Volume 108, Issue 7, Pages (April 2015)

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Presentation transcript:

Volume 108, Issue 7, Pages 1758-1772 (April 2015) 13C, 2H NMR Studies of Structural and Dynamical Modifications of Glucose-Exposed Porcine Aortic Elastin  Moshe C. Silverstein, Kübra Bilici, Steven W. Morgan, Yunjie Wang, Yanhang Zhang, Gregory S. Boutis  Biophysical Journal  Volume 108, Issue 7, Pages 1758-1772 (April 2015) DOI: 10.1016/j.bpj.2015.02.005 Copyright © 2015 Biophysical Society Terms and Conditions

Figure 1 Representative plots of Cauchy stress versus true strain of untreated (UT) and glucose-treated (GT) elastin in the longitudinal (L) and circumferential (C) directions. Note that the Cauchy stress versus true strain curves for the glucose-treated sample overlap for both the longitudinal and circumferential directions and are therefore not labeled. Biophysical Journal 2015 108, 1758-1772DOI: (10.1016/j.bpj.2015.02.005) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 2 Averaged Cauchy stress versus true strain of untreated (UT) and glucose-treated (GT) elastin (n = 7) in the longitudinal (L) and circumferential (C) directions. One-sided error bars represent one standard deviation. ∗p < 0.05. Biophysical Journal 2015 108, 1758-1772DOI: (10.1016/j.bpj.2015.02.005) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 3 DP 13C NMR spectra of hydrated untreated (A1 and B1) and hydrated glucose-treated (A2 and B2) porcine aortic elastin samples. The peaks between 60 and 80 ppm in the glucose-treated samples arise from the glucose solution. Spectra correspond to the aliphatic region (B1 and B2) and the carbonyl region (A1 and A2). Differences are observed in the resolution of the various peaks between the samples, as discussed in the text. Note the different vertical scales. Biophysical Journal 2015 108, 1758-1772DOI: (10.1016/j.bpj.2015.02.005) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 4 CP 13C NMR spectra of hydrated untreated (A1 and B1) and hydrated glucose-treated (A2 and B2) porcine aortic elastin samples. The peaks between 60 and 80 ppm in the glucose-treated samples arise from the glucose solution. Spectra correspond to the aliphatic region (B1 and B2) and the carbonyl region (A1 and A2). Differences are observed in the resolution of the various peaks between the samples as discussed in the text. Note the different vertical scales. Biophysical Journal 2015 108, 1758-1772DOI: (10.1016/j.bpj.2015.02.005) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 5 T1-T2 results from untreated (A) and glucose-treated (B) porcine aortic elastin at 37°C (intensity, indicated by the colorbar at right, is shown on a logarithmic scale). Four distinguishable peaks are observed in each sample, denoted by α1, α2, β, and γ. Differences in the relative populations of water in the assigned γ and β regions are observed between the samples, as discussed in the text. The numerical values of the T1 and T2 times and the relative intensities are provided in Table 4. To see this figure in color, go online. Biophysical Journal 2015 108, 1758-1772DOI: (10.1016/j.bpj.2015.02.005) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 6 Ramachandran angles for the samples in water (a, c, and e) and 2 M glucose (b, d, and f). Samples included AAAAA (a and b), desmosine with alanine (c and d), and isodesmosine residues with alanine (e and f) (alanine Ramachandran angles are shown). The angles were calculated using the final 1 ns of the 20 ns simulations (images are shown in color). Note that for AAAAA in glucose, there is a change or increase from β-spiral to α-helical, consistent with the experimental NMR results. A schematic representation of the desmosine and isodesmosine molecules used in the simulations is shown in Fig. S1. To see this figure in color, go online. Biophysical Journal 2015 108, 1758-1772DOI: (10.1016/j.bpj.2015.02.005) Copyright © 2015 Biophysical Society Terms and Conditions