Photochemical cycle and light-dark adaptation of monomeric and aggregated bacteriorhodopsin in various lipid environments

Spectral changes of bacteriorhodopsin (BR) reflecting its photochemical cycle and light-dark adaptation were monitored in order to study the effect of protein-protein and protein-lipid interactions on these reactions. For this purpose, the light-driven proton pump BR was reconstituted with various lipids, i.e., dimyristoyl- and dipalmitoyl-phosphatidylcholine, soybean phospholipids, and diphytanoyllecithin. In these vesicle systems, BR is monomeric above the lipid phase transition and above molar lipid to BR ratios of about 80. Well below the phase transition, BR is aggregated in a hexagonal lattice as in the purple membrane. This allows, on the one hand, comparison of monomeric and aggregated BR in the respective vesicle systems and, on the other hand, comparison of reconstituted BR with BR in the native purple membrane. The photoreaction cycle of all-trans-BR accompanying proton translocation proceeds via the same intermediates in the monomeric and aggregated pigment. Furthermore, both the rate and the activation energy for the decay of the cycle intermediate M-410 are independent of the aggregation state. From the results, we conclude that the functional unit responsible for BR's photocycle is the monomer itself. This is in accordance with previous observations that BR monomers are able to translocate protons during illumination [Drencher, N. A., & Heyn, M.P. (1979) FEBS Lett. 108, 307-310]. The light-dark adaptation reaction, however, is affected by BR's aggregation state. In the case of the monomer, the extent of light adaptation, i.e., the fraction of BR molecules containing 13-cis-retinal as chromophore which is converted by illumination to the respective pigment with the all-trans isomer, is reduced by 50% or more, and the rate of dark adaptation is slowed down about 2.5 times. For these properties too, the monomer is functional, but with a reduced efficiency. This indicates regulatory control by neighboring BR molecules. The rate of the photocycle as well as of dark adaptation is strongly affected by the chemical nature of the lipids used for reconstitution but not by the physical state of the lipid phase.

Calorimetric and fluorescence depolarization studies on the lipid phase transition of bacteriorhodopsin--dimyristoylphosphatidylcholine vesicles

The thermotropic lipid phase transition of dimyristoylphosphatidylcholine vesicles reconstituted with bacteriorhodopsin was investigated as a function of the lipid to protein ratio by means of differential scanning calorimetry and fluorescence depolarization of the embedded probe 1,6-diphenyl-1,3,5-hexatriene. Two attractive features of this system are that the lipid phase transition induces lipid-protein segregation and that the state of aggregation of the protein is known. Above the lipid phase transition and above molar lipid to protein ratios of about 100, bacteriorhodopsin is monomeric. Well below the phase transition, bacteriorhodopsin is aggregated in a hexagonal protein lattice. With increasing amounts of incorporated bacteriorhodopsin, the calorimetric transition broadens, and a second component develops at a temperature which is lower than that of the unperturbed transition. The latter transition was assigned to the disaggregation of the bacteriorhodpsin lattice which occurs 6-7 degrees C below the phase transition of the protein-free lipids according to previous measurements. The van't Hoff enthalpy of the phase transition, as determined from the fluorescence depolarization of diphenylhexatriene, is in surprisingly good agreement with that obtained from differential scanning calorimetry over a wide range of lipid to protein ratios. The differential scanning calorimetry data can be simulated on the basis of a model which takes the protein segregation and crystallization specifically into account. The essential feature of this model is that calorimetrically detectable lipid melting occurs in the temperature region of the protein crystallization, since for the disaggregation of the close packed bacteriorhodopsin lattice additional lipids of an intermediate chain conformation are required.

Transmembranous incorporation of photoelectrically active bacteriorhodopsin in planar lipid bilayers

Various methods to incorporate bacteriorhodopsin in black lipid membranes are reported. Both purple membrane patches and monomeric bacteriorhodopsin were used as starting material. The incorporation of bacteriorhodopsin into planar lipid bilayers was achieved by the following methods. (i) Purple membrane patches were transferred from water to solutions of lipids in n-alkanes. Black membranes were formed from such organic suspensions. (ii) Lipid layers containing solvent and purple membranes were spread on an air/water interface. These layers were used to form planar bilayers. (iii) Vesicles containing purple membranes or monomeric bacteriorhodopsin were spread on an air/water interface and, from the resulting layer, bilayers were formed. On illumination, steady-state photocurrents were observed in all three cases, indicating that these methods lead to functional transmembranous integration of the protein in the planar black lipid membrane. The influence of an applied electric field on the pumping process was studied on membranes formed by using method i. At approximately 200 mV, the photocurrent tends to zero. Furthermore, it was possible to make planar lipid bilayers photoelectrically active by adding vesicles containing monomeric bacteriorhodopsin to the bathing solution. Because, in this case, only transient photocurrents were observed, it can be concluded that the vesicles are attached to but not fused with the black lipid membrane.

Lipid--protein interactions in bacteriorhodopsin--dimyristoylphosphatidylcholine vesicles

Bacteriorhodopsin (BR) was incorporated into large unilamellar dimyristoyl- and dipalmitoylphosphatidylcholine vesicles (100--300-nm radius). The effect of this intrinsic membrane protein on the order and dynamics of the lipid and on the cooperativity and transition temperature (Tc) of the gel to liquid-crystalline phase transition was investigated as a function of the lipid:protein ratio (L/BR). The lipid phase transition induces protein segregation. Above Tc, bacteriorhodopsin is in the monomeric state. Below Tc, BR is aggregated in the same hexagonal lattice as in the purple membrane (PM). In this reconstituted system, BR has a photochemical cycle similar to that in the PM and is active as a light-driven proton pump. The lipid phase transition which was monitored by using the steady-state anisotropy of the fluorescent probe 1,6-diphenyl-1,3,5-hexatriene (DPH) broadens with decreasing L/BR but occurs at approximately the same Tc. Below Tc, the fluorescence anisotropy of DPH is quite high (0.35) and independent of the L/BR. Above Tc, however, the anisotrophy increases markedly with decreasing L/BR. It was recently pointed out that the fluorescence anisotropy of probes like DPH contains information not only on the dynamics (correlation times) but also on the order parameters of the lipids [Heyn, M. P. (1979) FEBS Lett. 108, 359--364]. The most likely explanation of the observed increase in anisotropy above Tc is that the perturbation of the lipid bilayer caused by the incorporation of BR leads both to an increase in order and to a slowing of the rotational diffusion of the lipids (increased viscosity). In agreement with this latter dynamical effect, the rotational diffusion constant of BR itself decreases above Tc with decreasing L/BR. Above Tc, the membrane viscosity as determined from the rotational diffusion constant of BR is at least 1.5 times larger than that obtained from the fluorescence depolarization of DPH. The formation of the BR lattice as a function of temperature was followed by using the circular dichroism (CD) exciton effect together with measurements of the rotational diffusion of BR. Both methods show similar transition curves for the protein crystallization whose midpoints, however, occur several degrees below Tc.

Sensory transduction in Halobacterium halobium: retinal protein pigment controls UV-induced behavioral response

Both photosystems, PS 370 and PS 565, controlling behavioral responses in Halobacterium halobium [E. Hildebrand and N. Dencher, Nature 257, 46 - 48 (1975)] are reversibly inhibited when bacteria are grown in the presence of 1 mM nicotine which is known to block biosynthesis of reti­nal.

Photobehavior can be restored within som e minutes to hours by adding retinal to nicotine-treated bacteria, PS 370 thereby reappearing earlier than PS 565. The reconstitution rate depends on the concentration and on the kind of retinal isomers applied. All-trans retinal is most effective. PS 370 becomes fully sensitive if reconstituted in the presence of nicotine. This rules out the possi­bility that the alkaloid may directly inhibit steps of signal transmission following photoreception.

The action spectrum of PS 370 regenerated with retinal alone of H. h., strain R1L3 (a mutant deficient in carotenoids), fails to show all secondary peaks around 450 nm which in strain R1 occur besides the prominent maximum at 370 nm. Addition of carotenoids (mainly α-bacterioruberin) to reconstituted cells of R1L3 restores the sensitivity in that spectral region. Carotenoids or flavin solely added to nicotine-treated bacteria cannot restore photobehavior.

We conclude that the active pigment o f PS 370, which mediates the photophobic response to increase of light intensity (step-up response), represents a retinal protein complex and that carote­noids participate in photoreceptor function as accessory pigments. The biochemical relation of the UV-absorbing retinal protein complex to bacteriorhodopsin is discussed.

Evidence for chromophore-chromophore interactions in the purple membrane from reconstitution experiments of the chromophore-free membrane

We recently presented evidence showing that the visible CD spectrum of the purple membrane from Halobacterium halobium consists of two contributions: a broad positive band centered at the absorption maximum due to the interaction of the chromophore with the protein to which it is bound, and an exciton coupling band due to the interaction between chromophores of adjacent bacteriohodopsin molecules in the hexagonal surface lattice (Heyn et al., 1975); This interpretation receives strong support from the present experiments in which the chromophore-free membrane is reconstituted by the addition of retinal. Since the coupling signal arises from the interaction between pairs of neighboring chromophores, its contribution to the spectrum would be expected to be very small in the initial stages of the titration experiment, but increasing quadratically with the percentage reconstitution. The broad positive band, on the other hand, is expected to increase linearly with the percentage reconstitution. On the basis of these considerations a satisfactory explanation of the CD reconstitution experiments could be given. Since it appears to be impossible to explain the titration experiments without the quadratic term, we conclude that chromophore-chromophore interactions play an important role. No significant changes in secondary structure upon reconstitution should be detected consistent with our binding model which neglects cooperativity;