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This page provides supplementary chemical data on acetone. ... vapor pressure of acetone ... NMR; Proton NMR (CDCl 3, 300 MHz) δ 2.16 (s, 6H)
Deuterated acetone ((CD 3) 2 CO), also known as acetone-d 6, is a form (isotopologue) of acetone (CH 3) 2 CO in which the hydrogen atom (H) is replaced with deuterium (heavy hydrogen) isotope (2 H or D). Deuterated acetone is a common solvent used in NMR spectroscopy. [1]
The two tautomeric forms can be distinguished by NMR spectroscopy, IR spectroscopy and other methods. [5] [6] The equilibrium constant tends to be high in nonpolar solvents; when K keto→enol is equal or greater than 1, the enol form is favoured. The keto form becomes more favourable in polar, hydrogen-bonding solvents, such as water. [7]
A 900 MHz NMR instrument with a 21.1 T magnet at HWB-NMR, Birmingham, UK Nuclear magnetic resonance spectroscopy, most commonly known as NMR spectroscopy or magnetic resonance spectroscopy (MRS), is a spectroscopic technique based on re-orientation of atomic nuclei with non-zero nuclear spins in an external magnetic field.
Chemical shifts with a different meaning appear in X-ray photoelectron spectroscopy as the shift in atomic core-level energy due to a specific chemical environment. The term is also used in Mössbauer spectroscopy, where similarly to NMR it refers to a shift in peak position due to the local chemical bonding environment. As is the case for NMR ...
Simple molecules have simple spectra. The spectrum of ethyl chloride consists of a triplet at 1.5 ppm and a quartet at 3.5 ppm in a 3:2 ratio. The spectrum of benzene consists of a single peak at 7.2 ppm due to the diamagnetic ring current. Together with carbon-13 NMR, proton NMR is a powerful tool for molecular structure characterization.
The energy of the peak is lower for aryl and unsaturated ketones. [6] Whereas 1 H NMR spectroscopy is generally not useful for establishing the presence of a ketone, 13 C NMR spectra exhibit signals somewhat downfield of 200 ppm depending on structure. Such signals are typically weak due to the absence of nuclear Overhauser effects.
The data are then processed through Fourier transformation along both the t 1 and t 2 axes, creating a 2D spectrum with peaks plotted along the diagonal and off-diagonal. When interpreting the COSY spectrum, diagonal peaks correspond to the 1D chemical shifts of individual nuclei, similar to the standard peaks in a 1D NMR spectrum.