RESUMEN
Fibroblast growth factors (FGFs) effect cellular responses by binding to FGF receptors (FGFRs). FGF bound to extracellular domains on the FGFR in the presence of heparin activates the cytoplasmic receptor tyrosine kinase through autophosphorylation. We have crystallized a complex between human FGF1 and a two-domain extracellular fragment of human FGFR2. The crystal structure, determined by multiwavelength anomalous diffraction analysis of the selenomethionyl protein, is a dimeric assemblage of 1:1 ligand:receptor complexes. FGF is bound at the junction between the two domains of one FGFR, and two such units are associated through receptor:receptor and secondary ligand:receptor interfaces. Sulfate ion positions appear to mark the course of heparin binding between FGF molecules through a basic region on receptor D2 domains. This dimeric assemblage provides a structural mechanism for FGF signal transduction.
Asunto(s)
Factor 2 de Crecimiento de Fibroblastos/química , Proteínas Tirosina Quinasas Receptoras/química , Receptores de Factores de Crecimiento de Fibroblastos/química , Secuencia de Aminoácidos , Sitios de Unión , Cristalización , Bases de Datos Factuales , Dimerización , Factor 1 de Crecimiento de Fibroblastos , Heparina/química , Humanos , Ligandos , Modelos Moleculares , Datos de Secuencia Molecular , Unión Proteica , Conformación Proteica , Proteínas/química , Receptor Tipo 2 de Factor de Crecimiento de Fibroblastos , Selenometionina/química , Selenoproteínas , Alineación de Secuencia , Transducción de Señal , Difracción de Rayos XRESUMEN
The fibroblast growth factors (FGFs) form a large family of structurally related, multifunctional proteins that regulate various biological responses. They mediate cellular functions by binding to transmembrane FGF receptors, which are protein tyrosine kinases. FGF receptors are activated by oligomerization, and both this activation and FGF-stimulated biological responses require heparin-like molecules as well as FGF. Heparins are linear anionic polysaccharide chains; they are typically heterogeneously sulphated on alternating L-iduronic and D-glucosamino sugars, and are nearly ubiquitous in animal tissues as heparan sulphate proteoglycans on cell surfaces and in the extracellular matrix. Although several crystal structures have been described for FGF molecules in complexes with heparin-like sugars, the nature of a biologically active complex has been unknown until now. Here we describe the X-ray crystal structure, at 2.9 A resolution, of a biologically active dimer of human acidic FGF in a complex with a fully sulphated, homogeneous heparin decassacharide. The dimerization of heparin-linked acidic FGF observed here is an elegant mechanism for the modulation of signalling through combinatorial homodimerization and heterodimerization of the 12 known members of the FGF family.
Asunto(s)
Factor 1 de Crecimiento de Fibroblastos/química , Heparina/química , Animales , Sitios de Unión , Línea Celular , Cristalografía por Rayos X , Dimerización , Escherichia coli , Factor 1 de Crecimiento de Fibroblastos/genética , Factor 1 de Crecimiento de Fibroblastos/metabolismo , Heparina/metabolismo , Humanos , Enlace de Hidrógeno , Modelos Moleculares , Oligosacáridos/química , Oligosacáridos/metabolismo , Células PC12 , Conformación Proteica , Ratas , Receptores de Factores de Crecimiento de Fibroblastos/genética , Receptores de Factores de Crecimiento de Fibroblastos/metabolismo , Proteínas Recombinantes/química , Proteínas Recombinantes/metabolismoRESUMEN
The structure of d(CGCGAAAAAACG)/d(CGTTTTTTCGCG) was determined at 2.3 A resolution in order to deduce the local structural features that give rise to DNA bending by adenine tracts. Whereas all previously reported B-DNA dodecamers have crystallized isomorphously (spacegroup P2(1)2(1)2(1) with unit cell dimensions of a = 24.5 A, b = 40.3 A, c = 65.9 A), the duplex reported here crystallizes in a different lattice (spacegroup P2(1)2(1)2 with unit cell dimensions of a = 44.8 A, b = 66.1 A, c = 42.9 A). The DNA exhibits a 30 degree bend in the helix axis that is 180 degrees away from the 20 degree bend exhibited by the adenine tract DNA crystal structures that have been previously determined. This bend is 90 degrees away from the bend predicted for an adenine tract by solution and gel experiments. The adenine tract is straight and bending occurs in the G+C-rich regions. Comparison of the various adenine tract DNA crystal structures reveals that in all cases the adenine tracts have nearly identical structures, even though the overall bends of the helix axes are quite different. This implies that the structure of the adenine tract is robust, at least under the conditions of crystallization. The base-pairs in the adenine tracts exhibit a large propeller twist that leads to the formation of bifurcated hydrogen bonds and a narrow minor groove. In the crystal structure of d(CGCGAAAAAACG)/d(CGTTTTTTCGCG), a minor groove spine of hydration is observed that probably stabilizes the straight structure of the adenine tract. This straight structure of the A-tract is not consistent with the results of fiber diffraction, gel experiments, and NMR studies. Although this may imply that the results of solution experiments need to be reinterpreted, the conditions under which the crystals were grown are different from those under which the solution experiments were done. The possibility remains that the 2-methyl-2,4-pentanediol necessary for crystal growth may facilitate formation of the spine of hydration that stabilizes the straight A-tract, although recent NMR results show the presence of the spine of hydration in aqueous solution. We have also extended our previously reported observation that non-self-complementary DNA structures can exist in the crystal lattice in two orientations. A dodecamer brominated on one strand provides experimental evidence that d(CGCAAAAAAGCG)/d(CGCTTTTTTG CG) is positioned in two orientations in the crystal lattice that are related by a 180 degree rotation around the pseudo-dyad axis of the sequence.(ABSTRACT TRUNCATED AT 400 WORDS)
Asunto(s)
Conformación de Ácido Nucleico , Oligodesoxirribonucleótidos/química , Adenina , Secuencia de Bases , Cristalización , Análisis de Fourier , Modelos Moleculares , Datos de Secuencia Molecular , SolucionesRESUMEN
The crystal structure of a DNA duplex dodecamer d(CGCAAAAATGCG) and its complementary strand has been determined at 2.6-A resolution. Although our goal was to deduce the structural features of the static bending of the helical axis exhibited by adenine-tract structures in solution, we conclude that the overall bend of 20 degrees in the direction of the major groove observed here arises from the forces associated with crystal packing. An isomorphous dodecamer brominated on one strand provides experimental evidence that this asymmetric sequence is positioned in two orientations in the crystal lattice that are related by a 180 degrees rotation around the pseudodyad axis of the sequence. The bend in these two differently positioned DNA molecules depends on their orientation in the crystal, not on their sequence. As with previously determined structures containing adenine tracts, the adenine and thymine base pairs are highly propeller twisted. The N-6 of the adenine comes within hydrogen bonding distance of the O-4 of thymine one step down the helix, facilitating the formation of a series of bifurcated hydrogen bonds within the adenine tract. The adenine tract is relatively straight and the bending is localized outside this region.