Abstract

Total cross sections have been measured for the scattering of Ar beams from perpendicular intersecting beams of N2, Ne, He, and H2. The beams were at 300°K and contained Maxwellian velocity distributions. The slit system approximated ideal slits, and the scattering-center density was calculated from rate-of-flow measurements and a modification of the usual beam-intensity equations. In addition, beams of He and H2 were scattered from an intersecting beam of Ar. Beam reversal reduced the angular-resolution correction to less than 1%. The background scattering of the primary beam could be estimated without recourse to pressure-gauge readings. Comparison of the experimental results was made with the Schiff—Landau—Lifshitz formula and calculations with the partial-wave WKB approximation with an assumed Lennard-Jones (12, 6) potential. The L-J total cross sections do not agree with the experimental results for Ar–He and Ar–H2 systems. The L-J angular-resolution corrections do not bring the beam-reversal measurements in line with the measurements with Ar as the scattering gas.

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