Studies on the lactose operon. III. Visualization and physical mapping of the lactose repressor-operator complex

Conformation of Lac repressor tetramer in solution, bound and unbound to operator DNA

We tested whether the Steitz et al. [(1974) Proc. Natl. Acad. Sci. U.S.A., 71:593-597] model of lactose repressor (LacR) (14 x 6.0 x 4.5 nm) represented the shape of free or operator-bound LacR in solution. The model predicts a 14 nm length for bound LacR. Direct measurement, using Pt-C shadow width standards, was 9.6 +/- 0.2 nm long. Using the Steitz model, we generated a distribution of measurements and converted them into a distribution of shadow widths using gold ball standards. Direct measurement of LacR produced a narrower shadow width distribution with a larger mean size than the Steitz model predicted. Measurement along two orthogonal axes of negatively stained LacR images generated a size distribution, also converted into a shadow width distribution using the gold ball standards. Since the experimental shadow width distribution exactly matched the shadow width distribution derived theoretically from negatively stained LacR, our negative-stained images are representative of LacR's conformation in solution. Approximately 56% of negatively stained LacR had a V-shaped fold around an axis orthogonal to its length, bringing the DNA binding domains of each dimer adjacent. This open end of the V binds single operator DNA. The other 44% of the LacR tetramer is in the extended form with its DNA binding sites at opposite ends. Although the V-shaped conformation has a closed hinge with the dimers associated along a side, the extended open-hinged state remains important since LacR must bind two distant operator sites for full repression. Our measurements predict the normal presence of both conformations in nearly equal amounts, suggesting that both are equally active in repressing the lac operon.

Quantification of particle sizes with metal replication under standard freeze-etching conditions: a gold ball standard for calibrating shadow widths was used to measure freeze-etched globular proteins

The real size of platinum-carbon (Pt-C) replicated particles is not directly equivalent to either its metal-coated diameter or its shadow width. This paper describes two indirect methods, shadow widths and coated particle diameters, for determining a particle's actual size beneath a Pt-C replication film. Both produce equivalent measurements using the same standardized conditions: 2.3 nm Pt-C films deposited at a 45 degree angle on an approximately -100 degrees C surface in a 10(-6) torr vacuum. For the first method, gold balls nucleated in a partial pressure of helium and deposited on flat indirect carbon films (root mean square roughness of 0.8 nm) on 400 mesh grids were used as test particles for calibrating shadow widths as a function of particle size. The gold ball test specimens were replicated, and a distribution of Pt-C shadow widths orthogonal to the Pt-C deposition direction was measured and averaged for gold balls 1.5 +/- 0.25 nm, 2.0 +/- 0.25 nm, etc. The diameter of each gold ball was measured within the Pt-C film along with its shadow width because the Pt-C did not obscure or adhere well to the gold. The shadow width distributions for each gold size do not differ significantly from log normal. Two proteins, the lactose repressor and the mitochondrial ATPase, F1, were also used as replication test objects. Negative staining of both proteins was conducted to measure their average diameters. In the second method, a distribution of Pt-C-coated lac repressor diameters perpendicular to the shadow direction was measured. The Pt-C film thickness measured on the quartz crystal monitor was subtracted from the average metal-coated protein diameter to obtain the lac repressor's diameter. The Pt-C-coated particle diameter distributions also did not differ significantly from log normal. While doing this work it was discovered that outgassing the Pt-C electron gun greatly affected Pt-C film granularity: 19 sec produced a high contrast, granular Pt-C film, whereas 120 sec yielded a low contrast, less granular Pt-C film. Both gold balls and protein particles were subjected in separate experiments to either 19 or 120 sec of outgassing of the Pt-C gun prior to Pt-C replication. Outgassing had a profound effect on the average size of the Pt-C shadow widths on both gold and protein particles. The Pt-C gun outgassing procedure also determined the smallest replicated particle that could be resolved. The frequency of some smaller gold ball sizes detected after replication was reduced disproportionately with 19 sec vs. 120 sec outgassing. However, Pt-C gun outgassing did not affect the average measured diameter of the Pt-C-coated protein particles. The "geometric assumption" that each metal-coated particle creates a shadow width the same size as the metal-coated particle diameter was tested using a globular protein. Pt-C replication of protein particles at a 45 degree and 20 degree angle could not confirm the geometric assumption because an average shadow width was always significantly larger than its average Pt-C-coated particle diameter. A model for how the large shadow widths are formed is presented. Gold balls were also replicated at a 45 degree angle with current high resolution conditions at a substrate temperature of -185 degrees C, and the results of these replicas were compared to the results reported here at approximately -100 degrees C.

Small-angle X-ray studies of the quaternary structure of the lac repressor from Escherichia coli

The quarternary structures of the lac repressor molecule from Escherichia coli and its tetrametic core, which can be derived from it by proteolytic cleavage, were studied in dilute solutions by small-angle X-ray scattering. The dimensions and general shape of the lac repressor and of the tetrameric core are reported. The core itself appears to be an elongated structure, and in the intact repressor the headpieces are located at its ends. The results ar derived from model calculations and from the following molecular parameters determined from the scattering curve and the pair distance distribution function: for lac repressor, radius of gyration 5.30 +/- 0.02 nm, radius of gyration of the cross section 2.20 +/- 0.03 nm, maximum diameter 18.0 +/- 0.5 nm, hydrated volume 329 +/- 20 nm3, relative molecular mass 149 000 +/- 15 000, for tetrameric core, radius of gyration 4.92 +/- 0.02 nm, radius of gyration of the cross section 2.24 +/- 0.03 nm, maximum diameter 16.0 +/- 0.5 nm, hydrated volume 278 +/- 15 nm3, relative molecular mass 120 000 +/- 10 000.

The functional repressor parts of a tetrameric lac repressor-beta-galactosidase chimaera are organized as dimers

The chimaeric protein repressor-galactosidase, in which fully active lac repressor is covalently linked to the active enzyme beta-galactosidase, was used as a system for probing the quaternary structure of lac repressor. Electron micrographs revealed repressor-galactosidase to be a tetrameric aggregate. When lac repressor, alone, was crosslinked with dimethyl suberimidate, dimers, trimers, tetramers, and oligomers of the protein subunit were produced, whereas crosslinking of the tetrameric repressor-galactosidase resulted in the production of only dimers of the chimaera. Treatment of lac repressor with iodine resulted in the formation of protein dimers; the same result was obtained with repressor-galactosidase. After limited proteolysis of lac repressor, no crosslinking was obtained after treatment with dimethyl suberimidate, whereas iodine still produced a covalent linkage. These results are interpreted as evidence that the lac repressor parts of the tetrameric repressor-galactosidase-chimaera are organized as dimers on the tetrameric-beta-galactosidase core. Because this chimaera has been previously shown to have normal repressor activity [B. Müller-Hill and J. Kania (1974) Nature, 249,561-563], we conclude that lac repressor still is biologically active as a dimeric aggregate.