Volume 103, Issue 5, Pages (September 2012)

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Volume 103, Issue 5, Pages 1020-1027 (September 2012) The α-Helix to β-Sheet Transition in Stretched and Compressed Hydrated Fibrin Clots  Rustem I. Litvinov, Dzhigangir A. Faizullin, Yuriy F. Zuev, John W. Weisel  Biophysical Journal  Volume 103, Issue 5, Pages 1020-1027 (September 2012) DOI: 10.1016/j.bpj.2012.07.046 Copyright © 2012 Biophysical Society Terms and Conditions

Figure 1 (A) Representative FTIR spectrum of a hydrated fibrin clot and the crystallographic structure of human fibrin(ogen) (2) (inset). (B) Deconvolution of resolution-enhanced amide I band and assignment to the secondary structure elements. Biophysical Journal 2012 103, 1020-1027DOI: (10.1016/j.bpj.2012.07.046) Copyright © 2012 Biophysical Society Terms and Conditions

Figure 2 Normalized FTIR ATR spectra of unstretched plasma clot (black line) and the same clot after twofold (strain = 1, green solid line), threefold (strain = 2, red solid line), and fourfold (strain = 3, blue solid line) elongation. Corresponding difference spectra (1-0, 2-0, and 3-0) obtained by subtraction of the initial spectrum at strain = 0 are shown as the dashed lines of the corresponding color. (Inset) The absorbance intensity ratio at 1622/1651 cm−1 as a function of strain. Strain is defined as stretched length/initial length-1. Biophysical Journal 2012 103, 1020-1027DOI: (10.1016/j.bpj.2012.07.046) Copyright © 2012 Biophysical Society Terms and Conditions

Figure 3 Normalized FTIR spectra of uncompressed plasma clot (red line) and the same clot after compression (green line). The difference spectrum is shown as a black dashed line. (Inset) Changes in the amide III band. Biophysical Journal 2012 103, 1020-1027DOI: (10.1016/j.bpj.2012.07.046) Copyright © 2012 Biophysical Society Terms and Conditions

Figure 4 SEM images of unperturbed (A), fourfold stretched (B), and strongly compressed (C) fibrin clots. Magnification bar = 10 μm. Note fiber bundling both in the stretched and compressed fibrin clots. Biophysical Journal 2012 103, 1020-1027DOI: (10.1016/j.bpj.2012.07.046) Copyright © 2012 Biophysical Society Terms and Conditions

Figure 5 Reversibility of the deformation-induced changes in FTIR ATR spectra. (A) The average ratio of second derivative of absorbance intensities at 1622/1651 cm−1 in unstretched, stretched at strains 1 (n = 9) and 2 (n = 4), and relaxed fibrin clots. (Inset) Relative reversibility of the average ratio of absorbance intensities at 1622/1651 cm−1 as a function of strain. The reversibility was calculated as 100∗(average value in the stretched state – average value after relaxation)/(average value in the stretched state – average initial value). (B) The average ratio of second derivative of absorbance intensities at 1622/1651 cm−1 in uncompressed, compressed, and decompressed fibrin clots (n = 10) at various pressures. (Inset) The residual ratio of absorbance intensities at 1622/1651 cm−1 in individual decompressed fibrin clots plotted against the ratio measured in the same fibrin clots at the peak of compression. Error bars represent standard deviations. Biophysical Journal 2012 103, 1020-1027DOI: (10.1016/j.bpj.2012.07.046) Copyright © 2012 Biophysical Society Terms and Conditions