Publication

Carbon-13 NMR spectra of lignins. 9. Spin-lattice relaxation times (T1) and determination of interunit linkages in three hardwood lignins (Alnus glutinosa, Corylus avellanus and Acer pseudoplatanus)

Manfred Schlosser
1982
Journal Articles

Abstract

The spin-lattice relaxation time (T1) for the aliph. C atoms in the C3 side chains of acetylated MWL from C. avellana was below 0.5 s, while C atoms of substituted arom. carbonyl and Me in methoxy and Ac groups lead to T1 values ranging between 1 and 3 s as detd. by the progressive satn. pulse Fourier transform technique. The 13C NMR spectroscopy off acetylated MWL from A. glutinosa, C. avellana and A. pseudoplatanus permitted tracing 5 interunite linkages in each lignin. [on SciFinder (R)]

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https://infoscience.epfl.ch/entities/publication/19308ce4-e940-4b18-9a01-b84b56012dc8

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Manfred Schlosser
1982
Journal Articles

Abstract

Official source

https://infoscience.epfl.ch/entities/publication/19308ce4-e940-4b18-9a01-b84b56012dc8

About this result

Related concepts (20)

Nuclear magnetic resonance spectroscopy

Nuclear magnetic resonance spectroscopy, most commonly known as NMR spectroscopy or magnetic resonance spectroscopy (MRS), is a spectroscopic technique to observe local magnetic fields around atomic nuclei. This spectroscopy is based on the measurement of absorption of electromagnetic radiations in the radio frequency region from roughly 4 to 900 MHz. Absorption of radio waves in the presence of magnetic field is accompanied by a special type of nuclear transition, and for this reason, such type of spectroscopy is known as Nuclear Magnetic Resonance Spectroscopy.

Spin–spin relaxation

In physics, the spin–spin relaxation is the mechanism by which Mxy, the transverse component of the magnetization vector, exponentially decays towards its equilibrium value in nuclear magnetic resonance (NMR) and magnetic resonance imaging (MRI). It is characterized by the spin–spin relaxation time, known as T2, a time constant characterizing the signal decay. It is named in contrast to T1, the spin–lattice relaxation time.

Spin–lattice relaxation

During nuclear magnetic resonance observations, spin–lattice relaxation is the mechanism by which the longitudinal component of the total nuclear magnetic moment vector (parallel to the constant magnetic field) exponentially relaxes from a higher energy, non-equilibrium state to thermodynamic equilibrium with its surroundings (the "lattice"). It is characterized by the spin–lattice relaxation time, a time constant known as T1.

Related publications (2)

Carbon-13 NMR spectra of lignins. 9. Spin-lattice relaxation times (T1) and determination of interunit linkages in three hardwood lignins (Alnus glutinosa, Corylus avellanus and Acer pseudoplatanus)

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Field-induced quasi-bound state within the two-magnon continuum of a square-lattice Heisenberg antiferromagnet

Proton chemical shift anisotropy: detection of cross correlation with dipole-dipole interactions by double-quantum filtered two-dimensional NMR exchange spectroscopy