Salem Faham

Heparin structure and interactions with basic fibroblast growth factor.

Crystal structures of heparin-derived tetra- and hexasaccharides complexed with basic fibroblast growth factor (bFGF) were determined at resolutions of 1.9 and 2.2 angstroms, respectively. The heparin structure may be approximated as a helical polymer with a disaccharide rotation of 174° and a translation of 8.6 angstroms along the helix axis. Both molecules bound similarly to a region of the bFGF surface containing residues asparagine-28, arginine-121, lysine-126, and glutamine-135; the hexasaccharide also interacted with an additional binding site formed by lysine-27, asparagine-102, and lysine-136. No significant conformational change in bFGF occurred upon heparin oligosaccharide binding, which suggests that heparin primarily serves to juxtapose components of the FGF signal transduction pathway.

The Crystal Structure of a Sodium Galactose Transporter Reveals Mechanistic Insights into Na+/Sugar Symport

Membrane transporters that use energy stored in sodium gradients to drive nutrients into cells constitute a major class of proteins. We report the crystal structure of a member of the solute sodium symporters (SSS), the Vibrio parahaemolyticus sodium/galactose symporter (vSGLT). The ∼3.0 angstrom structure contains 14 transmembrane (TM) helices in an inward-facing conformation with a core structure of inverted repeats of 5 TM helices (TM2 to TM6 and TM7 to TM11). Galactose is bound in the center of the core, occluded from the outside solutions by hydrophobic residues. Surprisingly, the architecture of the core is similar to that of the leucine transporter (LeuT) from a different gene family. Modeling the outward-facing conformation based on the LeuT structure, in conjunction with biophysical data, provides insight into structural rearrangements for active transport.

The crystal structure of mouse VDAC1 at 2.3 Å resolution reveals mechanistic insights into metabolite gating

The voltage-dependent anion channel (VDAC) constitutes the major pathway for the entry and exit of metabolites across the outer membrane of the mitochondria and can serve as a scaffold for molecules that modulate the organelle. We report the crystal structure of a β-barrel eukaryotic membrane protein, the murine VDAC1 (mVDAC1) at 2.3 Å resolution, revealing a high-resolution image of its architecture formed by 19 β-strands. Unlike the recent NMR structure of human VDAC1, the position of the voltage-sensing N-terminal segment is clearly resolved. The α-helix of the N-terminal segment is oriented against the interior wall, causing a partial narrowing at the center of the pore. This segment is ideally positioned to regulate the conductance of ions and metabolites passing through the VDAC pore.

Polymerization of the SAM domain of TEL in leukemogenesis and transcriptional repression

TEL is a transcriptional repressor that is a frequent target of chromosomal translocations in a large number of hematalogical malignancies. These rearrangements fuse a potent oligomerization module, the SAM domain of TEL, to a variety of tyrosine kinases or transcriptional regulatory proteins. The self‐associating property of TEL–SAM is essential for cell transformation in many, if not all of these diseases. Here we show that the TEL–SAM domain forms a helical, head‐to‐tail polymeric structure held together by strong intermolecular contacts, providing the first clear demonstration that SAM domains can polymerize. Our results also suggest a mechanism by which SAM domains could mediate the spreading of transcriptional repression complexes along the chromosome.

Modest stabilization by most hydrogen-bonded side-chain interactions in membrane proteins.

Understanding the energetics of molecular interactions is fundamental to all of the central quests of structural biology including structure prediction and design, mapping evolutionary pathways, learning how mutations cause disease, drug design, and relating structure to function. Hydrogen-bonding is widely regarded as an important force in a membrane environment because of the low dielectric constant of membranes and a lack of competition from water. Indeed, polar residue substitutions are the most common disease-causing mutations in membrane proteins. Because of limited structural information and technical challenges, however, there have been few quantitative tests of hydrogen-bond strength in the context of large membrane proteins. Here we show, by using a double-mutant cycle analysis, that the average contribution of eight interhelical side-chain hydrogen-bonding interactions throughout bacteriorhodopsin is only 0.6 kcal mol-1. In agreement with these experiments, we find that 4% of polar atoms in the non-polar core regions of membrane proteins have no hydrogen-bond partner and the lengths of buried hydrogen bonds in soluble proteins and membrane protein transmembrane regions are statistically identical. Our results indicate that most hydrogen-bond interactions in membrane proteins are only modestly stabilizing. Weak hydrogen-bonding should be reflected in considerations of membrane protein folding, dynamics, design, evolution and function.

Diversity Does Make a Difference: Fibroblast Growth Factor-Heparin Interactions

Fibroblast growth factors (FGFs) are members of a protein family with a broad range of biological activities. The best characterized FGFs interact with two distinct extracellular receptors--a transmembrane tyrosine kinase FGF receptor (FGFR) and a heparan f1p4ate-related proteoglycan of the extracellular matrix. These components form a FGF-FGFR-proteoglycan complex that activates the FGF-mediated signal transduction process through FGFR dimerization. Recent crystal structure determinations of FGF-heparin complexes have provided insights into both the interactions between these components and the role of heparin-like proteoglycans in FGF function. Future advances in this field will benefit enormously from an ability to specifically prepare homogeneous heparin-based oligosaccharides of defined sequence for use in biochemical and structural studies of FGF and many other systems.

Crystallization of bacteriorhodopsin from bicelle formulations at room temperature.

We showed previously that high‐quality crystals of bacteriorhodopsin (bR) from Halobacterium salinarum can be obtained from bicelle‐forming DMPC/CHAPSO mixtures at 37°C. As many membrane proteins are not sufficiently stable for crystallization at this high temperature, we tested whether the bicelle method could be applied at a lower temperature. Here we show that bR can be crystallized at room temperature using two different bicelle‐forming compositions: DMPC/CHAPSO and DTPC/CHAPSO. The DTPC/CHAPSO crystals grown at room temperature are essentially identical to the previous, twinned crystals: space group P21 with unit cell dimensions of a = 44.7 Å, b = 108.7 Å, c = 55.8 Å, β = 113.6°. The room‐temperature DMPC/CHAPSO crystals are untwinned, however, and belong to space group C2221 with the following unit cell dimensions: a = 44.7 Å, b = 102.5 Å, c = 128.2 Å. The bR protein packs into almost identical layers in the two crystal forms, but the layers stack differently. The new untwinned crystal form yielded clear density for a previously unresolved CHAPSO molecule inserted between protein subunits within the layers. The ability to grow crystals at room temperature significantly expands the applicability of bicelle crystallization.

How to Prepare Membrane Proteins for Solid-State NMR: A Case Study on the α-Helical Integral Membrane Protein Diacylglycerol Kinase from E. coli

Several studies have demonstrated that it is viable to use microcrystalline preparations of water‐soluble proteins as samples in solid‐state NMR experiments. 1 – 5 Here, we investigate whether this approach holds any potential for studying water‐insoluble systems, namely membrane proteins. For this case study, we have prepared proteoliposomes and small crystals of the α‐helical membrane‐protein diacylglycerol kinase (DGK). Preparations were characterised by 13C‐ and 15N‐cross‐polarization magic‐angle spinning (CPMAS) NMR. It was found that crystalline samples produce better‐resolved spectra than proteoliposomes. This makes them more suitable for structural NMR experiments. However, reconstitution is the method of choice for biophysical studies by solid‐state NMR. In addition, we discuss the identification of lipids bound to membrane‐protein crystals by 31P‐MAS NMR.

Construction of helix-bundle membrane proteins.

Publisher Summary This chapter presents some of the current understanding of the structure of α-helical membrane proteins and the forces that stabilize their structures. It focuses on the folding and stability of membrane proteins within the bilayer rather than on the thermodyamics of helix insertion into the membrane. It is not possible to point to a force that dominates in the construction of helix bundle membrane proteins. Hydrogen bonds can be extremely strong, but are relatively sparse and are not critical for the development of stable helix-helix interactions. Van der Waals interactions are certainly important, but the fact that a well-packed leucine zipper interface is not sufficient to drive TM helix association suggests that packing alone is not enough. Although the complex interplay between lipid structure and protein structure must play an important role, the fact that many membrane proteins remain folded and functional in detergent micelles suggests that lipid structure alone cannot entirely explain membrane protein architecture.

Native interface of the SAM domain polymer of TEL

BackgroundTEL is a transcriptional repressor containing a SAM domain that forms a helical polymer. In a number of hematologic malignancies, chromosomal translocations lead to aberrant fusions of TEL-SAM to a variety of other proteins, including many tyrosine kinases. TEL-SAM polymerization results in constitutive activation of the tyrosine kinase domains to which it becomes fused, leading to cell transformation. Thus, inhibitors of TEL-SAM self-association could abrogate transformation in these cells. In previous work, we determined the structure of a mutant TEL-SAM polymer bearing a Val to Glu substitution in center of the subunit interface. It remained unclear how much the mutation affected the architecture of the polymer, however.ResultsHere we determine the structure of the native polymer interface. To accomplish this goal, we introduced mutations that block polymer extension, producing a heterodimer with a wild-type interface. We find that the structure of the wild-type polymer interface is quite similar to the mutant structure determined previously. With the structure of the native interface, it is possible to evaluate the potential for developing therapeutic inhibitors of the interaction. We find that the interacting surfaces of the protein are relatively flat, containing no obvious pockets for the design of small molecule inhibitors.ConclusionOur results confirm the architecture of the TEL-SAM polymer proposed previously based on a mutant structure. The fact that the interface contains no obvious potential binding pockets suggests that it may be difficult to find small molecule inhibitors to treat malignancies in this way.