1997
DOI: 10.1021/ja972553o
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1H, 13C, 15N NMR and Ab Initio/IGLO/GIAO-MP2 Study of Mono-, Di-, Tri-, and Tetraprotonated Guanidine1

Abstract: Mono- and diprotonated guanidines were prepared in superacid solutions and studied by 1H, 13C, and 15N NMR spectroscopy. The structures, energies, and NMR chemical shifts were also calculated by ab initio/IGLO/GIAO-MP2 method. Excellent agreement were found between experimental and calculated 13C and 15N NMR chemical shifts. No persistent triprotonated guanidine was observed. Tri- and tetraprotonated guanidines were also studied by ab initio/IGLO/GIAO-MP2 method.

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Cited by 50 publications
(41 citation statements)
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References 15 publications
(36 reference statements)
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“…The global minimum does not reflect the experimental result of the X-ray structure analysisb ecause this ion does not have ap lanar geometry.T he local minimum, however,e xhibits planar geometry and is in good agreementw ith the crystal structure of 4.T his phenomenon has already been reported. [17,28] The energetic difference between the globala nd local minima is 0.284 kJ mol À1 .D ue to the very small energetic difference and the improved agreement with our experimental results, we used the structure with ap lanar geometry for the calculations of the molecular orbitals. We assumeaplanar geometry would be accessible only through simulation of the solid-state interactions.T herefore, we suggest that the high stabilityo ft he guanidinium(1 +)c ation does not depend on either electron delocalization or hydrogen-bonding interactions, buti saproduct of both properties together.…”
Section: Theoretical Calculationsmentioning
confidence: 72%
See 1 more Smart Citation
“…The global minimum does not reflect the experimental result of the X-ray structure analysisb ecause this ion does not have ap lanar geometry.T he local minimum, however,e xhibits planar geometry and is in good agreementw ith the crystal structure of 4.T his phenomenon has already been reported. [17,28] The energetic difference between the globala nd local minima is 0.284 kJ mol À1 .D ue to the very small energetic difference and the improved agreement with our experimental results, we used the structure with ap lanar geometry for the calculations of the molecular orbitals. We assumeaplanar geometry would be accessible only through simulation of the solid-state interactions.T herefore, we suggest that the high stabilityo ft he guanidinium(1 +)c ation does not depend on either electron delocalization or hydrogen-bonding interactions, buti saproduct of both properties together.…”
Section: Theoretical Calculationsmentioning
confidence: 72%
“…[27] The geometry of the guanidinium(2 +) cation is also consistent with resultso faprevious study from 1997 when the calculated and predicted geometries of the dication were comparedt oe xperimental and calculated 1 H, 13 C, and 15 Nc hemical shifts. [28] Furthermore, the protons were found in the differenceF ouriers ynthesis and were refinedi sotropically.…”
Section: Vibrational Spectra Of 1-3mentioning
confidence: 99%
“…Actually, if −44.1 ppm is the absolute shielding ( σ ), it can be transformed into the corresponding chemical shift ( δ , ppm) by means of the equation δ 13 C = 175.7 – 0.963 σ 13 C, affording 218 ppm. The measured value is 157 ppm , but the transformation equation was established to B3LYP/6‐311++G(d,p) calculations. Note that 157 ppm is a value typical for a C = N, for instance, of hydrazones .…”
Section: Resultsmentioning
confidence: 99%
“…[24] We therefore chose to compare the signal of our products with the signal of the commercial products thiourea, Smethylisopseudothiourea hemisulfate salt and S-methylisopseudothiourea. In the spectrum of DDSTU/HCl-13 C 1a C13 (figure 4, A) the peak at 183 ppm could then be attributed to the thiourea function ( fig.…”
Section: Methodsmentioning
confidence: 99%