in the interaction potential in the Born approximation, has been employed to calculate total collisional cross sections for ${e}^{\ifmmode\pm\else\textpm\fi{}}$-H scattering in the 20--500-eV energy range. The results are in good agreement with the adopted cross section of de Heer et al. and those obtained in the modified Glauber approximation and the [2,2] Pad\'e approximant for E\ensuremath{\ge}30 eV.