By R.J. Anderson, D. Bendell, P W. Groundwater, Edward W. Abel

ISBN-10: 0854044760

ISBN-13: 9780854044764

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Approximately 50% of the nuclei will be aligned “with” and 50% of the nuclei will be aligned “against” the magnetic field. Therefore we always attempt to conduct NMR experiments at the highest frequency possible; since the value for y is constant for a given nucleus, we do this by making the strength of the main magnetic field ( B ) as large as we can. ). 1) contains the term B e E rather than B. This is called the chemical shift effect, and to understand this key aspect of NMR spectra we need to consider what happens when we place our NMR sample in a magnetic field.

16a) and, as expected for intramolecular hydrogen bonding, is independent of concentration (1 64 1 cm- '). 15b has shifted the broad 0-H absorption to lower wavenumber (from 3330 to 3320 cm-'), but the absorption corresponding to nonhydrogen-bonded 0-H at 3584 cm-' is unaffected. 3. As can be observed, the smaller the ring becomes, the more strained the ring (as the bond angles become increasingly removed Infrared Spectroscopy 41 from the idealized angle of 120" for an sp2 hybridized carbon atom and the amount of eclipsing interactions with neighbouring groups increases), and the higher the stretching frequency of the carbonyl group in both the lactones and lactams.

A great deal of effort has gone into the design of modern NMR probes to make them as efficient as possible in terms of the signulto-noise ratio, through having the shortest distance possible between the sample and the receiver coil. In addition to being able to spin the sample within the coil, there are also variable-temperature units built into most NMR probes so that, if NMR data are required at different temperatures, a heated or cooled stream of gas can easily be passed over the NMR sample.

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Organic spectroscopic analysis by R.J. Anderson, D. Bendell, P W. Groundwater, Edward W. Abel

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