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Volumn 125, Issue 43, 2003, Pages 13219-13224

Experimental Evidence for a Temperature Dependent Transition between Normal and Inverse Equilibrium Isotope Effects for Oxidative Addition of H 2 to Ir(PMe2Ph)2(CO)Cl

Author keywords

[No Author keywords available]

Indexed keywords

EQUILIBRIUM ISOTOPE EFFECTS (EIE);

EID: 0142244912     PISSN: 00027863     EISSN: None     Source Type: Journal    
DOI: 10.1021/ja0362611     Document Type: Article
Times cited : (37)

References (60)
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  • 13
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    • Isotope Methods in Homogeneous Catalysis
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  • 15
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    • note
    • For other examples of situations in which there is a temperature-dependent transition between a normal and inverse EIE, see ref 2.
  • 24
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    • The symmetry factor includes both external (σ) and internal (n) symmetry numbers. See: Bailey, W. F.; Monahan, A. S. J. Chem. Educ. 1978, 55, 489-493.
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  • 32
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    • ref 3a and 4a
    • (c) ref 3a and 4a.
  • 33
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    • note
    • Application of the Teller-Redlich product rule permits the MMI term to be replaced by the vibrational product (VP) derived from the vibrational frequencies. See ref 13.
  • 34
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    • note
    • The EIE at 300 K is 0.57 in good agreement to the value of 0.46 calculated by Krogh-Jespersen and Goldman (ref 3a).
  • 35
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    • note
    • rot, the rotational temperature. The EIE data presented here are obtained by treating the rotational and nuclear partition functions classically. Consideration of quantum effects serves to modify the [SYM · MMI · EXC] (entropy) term at low temperature, but has no effect on the low-temperature limit of the EIE which is dominated by the ZPE (enthalpy) term.
  • 36
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    • note
    • It should be noted that the ZPE and enthalpy [exp(-ΔΔH/RT)] terms are not identical because the thermal population of vibrationally excited states also provides a contribution to the enthalpy term. Correspondingly, the [SYM · MMI · EXC] and entropy [exp(ΔΔS/R)] terms are not identical, but differ by a similar component to that relating ZPE and enthalpy. However, these differences are small such that ZPE ≈ [exp(-ΔΔH/RT)] and [SYM · MMI · EXC] ≈ [exp(ΔΔS/R)] are good approximations. For example, at 100 K, ZPE = 0.002 and [exp(-ΔΔH/RT)] = 0.002, whereas SYM · MMI · EXC = 5.48, and exp(ΔΔS/R) = 5.48; at 1000 K, ZPE = 0.542 and [exp(-ΔΔH/RT)] = 0.547, whereas SYM · MMI · EXC = 2.12, and exp(ΔΔS/R) = 2.11.
  • 37
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    • note
    • EXC is unity at 0 K, and so [SYM · MMI · EXC] = [SYM · MMI]
  • 38
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    • note
    • 2)] = 2.04 e.u.
  • 39
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    • note
    • 2)] = 1.36 e.u.
  • 40
  • 45
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    • Lide, D. R., Ed.; CRC Press: Boca Raton
    • 2 in the absence of contributions from nuclear spin statistics is 3.4 e.u. See ref 18 and Handbook of Chemistry and Physics, 72nd ed.; Lide, D. R., Ed.; CRC Press: Boca Raton 1991; p 5-35.
    • (1991) Handbook of Chemistry and Physics, 72nd Ed. , pp. 5-35
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    • toluene = -2047.3/T + 8.330. See: Handbook of Chemistry and Physics, 72nd ed.; Lide, D. R., Ed.; CRC Press: Boca Raton 1991; p 6-84.
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    • 2 in benzene: In x = -5.6949-765.47/(T/K). See: Clever, H. L. In Solubility Data Series; Young, C. L., Ed.; Pergamon Press: Oxford, 1981; Volume 5/6: Hydrogen and Deuterium, p 164.
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    • note
    • 2) has reacted.
  • 51
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    • note
    • The van't Hoff plot does not include the high-temperature data due to the deviation from ideal behavior at high temperature (see text).
  • 52
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    • Young, C. L., Ed.; Pergamon Press: Oxford: Hydrogen and Deuterium
    • 2 in benzene: In x = -5.7399-743.44/(T/K). See: Clever, H. L. In Solubility Data Series; Young, C. L., Ed.; Pergamon Press: Oxford, 1981; Volume 5/6: Hydrogen and Deuterium, p 287.
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    • 2 in toluene: In x = -6.0373-603.07/(T/K). See: Clever, H. L. In Solubility Data Series; Young, C. L., Ed.; Pergamon Press: Oxford, 1981; Volume 5/6: Hydrogen and Deuterium, p 169.
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    • 2 in toluene: In x = -6.0781-580.52/(T/K). See: Clever, H. L. In Solubility Data Series; Young, C. L., Ed.; Pergamon Press: Oxford, 1981; Volume 5/6: Hydrogen and Deuterium, p 288.
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.