Rates of assembly and degradation of bacterial ice nuclei.

The kinetics of ice-nucleus assembly from newly synthesized nucleation protein were observed following induction of nucleation gene expression in the heterologous host Escherichia coli. Assembly was significantly slower for the small proportion of ice nuclei active above -4.4 degrees C; this was consistent with the belief that these nuclei comprise the largest aggregates of nucleation protein. The kinetics of nucleus degradation were followed after inhibiting protein synthesis. Nucleation activity and protein showed a concerted decay, indicating that most of the functional ice nuclei are in equilibrium with a single cellular pool of nucleation protein. A minority of the ice nuclei decayed much more slowly than the majority; presumably their nucleation protein was distinct either by virtue of different structure or different subcellular compartmentalization, or because of its presence in a metabolically distinct subpopulation of cells.

Clustering of ice nucleation protein correlates with ice nucleation activity.

Antibodies raised against a synthetic peptide specifically detect ice nucleation proteins from Pseudomonas species in Western blots. In immunofluorescent staining of whole bacteria, the antibodies reveal the protein in clusters, as indicated by patches of intense fluorescence in Escherichia coli cells heterologously expressing Pseudomonas ice nucleation genes. The abundance, size, and brightness of the clusters vary considerably from cell to cell. Their varying sizes may explain the variability in activity of bacterial ice nuclei. Growth at lower temperatures produces more ice nuclei, and gives brighter and more frequent patches, than growth at 37 degrees C. The observed clustering may thus reflect formation of functional ice nucleation sites in vivo. The presence of ice nucleation protein in clusters is also correlated with alterations in cell morphology.

Nonlinear relationship between concentration and activity of a bacterial ice nucleation protein.

The expression level of an ice nucleation gene (inaZ) was varied in Escherichia coli to observe the relationship between activity and gene product. The ice nucleation activity increased as the 2nd to 3rd power of the membrane concentration of the inaZ gene product, implying that molecules of InaZ protein interact cooperatively in groups of two to three at the rate-limiting step of ice nucleus assembly. The 2nd to 3rd power relationship was independent of the threshold temperature at which ice nucleation was measured and was consistent over a 500-fold range of protein concentration. Such a relationship indicates that the same rate-limiting step must be common to the formation of ice nuclei displaying all the various threshold temperatures within a bacterial population. Observations of Pseudomonas syringae, expressing the inaZ gene at various levels, were consistent with a similar relationship and hence a similar mechanism of ice nucleus assembly in Pseudomonas.

Immunological characterization of ice nucleation proteins from Pseudomonas syringae, Pseudomonas fluorescens, and Erwinia herbicola.

Antibodies were raised against the InaW protein, the product of the ice nucleation gene of Pseudomonas fluorescens MS1650, after protein isolation from an Escherichia coli clone. On Western blots (immunoblots), these antibodies recognized InaW protein and InaZ protein (the ice nucleation gene product of Pseudomonas syringae S203), produced by both E. coli clones and the source organisms. The InaZ protein appeared in P. syringae S203 during stationary phase; its appearance was correlated with the appearance of the ice nucleation-active phenotype. In contrast, the InaW protein occurred at relatively constant levels throughout the growth phases of P. fluorescens MS1650; the ice nucleation activity was also constant. Western analyses of membrane preparations of P. syringae PS31 and Erwinia herbicola MS3000 with this antibody revealed proteins which were synthesized with development of the nucleating phenotype. In these species the presence or absence of the nucleating phenotype was controlled by manipulation of culture conditions. In all nucleation-positive cultures examined, cross-reacting low-molecular-weight bands were observed; these bands appeared to be products of proteolytic degradation of ice nucleation proteins. The proteolysis pattern of InaZ protein seen on Western blots showed a periodic pattern of fragment sizes, suggesting a highly repetitive site for protease action. A periodic primary structure is predicted by the DNA sequence of the inaZ gene.

Identification and purification of a bacterial ice-nucleation protein.

The protein product of a gene (inaZ) responsible for ice nucleation by Pseudomonas syringae S203 has been identified and purified after overexpression in Escherichia coli. The amino acid composition and the N-terminal sequence of the purified, denatured protein corresponded well with that predicted from the sequence of the inaZ gene. The product of inaZ was also found to be the major component in preparations of ice-nucleating, proteinaceous particles, obtained after extraction with and gel filtration in a mixture of urea and the nondenaturing detergent octyl beta-D-thioglucopyranoside. The activity of these preparations in the absence of added lipid implies that the protein participates directly in the nucleation process.

Mapping of the triazine binding site to a highly conserved region of the QB-protein.

A number of herbicide classes, including the s-triazines and ureas (atrazine, diuron) inhibit photosynthetic electron transport via a direct interaction with the QB-protein. This protein, also known as the 32-kDa protein or herbicide binding protein, is believed to bind the plastoquinone QB, which functions as the second stable electron acceptor at the reducing side of Photosystem II. The site of covalent attachment of the photoaffinity herbicide analog azido-[14C]atrazine to the QB-protein of spinach chloroplast thylakoid membranes has been determined. Two amino acid residues are labeled; one residue is methionine-214, the other lies between histidine-215 and arginine-225. Both residues are within a region of the amino acid sequence which is highly conserved between the QB-protein and the L and M reaction center proteins of Rhodopseudomonas capsulata and R. sphaeroides. This region includes the site of a mutation which results in diuron resistance in Chlamydomonas reinhardi (valine-219). However, this region is well removed from point mutations at phenylalanine-255 (which gives rise to atrazine resistance in C. reinhardi) and at serine-264, (which results in extreme atrazine resistance in C. reinhardi and naturally occurring weed biotypes). The patterns of labeling and mutation imply that the quinone and herbicide binding site is formed by at least two protein domains.

Ice nucleation activity of Pseudomonas fluorescens: mutagenesis, complementation analysis and identification of a gene product.

A DNA fragment of 7.5 kb from Pseudomonas fluorescens MS1650 confers an ice nucleation phenotype when cloned in Escherichia coli. This DNA encodes a protein with an apparent mol. wt of 180 kd, which is found in both inner and outer membrane fractions of transformed E. coli cells. Insertion mutations throughout a 3.9-kb region cause deficiency in ice nucleation, and eliminate the 180-kd protein. Complementation is not observed between any pair of mutations, suggesting that the nucleating phenotype is encoded by a single transcriptional unit. Mutations in most parts of the 3.9-kb region are not completely deficient in phenotype: they still generate ice nuclei at low frequency. One insertion mutation was found to generate pseudowild revertants, which had undergone deletions of the entire insertion and some of the adjacent sequence; these could account for the incomplete deficiency. These deletions displayed depressed nucleation temperatures, but their nucleation frequencies were close to that of the wild-type gene.

Coupling between the bacteriorhodopsin photocycle and the protonmotive force in Halobacterium halobium cell envelope vesicles. III. Time-resolved increase in the transmembrane electric potential and modeling of the associated ion fluxes.

Bacteriorhodopsin functions as an electrogenic, light-driven proton pump in Halobacterium halobium. In cell envelope vesicles, its photocycle kinetics can be correlated with membrane potential. The initial decay rate of the M photocycle intermediate(s) decreases with increasing membrane potential, allowing the construction of a calibration curve. The laser (592.5 nm) was flashed at various time delays following the start of background illumination (592 +/- 25 nm) and transient absorbance changes at 418 nm monitored in cell envelope vesicles. The vesicles were loaded with and suspended in either 3 M NaCl or 3 M KCl buffered with 50 mM HEPES at pH 7.5 and the membrane permeability to protons modified by pretreatment with N,N'-dicyclohexylcarbodiimide. In each case the membrane potential rose with a halftime of approximately 75 ms. The steady-state potential achieved depends on the cation present and the proton permeability of the membrane, i.e., higher potentials are developed in dicyclohexylcarbodiimide treated vesicles or in NaCl media as compared with KCl media. The results are modeled using an irreversible thermodynamics formulation, which assumes a constant driving reaction affinity (Ach) and a variable reaction rate (Jr) for the proton-pumping cycle of bacteriorhodopsin. Additionally, the model includes a voltage-gated, electrogenic Na+/H+ antiporter that is active when vesicles are suspended in NaCl. Estimates for the linear phenomenological coefficients describing the overall proton-pumping cycle (Lr = 3.5 X 10(-11)/mol2/J X g X s), passive cation permeabilities (LHu = 2 X 10(-10), LKu = 2.2 X 10(-10), LNau = 1 X 10(-11)), and the Na+/H+ exchange via the antiporter (Lex = 5 X 10(-11)) have been obtained.

Coupling between the bacteriorhodopsin photocycle and the protonmotive force in Halobacterium halobium cell envelope vesicles. II. Quantitation and preliminary modeling of the M----bR reactions.

The cell membrane of Halobacterium halobium (H. halobium) contains the proton-pump bacteriorhodopsin, which generates a light-driven transmembrane protonmotive force. The interaction of the bacteriorhodopsin photocycle with the electric potential component of the protonmotive force has been investigated. H. halobium cell envelope vesicles have been prepared by sonication and further purified by ultracentrifugation on Ficoll/NaCl/CsCl density gradients. Under continuous illumination (550 +/- 50 nm) varied from 0 to 40 mW cm-2, the vesicles maintain a membrane potential of 0 to -100 mV. The membrane potential was measured by flow dialysis of 3H-TPMP+ uptake and could be abolished by the uncoupler carbonylcyanide-m-chlorophenylhydrazone. Time-resolved absorption spectroscopy was used to measure the decay kinetics of the M photocycle intermediate, which was initiated by a weak laser flash (588 nm), while the vesicles were continuously illuminated as above. The M decay kinetics were fitted with two exponential decays by a computer deconvolution program. The faster decaying form decreases in amplitude (70 to 10% of the total) and the slower decaying form increases in amplitude and lifetime (23 to 42 ms) as the background light intensity increases. Although any correlation between the membrane potential and the bacteriorhodopsin photocycle M-forms is complex, the present data will allow specific tests of the physical mechanism for this interaction to be designed and conducted.

Retinal migration during dark reduction of bacteriorhodopsin.

When the retinal Schiff base in chymotryptically cleaved bacteriorhodopsin is reduced to a secondary retinylamine by prolonged exposure to 10% (wt/vol) sodium cyanoborohydride, at pH 10, in the absence of light, approximately 45% of the retinal is found linked to Lys-41 and 22% to Lys-40, and the remainder is scattered over various sites on the large chymotryptic fragment, including the physiological site at Lys-216. The retinal-binding site is destroyed or blocked by the reduction conditions, but the bacteriorhodopsin lattice remains intact. The results demonstrate that artifactual linkage to Lys-40/41 is possible under special conditions. Under these conditions, the epsilon-amino groups of Lys-40/41 show an enhanced ability to form retinylidene linkages with the retinal released by the physiological linkage site at Lys-216, due to some combination of close proximity to the normal linkage site, and increased reactivity with respect to other lysine epsilon-amino groups. The results are of interest for the characterization of the two newly discovered rhodopsin-like proteins, halorhodopsin and slow rhodopsin.

Bilayer acyl chain dynamics and lipid-protein interaction: the effect of the M13 bacteriophage coat protein on the decay of the fluorescence anisotropy of parinaric acid.

Nanosecond fluorescence polarization anisotropy decay is used to determine the effect of the bacteriophage M13 coat protein on lipid bilayer acyl chain dynamics and order. The fluorescent acyl chain analogues cis- and trans-parinaric acid were used to determine the rate and extent of the angular motion of acyl chains in liquid crystalline (39 degrees C) dimyristoylphosphatidylcholine bilayers free of coat protein or containing the coat protein at a protein:lipid ratio of 1:30. Subnanosecond time resolution was obtained by using synchrotron radiation as the excitation source for single photon counting detection. Previous measurements of Förster energy transfer from coat protein tryptophan to cis- or trans-parinaric acid have shown that these probes are randomly distributed in the bilayer with respect to the protein. The anisotropy decay observed for pure bilayers has the form of a rapid drop, followed by a nonzero constant region extending from roughly 3 ns to at least 12 ns. The magnitude of the anisotropy in the plateau region is simply related to the acyl chain order parameter. The effect of the M13 coat protein is to increase the acyl chain order parameter significantly while having only a small effect on the rate of angular relaxation. This behavior is rationalized in terms of a simple microscopic model. The order parameters for pure lipid and coat protein containing bilayers are compared to 2H-NMR values.

Attachment site(s) of retinal in bacteriorhodopsin.

After chemical reduction of the retinylidene-lysine Schiff base linkage in bacteriorhodopsin, the retinyl residue is covalently attached to Lys-216 (with a possible minor fraction on Lys-172) or to both Lys-216(172) and Lys-40/41. The linkage site (up to 100% on Lys-216; up to 70% on Lys-40/41) depends on whether the sample is reduced in the light or dark, whether the sample is light or dark adapted, and on temperature. Absorbance and circular dichroism spectra indicate that the retinyl residue is in its original binding site after reduction in the light. Thus, the different attachment sites may reflect changes that occur during the photoreaction cycle or during light/dark adaptation, or the reduction of accidental physiologically irrelevant Schiff base linkages to lysines close to the normal linkage in the structure of bacteriorhodopsin. In either case, the retinal does not leave its binding site. This last point severely limits the possible arrangements of the amino acid sequence in the bacteriorhodopsin tertiary structure and clearly distinguishes two models that are consistent with all criteria.

Fluorescence lifetime and time-resolved polarization anisotropy studies of acyl chain order and dynamics in lipid bilayers.

The time-resolved fluorescence intensity and anisotropy decays of cis- and trans-parinaric acids and phosphatidylcholines labeled with trans-parinaric acid have been characterized in bilayers formed by several phosphatidylcholines and by dipalmitoylphosphatidylcholine-cholesterol mixtures, at several temperatures. Both a conventional free-running nitrogen flashlamp and the novel synchrotron source at the Stanford Linear Accelerator Center (SLAC) were used as excitation sources for a modified single photon counting fluorescence lifetime apparatus. The measured emission decay kinetics of both isomers of parinaric acid were biexponential in all but one of the lipid systems examined. The fluorescence anisotropy of parinaric acid was large and constant in gel phase lipids, but showed a very rapid (approximately 2 GHz) decay of large amplitude in fluid lipids. In all lipid systems studied, the fluorescence anisotropy decayed to a nonzero asymptote, in striking contrast to the behavior observed in viscous solvent solutions. The asymptotic anisotropy was used to calculate an "order parameter" of the emission transition dipole. The value of the order parameter is quite close to that obtained by deuterium NMR. Cholesterol increased the order parameter measured in fluid dipalmitoylphosphatidylcholine but did not substantially affect the rate of angular relaxation. Experiments conducted with trans-parinaroylphosphatidylcholines yielded results virtually identical with those obtained with trans-parinaric acid.

Photochemical dimerization of parinaric acid in lipid bilayers.

Parinaric acid (9,11,13,15-octadecatetraenoic acid), a conjugated tetraene fatty acid, undergoes a second-order photochemical reaction in phospholipid bilayers. The reaction results in the loss of the characteristic absorption of this chromophore and the development of new absorption demonstrating the presence of a triene chromophore. The progress of this reaction is easily monitored by measurement of the decrease in the fluorescence intensity from a uniformly illuminated sample. The reaction rate measured in this way is sensitive to the thermal phase transition of the bilayer and to the presence of cholesterol. The relationship of the second-order rate constant to the lipid diffusion coefficient is discussed. This relationship differs from that previously used for the analysis of similar photochemical processes.

An analytic solution to the Förster energy transfer problem in two dimensions.

An analytic solution of the Förster energy transfer problem in two dimensions is presented for the case in which the orientation factor is independent of the donor-acceptor distance, and both the donors and acceptors are randomly distributed in a plane. A general solution based on the method of Förster is possible since all distances are measured in units of R0. The analytic solution is extended to the cases of donors embedded in structures that exclude acceptors, and donors that bind acceptors. The validity of the analytic solutions is demonstrated by comparison with numerical simulation calculations. Numerical approximations to the exact solutions are given for ease of computation. Specific applications to the case of fluorescence quenching of a membrane-bound donor by membrane-bound acceptors are presented.