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.