Total Collision Cross Sections for the Interaction of Molecular Beams of Cesium Chloride with Gases. Influence of the Dipole-Dipole Force upon the Scattering

Total cross sections (Q) for the interaction of beams of CsCl with a number of molecules were measured using an apparatus of ca 4′ angular resolution in which the temperature of the scattering gas could be varied from 200°—735°K. The temperature dependence of Q was studied for Ar, CH4, CH2F2, CHF3,...

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Veröffentlicht in:Journal of Chemical Physics (U.S.) 1960-08, Vol.33 (2), p.584-590
Hauptverfasser: Schumacher, Hugo, Bernstein, Richard B., Rothe, Erhard W.
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container_title Journal of Chemical Physics (U.S.)
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creator Schumacher, Hugo
Bernstein, Richard B.
Rothe, Erhard W.
description Total cross sections (Q) for the interaction of beams of CsCl with a number of molecules were measured using an apparatus of ca 4′ angular resolution in which the temperature of the scattering gas could be varied from 200°—735°K. The temperature dependence of Q was studied for Ar, CH4, CH2F2, CHF3, CF4, NO, H2S, NH3, and for cis- and trans-CHCl=CHCl. Relative values of Q at 300°K were measured for eight additional gases. The data were correlated using the Massey-Mohr theory, assuming an intermolecular potential V(r) = —C/r6, so that Q=b(C/vr)2/5, where vr is the relative velocity and b a known constant; the potential constant C was estimated from formulas for the dispersion, dipole-induced dipole, and dipole-dipole forces. For the nonpolar gases the observed small temperature dependence of Q agrees within experimental error (±3%) with that expected from the temperature dependence of vr. The theoretical values of Q differ by a nearly constant factor from the experimental results; thus relative cross sections (Q*) are predicted with fair accuracy. For the polar gases the Q's are large, decreasing significantly with increasing temperature. Because of the large dipole-dipole interaction, the approximate theoretical treatment (based on the limiting temperature-dependent dipole-dipole contribution to C) accounts only semiquantitatively for the observations.
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The data were correlated using the Massey-Mohr theory, assuming an intermolecular potential V(r) = —C/r6, so that Q=b(C/vr)2/5, where vr is the relative velocity and b a known constant; the potential constant C was estimated from formulas for the dispersion, dipole-induced dipole, and dipole-dipole forces. For the nonpolar gases the observed small temperature dependence of Q agrees within experimental error (±3%) with that expected from the temperature dependence of vr. The theoretical values of Q differ by a nearly constant factor from the experimental results; thus relative cross sections (Q*) are predicted with fair accuracy. For the polar gases the Q's are large, decreasing significantly with increasing temperature. 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For the nonpolar gases the observed small temperature dependence of Q agrees within experimental error (±3%) with that expected from the temperature dependence of vr. The theoretical values of Q differ by a nearly constant factor from the experimental results; thus relative cross sections (Q*) are predicted with fair accuracy. For the polar gases the Q's are large, decreasing significantly with increasing temperature. 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Influence of the Dipole-Dipole Force upon the Scattering</atitle><jtitle>Journal of Chemical Physics (U.S.)</jtitle><date>1960-08-01</date><risdate>1960</risdate><volume>33</volume><issue>2</issue><spage>584</spage><epage>590</epage><pages>584-590</pages><issn>0021-9606</issn><eissn>1089-7690</eissn><abstract>Total cross sections (Q) for the interaction of beams of CsCl with a number of molecules were measured using an apparatus of ca 4′ angular resolution in which the temperature of the scattering gas could be varied from 200°—735°K. The temperature dependence of Q was studied for Ar, CH4, CH2F2, CHF3, CF4, NO, H2S, NH3, and for cis- and trans-CHCl=CHCl. Relative values of Q at 300°K were measured for eight additional gases. The data were correlated using the Massey-Mohr theory, assuming an intermolecular potential V(r) = —C/r6, so that Q=b(C/vr)2/5, where vr is the relative velocity and b a known constant; the potential constant C was estimated from formulas for the dispersion, dipole-induced dipole, and dipole-dipole forces. For the nonpolar gases the observed small temperature dependence of Q agrees within experimental error (±3%) with that expected from the temperature dependence of vr. The theoretical values of Q differ by a nearly constant factor from the experimental results; thus relative cross sections (Q*) are predicted with fair accuracy. For the polar gases the Q's are large, decreasing significantly with increasing temperature. Because of the large dipole-dipole interaction, the approximate theoretical treatment (based on the limiting temperature-dependent dipole-dipole contribution to C) accounts only semiquantitatively for the observations.</abstract><doi>10.1063/1.1731189</doi><tpages>7</tpages><oa>free_for_read</oa></addata></record>
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ispartof Journal of Chemical Physics (U.S.), 1960-08, Vol.33 (2), p.584-590
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subjects AMMONIA
ANGULAR DISTRIBUTION
ARGON
BEAMS
CESIUM CHLORIDES
CHLORINATED HYDROCARBONS
CROSS SECTIONS
DIPOLES
ELECTRIC POTENTIAL
FLUORINATED HYDROCARBONS
GASES
INTERACTIONS
MEASURED VALUES
METHANE
MOLECULES
NITROGEN OXIDES
PHYSICS
RESOLUTION
SCATTERING
SULFUR COMPOUNDS
TEMPERATURE
VELOCITY
title Total Collision Cross Sections for the Interaction of Molecular Beams of Cesium Chloride with Gases. Influence of the Dipole-Dipole Force upon the Scattering
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