Comparison of the binding sites for the Escherichia coli cAMP receptor protein at the lactose and galactose promoters

Polyacrylamide gel electrophoresis has been used to visualise and quantitate complexes between the Escherichia coli cyclic AMP receptor protein (CRP) and DNA fragments containing the promoter region of either the E. coli galactose or lactose operons. We show that, although CRP binding to the gal fragment is weaker than binding to the lac fragment, in each case, stable complexes are formed between one dimer of CRP and one molecule of DNA. We have examined the effects of a series of deletions and point mutations in the gal promoter region on CRP binding. From the position of deletions and mutations which prevent the formation of stable complexes, we deduce the location and extent of the sequence at the CRP binding site. We show that it covers approximately the same length of sequence as the binding site at the lac promoter. Unlike the lac site, the gal site contains no palindromic sequence. We discuss the importance of symmetry in the sequence at CRP binding sites and the validity of CRP binding consensus sequences which have been proposed.     

Specific DNA binding of the cyclic AMP receptor protein to a synthetic oligodeoxyribonucleotide. A circular dichroism study

The interaction of the cAMP receptor protein (CRP) of Escherichia coli with a synthetic DNA undecamer (11 mer) comprising a portion of the specific target site in the gal operon and containing 8 basepairs out of the 10 basepair concensus making up specific CRP sites, has been studied by circular dichroism spectroscopy. The binding constants for the interaction of CRP with the 11 mer in the presence and absence of cAMP have been determined, and it is shown that CRP, both in the presence and absence of cAMP, induces a B-C transition in the conformation of the 11 mer.     

A theoretical model for the binding of cis-Pt(NH3)2(+2) to DNA

The binding of cis-Pt(NH3)2B1B2 to the bases B1 and B2, i.e., guanine (G), cytosine (C), adenine (A), and thymine (T), of DNA is studied theoretically. The components of the binding are analyzed and a model structure is proposed for the intrastrand binding to the dB1pdB2 sequence of a kinked double helical DNA. Quantum mechanical calculations of the ligand binding energy indicates that cis-Pt(NH3)2(+2) (cis-PDA) binds to N7(G), N3(C), O2(C), O6(G), N3(A), N7(A), O4(T) and O2(T) in order of decreasing binding energy. Conformational analysis provides structures of kinked DNA in which adjacent bases chelate to cis-PDA. Only bending toward the major groove allows the construction of acceptable square planar complexes. Examples are presented for kinks of -70 degrees and -40 degrees at the receptor site to orient the base pairs for ligand binding to B1 and B2 to form a nearly square planar complex. The energies for complex formation of cis-PDA to the various intra-strand base sites in double stranded DNA are estimated. At least 32 kcal/mole separates the energetically favorable dGpdG.cis-PDA chelate from the dCpdG.cis-PDA chelate. All other possible chelate structures are much higher in energy which correlates with their lack of observation in competition with the preferred dGpdG chelate. The second most favorable ligand energy occurs with N3(C). A novel binding site involving dC(N3)pdG(N7) is examined. Denaturation can result in an anti----syn rotation of C about its glycosidic bond to place N3(C) in the major groove for intrastrand binding in duplex DNA. This novel intrastrand dCpdG complex and the most favored dGpdG structure are illustrated with stereographic projections.     

RNA polymerase and gal repressor bind simultaneously and with DNA bending to the control region of the Escherichia coli galactose operon.

The Escherichia coli galactose operon contains an unusual array of closely spaced binding sites for proteins governing the expression from the two physically overlapping gal promoters. Based on studies of two gal promoter-up mutants we have previously suggested RNA-polymerase-induced DNA bending of gal promoter DNA. Here we present new evidence confirming and extending this interpretation. It was obtained by the circular permutation assay of gel electrophoretic mobility [Wu and Crothers (1984), Nature, 308, 509-513] applied to three analogous series of circularly permuted fragments derived from wild-type and two promoter-up mutant DNAs. The same circularly permuted DNA fragments have further been used to study the binding of gal repressor to its operator sites by electrophoretic mobility shift and by DNase I footprinting techniques. The main results are: (i) complexes carrying repressor either exclusively at the upstream operator O1 or at the downstream operator O2 exhibit different electrophoretic mobilities; (ii) binding to either one of the operators results in protein-induced DNA bending by the criteria of the circular permutation mobility assay; and (iii) occupation of both gal operators by gal repressor does not prevent cAMP-CRP-independent binding of RNA polymerase to the gal promoters, as judged by DNase I protection and gel retardation assays. The latter finding imposes constraints on any attempt to model the regulation of gal expression by assumed DNA-protein and protein-protein interactions.     

Turn of promotor DNA by cAMP receptor protein characterized by bead model simulation of rotational diffusion

The rotation diffusion of DNA double helices and their complexes with the cAMP receptor protein (CRP) has been simulated by bead models, in order to derive information on their structure in solution by comparison with results obtained from dichroism decay measurements. Straight DNA double helices are simulated by linear, rigid strings of overlapping beads. The radius of the beads and the length of the string are increased simultaneously by the same increments from initial outer dimensions derived from crystallographic data to final values, which are fitted to experimental rotation time constants observed for short DNA fragments (less than 100 bp). The final values reflect the solvated structure with the same 'solvation layer' added in all three dimensions. The protein is simulated by overlapping beads, which are assembled to a structure very similar to that found by x-ray crystallography. Complexes of the protein with DNA are formed with the centres of palindromic DNA sites at the centre of the two helix-turn-helix-motifs of the protein with some overlap of the two components. Simulation of the experimental data obtained for CRP complexes with specific DNA in the presence of cAMP requires strong bending of the double helices. According to our simulation the DNA is almost completely wrapped around the protein both in the complexes with a 62 bp fragment containing the standard CRP site and with a 80 bp fragment containing the second binding site of the lac operon. Simulations of the data obtained for a 203 bp fragment with both binding sites suggest that the two bound CRP proteins are in contact with each other and that the DNA is wrapped around the two protein dimers. A stereochemical model is suggested with a tetrahedral arrangement of the four protein subunits, which provides the advantage that two binding sites of the protein formed by two subunits each are located favorable for tight contacts to two binding sites on bent DNA, provided that the DNA sites are separated by an integer number of helix turns. In summary, the simulations demonstrate strong bending, which can be reflected by an arc radius in the range around 50 A. According to these data the overall bending angle of our longest DNA fragment is approximately 180 degrees, and thus the protruding ends are sufficiently close to each other such that RNA polymerase, for example, could contact both helical segments.     

Calorimetric studies of the binding of ferric ions to ovotransferrin and interactions between binding sites.

Transferrins are two-domain proteins with a very strong site for iron binding located in each domain. Using ultrasensitive titration calorimetry, the binding of ferric ion (chelated with a 2-fold molar excess of nitrilotriacetate) to the two sites of ovotransferrin was studied in detail as well as the binding to the single site in the N- and C-terminal half-molecules. In the presence of excess bicarbonate ion, the binding occurs in two kinetic steps. The fast process of contact binding is instantaneous with respect to instrument response time, is strongly exothermic for the N site and less so for the C site, and corresponds to binding of the chelated ferric ion. The slower process of bicarbonate insertion with concomitant release of nitrilotriacetate occurs on a time scale of 2-20 min over the temperature range 7-37 degrees C and is endothermic for the N site and exothermic for the C site, with rates being significantly slower for insertion at the C site. The delta H of binding is strongly temperature-dependent for both sites, arising from a large negative delta Cp of binding which probably indicates removal of hydrophobic groups from contact with water. When bicarbonate ion is absent, only the fast process of contact binding is seen. Each site within a half-molecule is qualitatively similar to the same site in intact ovotransferrin, although quantitative differences were detected. It was shown that contact binding to ovotransferrin occurs reversibly with free exchange of Fe+3 between N and C sites, while the attachment to either site becomes essentially irreversible after bicarbonate insertion. The strong preference for the first ferric ion to bind to the N site is shown to be due to its larger contact binding constant and the faster rate of bicarbonate insertion, relative to the C site, and is not due to stronger thermodynamic binding after bicarbonate insertion. True equilibrium is achieved only over much longer periods of time. In another series of experiments, direct binding studies were carried out between the two half-molecules under different states of ligation with Fe+3 in the presence of bicarbonate. The results indicate that the two binding sites in ovotransferrin, separated by ca. 40 A, are not independent of one another but communicate as a result of ligand-dependent changes in the heats and free energies of domain-domain interactions.(ABSTRACT TRUNCATED AT 400 WORDS)     

Turn of Promotor DNA by cAMP Receptor Protein Characterized by Bead Model Simulation of Rotational Diffusion

Abstract

The rotation diffusion of DNA double helices and their complexes with the cAMP receptor protein (CRP) has been simulated by bead models, in order to derive information on their structure in solution by comparison with results obtained from dichroism decay measurements. Straight DNA double helices are simulated by linear, rigid strings of overlapping beads. The radius of the beads and the length of the string are increased simultaneously by the same increments from initial outer dimensions derived from crystallographic data to final values, which are fitted to experimental rotation time constants observed for short DNA fragments (< 100 bp). The final values reflect the solvated structure with the same ‘solvation layer’ added in all three dimensions. The protein is simulated by overlapping beads, which are assembled to a structure very similar to that found by x-ray crystallography. Complexes of the protein with DNA are formed with the centres of palindromic DNA sites at the centre of the two helix- turn-helix-motifs of the protein with some overlap of the two components. Simulation of the experimental data obtained for CRP complexes with specific DNA in the presence of cAMP requires strong bending of the double helices. According to our simulation the DNA is almost completely wrapped around the protein both in the complexes with a 62 bp fragment containing the standard CRP site and with a 80 bp fragment containing the second binding site of the lac operon. Simulations of the data obtained for a 203 bp fragment with both binding sites suggest that the two bound CRP proteins are in contact with each other and that the DNA is wrapped around the two protein dimers. A stereochemical model is suggested with a tetrahedral arrangement of the four protein subunits, which provides the advantage that two binding sites of the protein formed by two subunits each are located favorable for tight contacts to two binding sites on bent DNA provided that the DNA sites are separated by an integer number of helix turns. In summary, the simulations demonstrate strong bending, which can be reflected by an arc radius in the range around 50 Å. According to these data the overall bending angle of our longest DNA fragment is approximately 180°, and thus the protruding ends are sufficiently close to each other such that RNA polymerase, for example, could contact both helical segments.