Abstract
C2H4–NO, C2H4–O2 and C2H4–(CH3)2NH–O2 mixtures have been irradiated with an argon resonance lamp emitting only the 1048‐ and 1067‐Å lines. The ionization efficiency ratios: ηC2D4NO, ηC2H4NO, ηC2D4/ηC2H4 were determined to be 0.30±0.003, 0.27±0.003 and 1.12, respectively. trans‐2‐Butene and cis‐2‐butene are major products when NO (I.P.=9.25 eV) or (CH3)2NH (I.P.=8.24 eV) are added to C2H4. Radiation of pure C2H4 or of C2H4–O2 mixtures yielded only minor traces of 2‐C4H8. In accord with earlier radiolysis studies we ascribe the formation of 2‐C4H8 to the charge‐transfer process C4H8++NO (or (CH3)2NH)→C4H8+NO+ (or (CH3)2NH+), where C4H8+ may possess some excess internal energy carried over from the exothermic condensation reaction (C2H4*)++C2H4→(C4H8*)+. For a constant C2H4–NO mixture M(C4H8)/N increases drastically with an increase of the pressure of C2H4 from 0.1 to 6 torr. Also, in pure C2H4, M(CH3)/N which is close to unity at 0.5 torr is seen to diminish to 0.2 when the pressure is raised to 29.8 torr. These effects are largely ascribed to a competition between decomposition and stabilization of the [C4H8*]+ product ion. A rate constant of 107 sec−1 is derived for the unimolecular decomposition of (C4H8*)+ assuming that stabilization occurs at every collision with C2H4. It is shown that Ne is about 100 times less efficient than C2H4 in stabilizing (C4H8*)+. The superexcited C2H4* dissociates as follows, C2H4*→C2H2+H2 and C2H4*→C2H2+2H. Isotopic analysis of the hydrogen formed in the photoionization of CH2CD2 shows that the relative probabilities for the elimination of H2, HD, and D2 from CH2CD2* are the same for the superexcited molecule as for the excited molecule formed by absorption of 8.4‐ to 10‐eV photons.