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Abstract

2.1 NMR Master EquationTo apply (2.8) the linear frequency has to be transformed into angular frequency:

$$\gamma = \frac{2\pi \nu } {{B}_{0}} = \frac{2\pi \,200.13 \times 1{0}^{6}\,\mathrm{Hz}} {4.7\,\mathrm{T}} = 2.675 \times 1{0}^{8}\,{\mathrm{rad\,s}}^{-1}\,{T}^{-1}.$$

For other nuclei see list of constants on p. xviii.

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Notes

  1. 1.

    sinc(0) = 1 as can be seen from l’Hospital’s rule.

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Correspondence to Edme H. Hardy .

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© 2012 Springer-Verlag Berlin Heidelberg

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Hardy, E.H. (2012). Solutions. In: NMR Methods for the Investigation of Structure and Transport. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-21628-2_5

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