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. Author manuscript; available in PMC: 2015 Oct 1.
Published in final edited form as: J Magn Reson. 2014 Sep 9;247:81–87. doi: 10.1016/j.jmr.2014.08.014

Figure 2.

Figure 2

(A) Frequency dependence of 1/T1 ( ) for 25DTBSQ in ethanol at 293 K. The relaxation is modeled as the sum (- -, short dash) of contributions from spin rotation (SR) (—, solid) Eq. (2), a local mode (local) (— —, long dash) Eq. (3), modulation of g-anisotropy (g) (— - - -, dash dot) Eq. (5) and modulation of dipolar interactions with solvent nuclei (solvent) (– –, medium dash) Eq. (8). (B) Frequency dependence of 1/T1 in C2H5OH ( ), in CH3OH (x), in C2H5OD (○) and in C2D5OD (▷). The dashed lines through the data are the sums of contributions to the spin lattice relaxation as described in the text, calculated with Eq. 2, 3, 5, and 8.