Kirk G. Hines

Contribution of Membrane Elastic Energy to Rhodopsin Function

We considered the issue of whether shifts in the metarhodopsin I (MI)-metarhodopsin II (MII) equilibrium from lipid composition are fully explicable by differences in bilayer curvature elastic stress. A series of six lipids with known spontaneous radii of monolayer curvature and bending elastic moduli were added at increasing concentrations to the matrix lipid 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) and the MI-MII equilibrium measured by flash photolysis followed by recording UV-vis spectra. The average area-per-lipid molecule and the membrane hydrophobic thickness were derived from measurements of the (2)H NMR order parameter profile of the palmitic acid chain in POPC. For the series of ethanolamines with different levels of headgroup methylation, shifts in the MI-MII equilibrium correlated with changes in membrane elastic properties as expressed by the product of spontaneous radius of monolayer curvature, bending elastic modulus, and lateral area per molecule. However, for the entire series of lipids, elastic energy explained the shifts only partially. Additional contributions correlated with the capability of the ethanolamine headgroups to engage in hydrogen bonding with the protein, independent of the state of ethanolamine methylation, with introduction of polyunsaturated sn-2 hydrocarbon chains, and with replacement of the palmitic acid sn-1 chains by oleic acid. The experiments point to the importance of interactions of rhodopsin with particular lipid species in the first layer of lipids surrounding the protein as well as to membrane elastic stress in the lipid-protein domain.

Elastic properties of polyunsaturated phosphatidylethanolamines influence rhodopsin function

Membranes with a high content of polyunsaturated phosphatidylethanolamines (PE) facilitate formation of metarhodopsin-II (M(II)), the photointermediate of bovine rhodopsin that activates the G protein transducin. We determined whether M(II)-formation is quantitatively linked to the elastic properties of PEs. Curvature elasticity of monolayers of the polyunsaturated lipids 18 : 0-22 : 6(n - 3)PE, 18 : 0-22 : 5(n)- 6PE and the model lipid 18 : 1(n - 9)-18 : 1,(n- 9)PE were investigated in the inverse hexagonal phase. All three lipids form lipid monolayers with rather low spontaneous radii of curvature of 26-28 angstroms. In membranes, all three PEs generate high negative curvature elastic stress that shifts the equilibrium of MI(I)/M(II) photointermediates of rhodopsin towards M(II) formation.

Rhodopsin/Lipid Hydrophobic Matching—Rhodopsin Oligomerization and Function

Lipid composition of the membrane and rhodopsin packing density strongly modulate the early steps of the visual response of photoreceptor membranes. In this study, lipid-order and bovine rhodopsin function in proteoliposomes composed of the sn-1 chain perdeuterated lipids 14:0d27-14:1-PC, 16:0d31-16:1-PC, 18:0d35-18:1-PC, or 20:0d39-20:1-PC at rhodopsin/lipid molar ratios from 1:70 to 1:1000 (mol/mol) were investigated. Clear evidence for matching of hydrophobic regions on rhodopsin transmembrane helices and hydrophobic thickness of lipid bilayers was observed from (2)H nuclear magnetic resonance order parameter measurements at low rhodopsin concentrations. Thin bilayers stretched to match the length of transmembrane helices observed as increase of sn-1 chain order, while thicker bilayers were compressed near the protein. A quantitative analysis of lipid-order parameter changes suggested that the protein adjusts its conformation to bilayer hydrophobic thickness as well, which confirmed our earlier circular-dichroism measurements. Changes in lipid order parameters upon rhodopsin incorporation vanished for bilayers with a hydrophobic thickness of 27 ± 1 Å, suggesting that this is the bilayer thickness at which rhodopsin packs in bilayers at the lowest membrane perturbation. The lipid-order parameter studies also indicated that a hydrophobic mismatch between rhodopsin and lipids triggers rhodopsin oligomerization with increasing rhodopsin concentrations. Both hydrophobic mismatch and rhodopsin oligomerization result in substantial shifts of the equilibrium between the photointermediates metarhodopsin I and metarhodopsin II; increasing bilayer thickness favors formation of metarhodopsin II while oligomerization favors metarhodopsin I. The results highlight the importance of hydrophobic matching for rhodopsin structure, oligomerization, and function.

Significance of an opiate mechanism in the adjustment of cerebrocortical oxygen consumption and blood flow during hypercapnic stress.

The role of adrenal medulla-derived enkephalins in the control of hypercapnic cerebrocortical blood flow (CBF) and oxygen consumption (CMRO2) was investigated in the ketamine anesthetized rat. Three experimental interventions were utilized: inhibition of opioid receptors with naloxone, decrease of adrenal enkephalin production with chronic adrenal medullectomy, and treatment of adrenal demedullated animals with the synthetic enkephalin analog, D-Ala2, N-Me-Phe4, Gly5-ol-enkephalin (DAGO). In intact, untreated animals hypercapnia increased CBF and CMRO2 by approximately 300 and 35%, respectively. Naloxone reduced the hypercapnic increase of CBF, and transformed the hypercapnic increase of CMRO2 into a decrease. The mid-points of the dose-response curves for (1)-naloxone and (d)-naloxone were 10 micrograms/kg and 100 micrograms/kg, respectively. Adrenal demedullation and treatment with (1)-naloxone (0.2 mg/kg) decreased the hypercapnic CBF and CMRO2 by approximately 50%. DAGO treatment of adrenal demedullated animals restored the hypercapnic CBF and CMRO2 to values similar to those found in intact animals. These observations suggest that opioid peptides (most likely adrenal medulla-derived enkephalins) play a significant role in the regulation of CMRO2 and CBF during moderate hypercapnia.

Controlling GPCR Rhodopsin Function by Small, Physiologically Relevant Changes in Bilayer Hydrophobic Thickness

It was established previously that the G protein-coupled membrane receptor rhodopsin has transmembrane helices which match a hydrophobic bilayer thickness of 27±1 A. Here we demonstrate that small changes of bilayer thickness of ±2 A about that match point translate in the considerable changes of rhodopsin activation measured as the metarhodopsin I (MI)/metarhodopsin II (MII) equilibrium. We observed a biphasic behavior of the MI/MII equilibrium, with a sharp decline towards MI from 25-27 A followed by a rapid increase of MII from 27-29 A. Results are qualitatively identical for thickness changes induced by mixing of 16:0-16:1 PC and 18:0-18:1 PC, or 16:1-16:1 PC and 18:1-18:1 PC, or addition of 0-30 mol% cholesterol to 16:0-16:1 PC. The biphasic behavior was observed regardless of lipids used to alter bilayer hydrophobic thickness suggesting a relationship between small changes in hydrophobic thickness and rhodopsin function. It strongly favors an explanation based on a change of elastic stresses in lipid bilayers upon the transition from negative curvature in lipid monolayers near the protein below 27 A hydrophobic thickness to positive monolayer curvature above the match point. A continuum elastic model of the membrane, including the effect of lipid monolayer curvature near the protein, predicts membrane mediated clustering of rhodopsin and stabilization of the MI photointermediate at the matching point. Small, physiologically relevant changes in cholesterol content of bilayers with a thickness in the physiologically relevant range do drastically down- or up regulate the amount of MII which is the state that activates G protein.

Cholesterol Enhances or Reduces Metarhodopsin II Formation Depending on Bilayer Thickness

Cholesterol is one of the most efficient modulators of G Protein-Coupled Receptor (GPCR) function. We monitored the effect of cholesterol on rhodopsin function for a set of bilayers with different hydrophobic thickness. Surprisingly, cholesterol shifts the Metarhodopsin-I (MI)/Metarhodopsin-II (MII) equilibrium toward MII for bilayers thinner than the average length of hydrophobic transmembrane helices (2.7 nm), and to MI for thicker bilayers. In previous work conducted on rod outer segment disks and model membranes, increasing cholesterol concentration always shifted the equilibrium towards MI. It was proposed that the cholesterol effect is primarily related to a tighter packing of lipid hydrocarbon chains which generates a less permissive environment for the formation of MII. To gain deeper insights into mechanisms, we followed changes in lipid-rhodopsin interaction by 2H NMR using deuterated lipids. It was reported by us and the Brown laboratory that an increase of bilayer hydrophobic thickness in the absence of cholesterol favors MII with a turnover to MI for bilayers that are very thick. Indeed, the cholesterol-induced shifts towards MII for thinner membranes correlated nicely with the cholesterol-induced increase of bilayer hydrophobic thickness measured by NMR suggesting that the increase in bilayer thickness by cholesterol plays a major role in controlling the energetics of the MI-MII equilibrium. Furthermore, changes in average lipid order parameters due to the presence of rhodopsin were much larger in cholesterol-containing membranes than in cholesterol-free membranes suggesting strongly that the perturbation in the lipid matrix from protein insertion reaches much further away from the protein. This is expected for membranes that are stiffer due to the presence of cholesterol. The consequences of these findings for lipid mediated shifts in rhodopsin function and rhodopsin-rhodopsin interactions will be discussed.