Microwave Spectrum, Structure, and Dipole Moment of Difluorophosphine Borane
dc.contributor.author | Pasinski, John P. | en_US |
dc.contributor.author | Kuczkowski, Robert L. | en_US |
dc.date.accessioned | 2010-05-06T23:36:35Z | |
dc.date.available | 2010-05-06T23:36:35Z | |
dc.date.issued | 1971-03-01 | en_US |
dc.identifier.citation | Pasinski, John P.; Kuczkowski, Robert L. (1971). "Microwave Spectrum, Structure, and Dipole Moment of Difluorophosphine Borane." The Journal of Chemical Physics 54(5): 1903-1908. <http://hdl.handle.net/2027.42/71354> | en_US |
dc.identifier.uri | https://hdl.handle.net/2027.42/71354 | |
dc.description.abstract | The structure of difluorophosphine borane (HF2P☒BH3) has been determined from the microwave spectra of six isotopic species. The expected staggered conformation and CsCs symmetry have been confirmed. The structural parameters are: d(PH) = 1.409 ± 0.004Å;d(PF) = 1.552 ± 0.006Å;d(PB) = 1.832 ± 0.009Å;d(BHa) = 1.226 ± 0.005Å;d(BHs) = 1.200 ± 0.007Å;∠HaBHa = 112.7 ± 0.5°;∠HaBHs = 115.9 ± 0.4°;∠FPF = 100.0 ± 0.5°;∠FPH = 98.62 ± 0.25°;∠BPF = 117.7 ± 0.3°d(PH)=1.409±0.004Å;d(PF)=1.552±0.006Å;d(PB)=1.832±0.009Å;d(BHa)=1.226±0.005Å;d(BHs)=1.200±0.007Å;∠HaBHa=112.7±0.5°;∠HaBHs=115.9±0.4°;∠FPF=100.0±0.5°;∠FPH=98.62±0.25°;∠BPF=117.7±0.3°. Two angles (PBHs = 109.9 ± 0.3°;PBHa = 99.89 ± 0.26°)(PBHs=109.9±0.3°;PBHa=99.89±0.26°) indicate a tilt of the borane group away from the fluorine atoms. The value of the dipole moment obtained from Stark splittings is 2.504 ± 0.030 D. A range for the barrier to internal rotation is estimated as 3600–4500 cal/mole. The change in structural parameters of HF2PBH3 compared to similar compounds, the stability of HF2PBH3 towards dissociation, and the tilted borane group are discussed. | en_US |
dc.format.extent | 3102 bytes | |
dc.format.extent | 415722 bytes | |
dc.format.mimetype | text/plain | |
dc.format.mimetype | application/pdf | |
dc.publisher | The American Institute of Physics | en_US |
dc.rights | © The American Institute of Physics | en_US |
dc.title | Microwave Spectrum, Structure, and Dipole Moment of Difluorophosphine Borane | en_US |
dc.type | Article | en_US |
dc.subject.hlbsecondlevel | Physics | en_US |
dc.subject.hlbtoplevel | Science | en_US |
dc.description.peerreviewed | Peer Reviewed | en_US |
dc.contributor.affiliationum | Department of Chemistry, The University of Michigan, Ann Arbor, Michigan 48104 | en_US |
dc.description.bitstreamurl | http://deepblue.lib.umich.edu/bitstream/2027.42/71354/2/JCPSA6-54-5-1903-1.pdf | |
dc.identifier.doi | 10.1063/1.1675116 | en_US |
dc.identifier.source | The Journal of Chemical Physics | en_US |
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dc.identifier.citedreference | (a) Bartell and Su, employing extended Hückel MO calculations, have also pointed out that HF2PHF2P and F3PF3P behave anomalously.15b They showed that the bonded overlap populations normally increased when more electronegative groups were attached to phosphorous except in the case of the PO overlaps in HF2POHF2PO vs F3PO.F3PO. The EHMO calculations by us on HF2P‐BH3HF2P‐BH3 and F3P‐BH3F3P‐BH3 resulted in a slightly greater P‐B bond overlap population for HF2P‐BH3HF2P‐BH3 vs F3PBH3(<1%).F3PBH3(<1%). In contrast to the mechanism suggested in the text, the σ and π contributions in both molecules were essentially the same. (b) L. S. Bartell, S. L. Su, and H. Yow, Inorg. Chem. 9, 1903 (1970). | en_US |
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dc.owningcollname | Physics, Department of |
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