17O and 1H NMR spectral parameters in isolated water molecules

Small amounts of water enriched in oxygen-17 were studied by 17 O and 1 H NMR in binary gaseous mixtures with Xe, Kr, CHF 3 and CH 3 F and CO 2 . The distinct linear dependences of 17 O and 1 H chemical shifts and 1 J ( 17 O, 1 H) spin-spin coupling on the density of every gas solvent were measured....

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Veröffentlicht in:Physical chemistry chemical physics : PCCP 2018-01, Vol.2 (35), p.22468-22476
Hauptverfasser: Makulski, W odzimierz, Wilczek, Marcin, Jackowski, Karol
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Wilczek, Marcin
Jackowski, Karol
description Small amounts of water enriched in oxygen-17 were studied by 17 O and 1 H NMR in binary gaseous mixtures with Xe, Kr, CHF 3 and CH 3 F and CO 2 . The distinct linear dependences of 17 O and 1 H chemical shifts and 1 J ( 17 O, 1 H) spin-spin coupling on the density of every gas solvent were measured. After the extrapolation of experimental results to zero density the relevant parameters in the isolated H 2 17 O molecule were determined. The same procedure was applied for H 2 16 O when its proton chemical shift was analyzed but the secondary isotope effect in the 1 H shielding of H 2 17 O and H 2 16 O molecules was too small for detection. As shown, all the intermolecular effects in nuclear magnetic shielding are negative and these effects are more significant for 17 O nuclei than for protons. It is consistent with the appropriate gas-to-liquid shifts of water which also indicate deshielding effects for both the investigated nuclei. On the other hand, the 1 J 0 ( 17 O, 1 H) coupling constant in H 2 17 O, which is completely free from intermolecular interactions, considerably differs from the 1 J ( 17 O, 1 H) experimental values obtained for water in liquid solutions. The present experimental data of the isolated H 2 17 O molecule are compared with selected results of shielding and spin-spin coupling calculations available from the literature and with the recent experimental data for a water molecule encapsulated in the C 60 fullerene. Additionally, on the basis of actual results the magnetic dipole moment of the 17 O nucleus is revalued for greater accuracy. Small amounts of water were studied by 17 O and 1 H NMR in binary gaseous mixtures with Xe, Kr, CHF 3 and CH 3 F and CO 2 .
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The distinct linear dependences of 17 O and 1 H chemical shifts and 1 J ( 17 O, 1 H) spin-spin coupling on the density of every gas solvent were measured. After the extrapolation of experimental results to zero density the relevant parameters in the isolated H 2 17 O molecule were determined. The same procedure was applied for H 2 16 O when its proton chemical shift was analyzed but the secondary isotope effect in the 1 H shielding of H 2 17 O and H 2 16 O molecules was too small for detection. As shown, all the intermolecular effects in nuclear magnetic shielding are negative and these effects are more significant for 17 O nuclei than for protons. It is consistent with the appropriate gas-to-liquid shifts of water which also indicate deshielding effects for both the investigated nuclei. On the other hand, the 1 J 0 ( 17 O, 1 H) coupling constant in H 2 17 O, which is completely free from intermolecular interactions, considerably differs from the 1 J ( 17 O, 1 H) experimental values obtained for water in liquid solutions. The present experimental data of the isolated H 2 17 O molecule are compared with selected results of shielding and spin-spin coupling calculations available from the literature and with the recent experimental data for a water molecule encapsulated in the C 60 fullerene. Additionally, on the basis of actual results the magnetic dipole moment of the 17 O nucleus is revalued for greater accuracy. 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The distinct linear dependences of 17 O and 1 H chemical shifts and 1 J ( 17 O, 1 H) spin-spin coupling on the density of every gas solvent were measured. After the extrapolation of experimental results to zero density the relevant parameters in the isolated H 2 17 O molecule were determined. The same procedure was applied for H 2 16 O when its proton chemical shift was analyzed but the secondary isotope effect in the 1 H shielding of H 2 17 O and H 2 16 O molecules was too small for detection. As shown, all the intermolecular effects in nuclear magnetic shielding are negative and these effects are more significant for 17 O nuclei than for protons. It is consistent with the appropriate gas-to-liquid shifts of water which also indicate deshielding effects for both the investigated nuclei. On the other hand, the 1 J 0 ( 17 O, 1 H) coupling constant in H 2 17 O, which is completely free from intermolecular interactions, considerably differs from the 1 J ( 17 O, 1 H) experimental values obtained for water in liquid solutions. The present experimental data of the isolated H 2 17 O molecule are compared with selected results of shielding and spin-spin coupling calculations available from the literature and with the recent experimental data for a water molecule encapsulated in the C 60 fullerene. Additionally, on the basis of actual results the magnetic dipole moment of the 17 O nucleus is revalued for greater accuracy. 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The distinct linear dependences of 17 O and 1 H chemical shifts and 1 J ( 17 O, 1 H) spin-spin coupling on the density of every gas solvent were measured. After the extrapolation of experimental results to zero density the relevant parameters in the isolated H 2 17 O molecule were determined. The same procedure was applied for H 2 16 O when its proton chemical shift was analyzed but the secondary isotope effect in the 1 H shielding of H 2 17 O and H 2 16 O molecules was too small for detection. As shown, all the intermolecular effects in nuclear magnetic shielding are negative and these effects are more significant for 17 O nuclei than for protons. It is consistent with the appropriate gas-to-liquid shifts of water which also indicate deshielding effects for both the investigated nuclei. On the other hand, the 1 J 0 ( 17 O, 1 H) coupling constant in H 2 17 O, which is completely free from intermolecular interactions, considerably differs from the 1 J ( 17 O, 1 H) experimental values obtained for water in liquid solutions. The present experimental data of the isolated H 2 17 O molecule are compared with selected results of shielding and spin-spin coupling calculations available from the literature and with the recent experimental data for a water molecule encapsulated in the C 60 fullerene. Additionally, on the basis of actual results the magnetic dipole moment of the 17 O nucleus is revalued for greater accuracy. Small amounts of water were studied by 17 O and 1 H NMR in binary gaseous mixtures with Xe, Kr, CHF 3 and CH 3 F and CO 2 .</abstract><cop>Cambridge</cop><pub>Royal Society of Chemistry</pub><doi>10.1039/c8cp01748d</doi><tpages>9</tpages></addata></record>
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source Royal Society Of Chemistry Journals; Alma/SFX Local Collection
subjects Buckminsterfullerene
Chemical equilibrium
Coupling
Coupling (molecular)
Density
Dipole moments
Fullerenes
Isotope effect
Magnetic dipoles
Magnetic shielding
Mathematical analysis
NMR
Nuclear magnetic resonance
Nuclei (nuclear physics)
Organic chemistry
Oxygen enrichment
Parameters
Water chemistry
title 17O and 1H NMR spectral parameters in isolated water molecules
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