Structural dynamics of the lac repressor-DNA complex revealed by a multiscale simulation

A multiscale simulation of a complex between the lac repressor protein (LacI) and a 107-bp-long DNA segment is reported. The complex between the repressor and two operator DNA segments is described by all-atom molecular dynamics; the size of the simulated system comprises either 226,000 or 314,000 atoms. The DNA loop connecting the operators is modeled as a continuous elastic ribbon, described mathematically by the nonlinear Kirchhoff differential equations with boundary conditions obtained from the coordinates of the terminal base pairs of each operator. The forces stemming from the looped DNA are included in the molecular dynamics simulations; the loop structure and the forces are continuously recomputed because the protein motions during the simulations shift the operators and the presumed termini of the loop. The simulations reveal the structural dynamics of the LacI-DNA complex in unprecedented detail. The multiple domains of LacI exhibit remarkable structural stability during the simulation, moving much like rigid bodies. LacI is shown to absorb the strain from the looped DNA mainly through its mobile DNA-binding head groups. Even with large fluctuating forces applied, the head groups tilt strongly and keep their grip on the operator DNA, while the remainder of the protein retains its V-shaped structure. A simulated opening of the cleft of LacI by 500-pN forces revealed the interactions responsible for locking LacI in the V-conformation.     

Demonstration of two operator elements in gal: in vitro repressor binding studies.

Genetic and DNA base sequence analyses of cis-dominant mutations that derepress the gal operon of Escherichia coli suggested the existence of two operator loci needed for gal repression. One (OE) is located immediately upstream to the two overlapping gal promoters and the other (OI) is inside the first structural gene. We have investigated the ability of wild-type and mutant OE and OI DNA sequences to bind to gal repressor. The repressor has been purified from cells containing a multicopy plasmid in which the repressor gene is brought under the control of phage lambda PL promoter. The DNA-repressor interactions are detected by the change in electrophoretic mobility of labeled DNA that accompanies its complex formation with repressor protein. The purified repressor shows concentration-dependent binding to both O+E and O+I but not to OEc and OIc sequences. These results authenticate the proposed operator role of the two homologous gal DNA control elements and thereby establish that the negative control of the gal operon requires repressor binding at both OE and OI, which are separated by greater than 90 base pairs.     

Cyclic AMP-dependent constitutive expression of gal operon: use of repressor titration to isolate operator mutations.

When the gal operator region is present in a multicopy plasmid it binds to all ("titrates") the gal repressor and "induces" the chromosomal gal operon. To make operator mutations (Oa) with reduced affinity toward the repressor, plasmid DNA was irradiated with UV light and mutant derivatives were isolated that were unable to release the chromosomal gal genes from repression. Then with such an Oa plasmid operator revertants were isolated that had reacquired the ability to release repression. Both sets of mutations have been localized by DNA sequence analysis. When the Oa mutations were transferred from the plasmid to the chromosome by recombination these mutant operators were found to make gal expression constitutive (independent of repressor) but still dependent on cAMP, whereas the previously reported gal operator mutants (Oc) are constitutive both in the presence and in the absence of cAMP. The titration method of isolating mutants enables the isolation of strains with operator mutations that also affect normal promoter activity, and it provides an easy way to isolate revertants of operator mutations.     

Promoters largely determine the efficiency of repressor action.

Operator sequence and repressor protein regulate the activity of the lac promoter over a greater than 1000-fold range. Combinations of the lac operator with other promoter sequences, however, differ vastly in the level of repression. The data presented show that the extent of repression is determined largely by the rates of complex formation of the competing systems operator-repressor and promoter-RNA polymerase and by the rate at which RNA polymerase clears the promoter. Moreover, up to 70-fold differences in the level of repression were found when the operator was placed in different positions within the promoter sequence. A kinetic model is proposed that explains the observed effects and that allows predictions on promoters controlled by negatively acting elements.     

Contacts between the lac repressor and the thymines in the lac operator.

We have identified important points of contact between the lac repressor and the lac operator by crosslinking the repressor to bromouracil-substituted operator. We substituted bromouracils for thymines in a 55-base-long restriction fragment containing the lac operator and labeled one or the other 5' end with 32P. Ultraviolet irradiation of this fragment produced single-strand breakds at the bromouracils. We examined breakage at each bromouracil in the sequence by denaturing the DNA and displaying the UV-generated fragments on a polyacrylamide gel. In the presence of lac repressor, UV radiation failed to break at specific sites. We attribute this to a competing reaction in which the DNA crosslinks to the repressor rather than breaking. These crosslinkable sites thus define positions at which the lac repressor protein lies close to the methyl group of a thymine in the major groove of DNA.