Protein Structure and Hydration Probed by SANS and Osmotic Stress

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Protein Structure and Hydration Probed by SANS and Osmotic Stress Christopher Stanley, Susan Krueger, V. Adrian Parsegian, Donald C. Rau  Biophysical Journal  Volume 94, Issue 7, Pages 2777-2789 (April 2008) DOI: 10.1529/biophysj.107.122697 Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 1 SDS-PAGE of E. coli expressed and purified yeast guanylate kinase (lane 1) and a protein standards ladder (lane 2). Gels were stained with SYPRO Orange. Biophysical Journal 2008 94, 2777-2789DOI: (10.1529/biophysj.107.122697) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 2 SANS profiles of lysozyme at 5.5mg/mL in D2O with no solute and in the presence of 8% PEG 400. For easier comparison, the SANS intensity is normalized by the scattering at zero angle, I(Q)/I(0). The protein appears smaller with added solute; Guinier fits to these curves yield radii of gyration Rg=13.3±0.1 Å and 12.7±0.1 Å for no solute and 8% PEG 400, respectively. Biophysical Journal 2008 94, 2777-2789DOI: (10.1529/biophysj.107.122697) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 3 Lysozyme Rg determined by SANS and the zero-angle neutron scattering intensity ratio with and without solute, Is(0)/I0(0), both as a function of solute volume fraction, fv, for (A) glycine betaine, (B) TEG, (C) PEG of molecular weight 400, and (D) PEG 1000. Solid lines are fits made to Rg with a composite model (Eqs. 3 and 4) to calculate the amount of protein-associated water, Nw, and dashed lines show the expected intensity ratio dependence on fv based on the Rg fits. Biophysical Journal 2008 94, 2777-2789DOI: (10.1529/biophysj.107.122697) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 4 (A) Experimental SANS from ligand-free GK, the enzyme complex with GMP, and the ternary complex GK/GMP/ADP at 5mg/mL in D2O (data points) and SANS profiles calculated from the corresponding crystal structures using Xtal2sas (solid lines). Curves are shifted for clarity. (B) The corresponding guanylate kinase crystal structures: 1, GK, 1EX6; 2, GK/GMP, 1EX7; and 3, GK/GMP/MgADP, 1LVG. Biophysical Journal 2008 94, 2777-2789DOI: (10.1529/biophysj.107.122697) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 5 SANS profiles for GK at 5mg/mL in D2O with no solute and in the presence of 8% PEG 400. For comparison, the SANS intensity is normalized by the scattering at zero angle, I(Q)/I(0). The protein appears smaller with added solute; Guinier fits to these curves yield Rg=17.0±0.1Å and 16.0±0.2Å for no solute and 8% PEG 400, respectively. Biophysical Journal 2008 94, 2777-2789DOI: (10.1529/biophysj.107.122697) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 6 Contrast variation for GK by H2O/D2O and solute/D2O. Plotted is the square root of the zero-angle scattering intensity, Is0Mp/cpNA1/2, versus bulk solution scattering-length density, ρ0. (Inset) Detailed view of the solute/D2O contrast variation region. The different slopes from the H2O/D2O contrast variation line with added solutes are attributed to protein-associated water. Biophysical Journal 2008 94, 2777-2789DOI: (10.1529/biophysj.107.122697) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 7 (A) The GK zero-angle neutron scattering intensity ratio, Is(0)/I0(0), as a function of solute volume fraction, fv. Solid lines are fits using Eq. 2. (B) Measured change in GK Rg versus solute fv. Dashed lines are given for glycerol and PEG 1000 to guide the eye. Glycerol has a negligible effect on GK Rg, whereas the effects of the other solutes become more pronounced according to their size. Glycerol has greater access to the water molecules within the GK cavity, whereas the other solutes are partially excluded. Biophysical Journal 2008 94, 2777-2789DOI: (10.1529/biophysj.107.122697) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 8 Models of GK with (A) 319 associated water molecules located uniformly around the protein surface, (B) 808 waters around the protein surface and filling the binding cavity, and (C) 250 waters localized within the protein cavity. Protein is cyan and water oxygen atoms are red. The models were created using VMD and the coordinates were used for calculating Rg values and SANS Is(Q) profiles with changing bulk-solution scattering-length density. Biophysical Journal 2008 94, 2777-2789DOI: (10.1529/biophysj.107.122697) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 9 (A) Calculated Rg values for the GK-water models shown in Fig. 8. Bulk-solution scattering-length density was varied according to solute fv, with TEG as the solute for the Nw=319 model (Fig. 8 A) and PEG 400 for the models with Nw=808 (Fig. 8 B) and Nw=250 (Fig. 8 C). (B) Calculated SANS profiles for the GK-water model incorporating 808 waters (Fig. 8 B) and with contrast variation by added PEG 400. Biophysical Journal 2008 94, 2777-2789DOI: (10.1529/biophysj.107.122697) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 10 Calorimetric heat of GMP binding versus [GMP]/[GK] ratio, both without solute and with 20% PEG 400. Corresponding background titrations of GMP into buffer also are shown (open symbols). Biophysical Journal 2008 94, 2777-2789DOI: (10.1529/biophysj.107.122697) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 11 (A) Osmotic stress effects on GMP binding to GK. The slope of the curves is proportional to the change in hydration, ΔNw, accompanying ligand binding. (B) Osmotic stress effects on ADP binding to GK in the presence of Mg2+ and in the presence and absence of GMP. Biophysical Journal 2008 94, 2777-2789DOI: (10.1529/biophysj.107.122697) Copyright © 2008 The Biophysical Society Terms and Conditions

Figure 12 Compensation between the enthalpic, ΔH, and entropic, TΔS, contributions to GK ligand binding in the presence of solutes. The different ligand-binding experiments and solutes used are plotted together and give a slope, d(ΔH)/d(TΔS)=0.98±0.02. Biophysical Journal 2008 94, 2777-2789DOI: (10.1529/biophysj.107.122697) Copyright © 2008 The Biophysical Society Terms and Conditions