Resonance Raman spectra of chlorophylls dissolved in liquid crystal matrices. I. The interaction between chlorophylls and a liquid crystalline MBBA + EBBA mixture

The resonance Raman (RR) spectra of chlorophyll (Chl) a, Chl b and pheophytin a dissolved in a liquid-crystalline MBBA + EBBA mixture were measured. The RR frequencies of chlorophylls in the liquid crystal (LC) are compared with those of solutions of various chlorophyll monomers and aggregates taken from the literature. It is concluded that Chl a and Chl b in LC exist largely as the solvated monomers, even at high concentration. The magnesium atoms in both Chl a and Chl b are pentacoordinated.     

Spectral properties of chlorophyll a in liquid crystal

Solution of chlorophyll a in liquid crystals mixture (MBBA + EBBA) was investigated. Chl molecules are in LC in low electric field oriented. They can be divided into two groups: one strongly interacting with LC and subjected to reorientation by the electric field, and another weakly interacting with the solvent and insensitive to the voltage applied. The emission spectrum of the first type of chlorophyll is strongly perturbed. At higher voltages, the pigment molecules orientation in the plane of the electrode is another. Pigment absorption and emission anisotropy provides information about the reorientation of LC molecules. Even at high (10^?3M) Chl concentration and regular pigment array, the interaction between the pigment and solvent exceeds pigment-pigment interaction because the solvent appears to have a stronger influence on the Chl spectrum.     

Resonance Raman spectra of chlorophylls dissolved in liquid crystal matrices. III. Orientational distribution function of chlorophyll b in an MBBA + EBBA liquid crystalline matrix

Polarized resonance Raman spectra of chlorophyll (Chl) b oriented in a mixture of p-methoxybenzylideno-p'-butylaniline (MBBA) and p-ethoxybenzylideno-p'-butylaniline (EBBA) have been measured. The spectra have been analyzed and the second- and fourth-rank order parameters and the orientational distribution function of Chl b are presented.     

Circular dichroism and magnetic circular dichroism spectra of chlorophylls a and b in nematic liquid crystals. II. Magnetic circular dichroism spectra

Absorption and magnetic circular dichroism (MCD) spectra are reported for chlorophyll (Chl) a and Chl b dissolved in nematic liquid crystal solvents. The spectra were measured with the dye molecules oriented uniaxially along the direction of. the magnetic field and measuring light beam. It is significant that under such conditions the MCD spectra recorded in the wavelength region of the Q and Soret bands of the chlorophyll are essentially unchanged with respect to rotation of the sample cell around this axis, even though there is almost complete orientation of the chlorophyll molecules by the liquid crystals. The MCD spectra of Chl a and b in the nematic liquid crystal solvents used in this study are surprisingly similar to the spectra obtained under isotropic conditions. These results illustrate an important technique with which to examine the optical spectra of dyes oriented in liquid crystal matrices in which the anisotropic effects can be reduced the negligible proportions by the application of a strong magnetic field parallel to the direction of the measuring light beam. The first deconvolution calculations are reported that describe the deconvolution of pairs of absorption and MCD spectra, in the Q and B band regions, for both Chl a and b. The spectral analysis to obtain quantitative estimates of transition energies was accomplished by carrying out detailed deconvolution calculations in which the both the absorption and MCD spectral envelopes were fitted with the same number of components; each pair of components had the same hand centres and bandwidth values. This procedure resulted in an assignment of each of the main transitions in the absorption spectra of both Chl a and b. Chl a is clearly monomeric, with Qy, Qx, By and Bx located at 671, 582, 439 and 431 nm, respectively. Analysis of the spectral data for Chl b located Qy, By and Bx, at 662, 476 and 464 nm, respectively.     

Aggregation of chlorophylls in monolayers. VI. Infrared study of the CH stretching bands of chlorophyll a and of chlorophyll b in monolayers

The CH vibrational stretch bands of chlorophyll (Chl) in monolayers, obtained by the Langmuir-Blodgett technique have been studied by infrared spectroscopy. Compared to a solution or to a multilayer which shows three to four bands, the spectra of Chl a or Chl b molecules in monolayers have revealed more than seven bands, which are assigned to the various CH groups in the molecule. In contrast to solutions or to multilayer samples which give featureless bands, each band of the monolayers is composed of many components which are modified when the system is perturbed either by drying or by hydration techniques. The separation between the components of the CH aliphatic bands is typical of crystalline field splitting and the modification of the intensities of these components is associated with the movement of the phytyl chain of the chlorophyll molecules. The CH aromatic stretch bands have been observed; the displacement and variation of the intensities of these bands are associated with deformation of the porphyrin ring. The CH band of the formyl group on Chl b has also been observed. The displacement and variation of the intensity of this band are related to the association that this group makes with the surrounding molecules and with the displacement of the porphyrin ring.     

Formation of liquid crystalline phase of actin filament solutions and its dependence on filament length as studied by optical birefringence.

We studied the formation and structure of liquid crystalline phase of F-actin solutions by polarized light photometry, assuming that a small domain of the liquid crystalline phase works as a linear retardation plate. Transmittance of polarized light due to the birefringence of liquid crystalline phase appeared above a threshold concentration of F-actin. The threshold increased with a decrease in filament length, which was regulated by calcium-activated gelsolin. The intensity increased linearly with increasing concentrations until it reached a stationary value. The deviation of optical axis direction of the putative retardation plate was estimated 7-15 degrees. These results indicate that:(a) the liquid crystalline phase is formed above a threshold concentration of F-actin; (b) the threshold is proportional to the inverse of filament length; (c) the ordered phase coexists with the isotropic one, increasing the volume fraction with increasing concentrations until all filaments take the liquid crystalline structure; (d) the filaments in liquid crystalline phase take a highly ordered array. These results can be attributed to the excluded volume effect of rod-like molecules on the formation of liquid crystalline structure.     

Theoretical conformational analysis of phospholipids. II. Role of hydration in the gel to liquid crystal transition of phospholipids

To obtain a satisfactory agreement between computed transition temperatures and those determined experimentally, we introduce explicitly water molecules which hydrate the polar headgroup of dipalmitoylphosphatidylethanolamine molecules. The calculated free energy curves as a function of the intermolecular interchain distance and the degree of hydration of the polar groups permit the determination of the transition of the phospholipid system from the gel to the liquid crystalline phase. The detailed structure of the hydration shell is defined using the supermolecular approach.     

Interdigitation does not affect translational diffusion of lipids in liquid crystalline bilayers.

Asymmetric phosphatidylcholine molecules with one acyl chain twice as long as the other, below their phase transition temperature, from a mixed interdigitated phase in which the longer acyl chain spans the entire bilayer. Experimental evidence in the literature suggests that, above their phase transition temperature, these molecules may still exhibit partial interdigitation, with the longer acyl chain extending partially into the opposite leaflet, and are packed more tightly than equivalent symmetric phosphatidylcholines. Using the fluorescence recovery after photobleaching technique, we have investigated the translational diffusion in multilayers of a liquid crystalline phase, asymmetric phosphatidylcholine, 1-stearoyl-2-capryl-phosphatidylcholine (C18C10PC). We used as a fluorescent probe either a phospholipid analog of the same acyl chain composition, NBD-C18C10PE, or the symmetric equivalent of the same molecular weight, N-(7-nitrobenzoxa-2,3-diazol-4-yl)-dimyristoyl-phosphatidyle thanolamine (NBD-DMPE). Translational diffusion coefficients were also determined by using both probes in multilayers of dimyristoyl-phosphatidylcholine (DMPC) and in the eutectic mixture DMPC/C18C10PC (40/60 mol). We found that in a given host lipid, NBD-C18C10PE and NBD-DMPE diffuse at the same rate, which suggests that their bilayer free area is almost identical. This result can be explained by considering that in the liquid crystalline state, the increase in molecular packing is compensated by an increase in acyl chain dynamics. This view, which is supported by literature data, clearly suggests that the acyl chain interdigitation occurring in the liquid crystalline phase is highly dynamic.     

Electron microscopy of liquid crystalline DNA: direct evidence for cholesteric-like organization of DNA in dinoflagellate chromosomes

Freeze-fracture-etch replicas of concentrated DNA solutions which appeared, by polarized light microscopy, to be in a cholesteric-like liquid crystalline state were examined by high resolution transmission electron microscopy (TEM). Individual DNA molecules were resolvable, and the microscopic morphologies observed for such replicas confirmed the cholesteric organization of DNA molecules in this liquid crystalline state. Furthermore, replica morphologies were strikingly similar to TEM images of dinoflagellate chromosomes in both thin section and freeze-etch replicas, providing strong support for the cholesteric DNA packing model proposed for the organization of DNA in these chromosomes by Bouligand and Livolant.     

Theoretical conformational analysis of phospholipids II. Role of hydration in the gel to liquid crystal transition of phospholipids

To obtain a satisfactory agreement between computed transition temperatures and those determined experimentally, we introduce explicitly water molecules which hydrate the polar headgroup of dipalmitoylphosphatidylethanolamine molecules. The calculated free energy curves as a function of the intermolecular interchain distance and the degree of hydration of the polar groups permit the determination of the transition of the phospholipid system from the gel to the liquid crystalline phase. The detailed structure of the hydration shell is defined using the supermolecular approach.     

Thermodynamic model of the formation of bridges between nucleic acid molecules in a liquid crystal]

A thermodynamic model of the formation of bridges consisting of alternating daunomycin molecules and copper ions and connecting neighboring nucleic acid molecules in a particle of a liquid crystalline dispersion was constructed. The model is based on the conception that ligands are adsorbed on lattices of reaction centers which are formed in a liquid crystal at a particular spatial arrangement of adjacent nucleic acid molecules (phasing). Equations were derived that describe typical experimentally obtained S-shaped dependences of bridge concentration on the concentration of copper ions and daunomycin molecules in an initial solution. It was shown that dependences of this kind take place in two variants of the adsorption model: when the binding of daunomycin with adjacent nucleic acid molecules is considered to be independent on the formation of bridges and when bridges compete with single daunomycin molecules for the sites on adjacent nucleic acid molecules.     

A liquid crystalline phase in spermidine-condensed DNA.

Over a large range of salt and spermidine concentrations, short DNA fragments precipitated by spermidine (a polyamine) sediment in a pellet from a dilute isotropic supernatant. We report here that the DNA-condensed phase consists of a cholesteric liquid crystal in equilibrium with a more concentrated phase. These results are discussed according to Flory's theory for the ordering of rigid polymers. The liquid crystal described here corresponds to an ordering in the presence of attractive interactions, in contrast with classical liquid crystalline DNA. Polyamines are often used in vitro to study the functional properties of DNA. We suggest that the existence of a liquid crystalline state in spermidine-condensed DNA is relevant to these studies.     

Molecular dynamics simulation of lipid packing and mobility in bilayer membranes

A model of lipid bilayer membrane in water has been developed. Parameters have been selected that allow molecular dynamics simulation of lipid bilayers in the all-atom approximation. The calculated indices of packing and mobility of lipid molecules for the liquid crystalline state of the bilayer agree well with the experimental data. Based on the model of the liquid crystalline state of the membrane, a system in the gel-like state has been constructed. The gel-state model reproduces well the packing of lipids in real bilayers, whereas the mobility of molecules proves to be overestimated.     

Origin of the chlorophyll b formyl oxygen in Chlorella vulgaris.

Chlorophyll (Chl) b is an accessory light-harvesting pigment of plants and chlorophyte algae. Chl b differs from Chl a in that the 3-methyl group on ring B of chl a is replaced by a 3-formyl group on Chl b. The present study determined the biosynthetic origin of the Chl b formyl oxygen in in vivo labeling experiments. A mutant strain of the unicellular chlorophyte Chlorella vulgaris, which can not synthesize Chls when cultured in the dark but rapidly greens when transferred to the light, was grown in the dark for several generations to deplete Chls, and then the cells were transferred to the light and allowed to form Chls in a controlled atmosphere containing 18O2. Chl a and Chl b were purified from the cells and analyzed by high-resolution mass spectroscopy. Analysis of the mass spectra indicated that over 76% of the Chl a molecules had incorporated an atom of 18O. For Chl b, 58% of the molecules had incorporated an atom of 18O at one position and 34% of the molecules had incorporated an atom of 18O at a second position. These results demonstrate that the isocyclic ring keto oxygen of both Chl a and Chl b, as well as the formyl oxygen of Chl b, is derived from O2.     

Molecular dynamics simulation of packing and mobility of lipids in bilayer membranes

A model of DSPC lipid membrane in gel and liquid-crystalline states has been developed. The parameters have been determined that enable one to calculate the molecular dynamics of lipid bilayers in the full-atromic approximation. The parameters of packing and mobility of lipid molecules for the liquid crystalline state of the bilayer have been calculated. The values agree well with experimental data. Based on the model of the liquid crystalline state of the membrane, a system in the gel-like state has been constructed. The model of the gel-like state reproduces well the packing of lipids in real bilayers, whereas the mobility of molecules in the gel-like state was found to be overestimated.     

Deuterium magnetic resonance study of the gel and liquid crystalline phases of dipalmitoyl phosphatidylcholine.

Deuterium magnetic resonance is applied to the study of the liquid crystalline and gel phases, and of the phase transition, of a multilamellar dispersion of chain perdeuterated (d62)-dipalmitoyl phosphatidylcholine/H2O. Analysis of the deuterium spectra in terms of the moments of the spectra allows one to make quantitative statements concerning the distribution of quadrupolar splittings even in complicated situations, e.g., when using perdeuterated sampled or when there are mixed phases. This analysis indicates that d62-dipalmitoyl phosphatidylcholine in excess H2O undergoes a sharp phase transition (with a width of less than 1 degree C) at approximately 37 degrees C and that there appears to be hysteresis in the phase transition of approximately 1 degree C. In the lamellar liquid crystalline phase above 37 degrees C the spectra show a number of well-resolved features whose quadrupolar splittings can be followed as the temperature is varied. The gel phase near 20 degrees C possesses a very broad, almost featureless spectrum that does not seem to support a model of the gel phase wherein the hydrocarbon chains are fully extended in the all-trans conformation. At temperatures near 0 degrees C the spectra clearly indicate that a large fraction of the lipid molecules cease the rotation about their long axes, giving a spectrum more characteristic of a rigid or solid sample. These results give a picture of the gel phase as a phase characterized by considerable hydrocarbon chain disorder near 20 degrees C and becoming a more solid-like phase near 0 degrees C. The spin-lattice relaxation time, T1, has been measured at 20 degrees C in the gel phase, and at 37 and 45 degrees C in the liquid crystalline phase. The values of T1 obtained for each of the resolvable peaks in the spectrum at 37 degrees C are compared to the values (for each peak) of T2e, the decay time of the quadrupolar echo, obtained at the same temperature. These results are discussed in terms of a simple two-motion model.     

Quantitative analysis of molecular orientation in chlorophyll a Langmuir monolayer: a polarized visible reflection spectroscopic study.

Polarized visible reflection spectra of a chlorophyll a (Chl.a) Langmuir monolayer have been measured in situ at various surface pressures. By applying Hansen's optics to the three-phase plane-bounded system (air/Chl.a monolayer/water), the negative reflection absorbances observed were reproduced satisfactorily by the theoretical calculation. Molecular orientation of Chl.a in the monolayer was evaluated quantitatively as a function of surface pressure, from the reflection absorbance of p- and s-polarized spectra of the red (Qy) band. It has been proven that Chl.a molecules in the monolayer form aggregates (islands) even in the low surface pressure region and that during the monolayer compression the molecules are gradually reorganized from inhomogeneous islands to ordered structures, with the chromophores oriented on the average vertically to the water surface.     

Proton NMR bandshape studies of lamellar liquid crystals and gel phases containing lecithins and cholesterol.

Proton NMR spectra for gel and liquid crystalline samples, composed of dimyristoyl and/or dipalmitoyl lecithin, cholesterol and water, can be consistently interpreted in terms of mesophase symmetry and molecular diffusion according to a model proposed by Wennerstrom (Wennerstrom, H. (1973) Chem. Phys. Lett. 18, 41-44). It is shown by computer simulation that the characteristic "super-lorentzian" bandshape of the lamellar mesophase can be described by the superposition of three gaussian curves. The NMR signal of the gel phase can be simulated by the superposition of two gaussian curves with widths at half height of 2.5 kHz and 19 kHz. An upper limit of the lateral diffusion coefficient of the lecithin molecules in the gel phase is calculated to be about 5-10(-15) m-2/s. It is therefore concluded that the static intermolecular dipolar couplings average to zero in the lamellar mesophase. An estimation of the order parameter of the liquid crystalline phase is made from experimental data and a calculated "rigid lattice" linewidth. A two phase system is shown to exist in the temperature range 28-34 degrees C for a mesophase of a mixture of dimyristoyl and dipalmitoyl lecithin. The presence of cholesterol results in enhanced lateral diffusion of the lecithin molecules at temperatures below the Chapman transition point.     

Liquid crystallinity in condensed type I collagen solutions. A clue to the packing of collagen in extracellular matrices.

We recently described a new type of assembly of collagen molecules, forming typical liquid crystalline phases in highly concentrated solutions after sonication. The present work shows that intact 300 nm long collagen molecules also form cholesteric liquid crystalline domains, but the time required is much longer, several weeks instead of several days. Differential calorimetry and X-ray diffraction show that sonication does not alter the triple-helical structure of the collagen fragments. In the viscous solutions, observed between crossed polars in optical microscopy, the textures vary as a function of the concentration. Molecules first align near the air interface at the coverslip edge, then as the concentration increases by slow evaporation of the solvent, the birefringence extends inwards and liquid crystalline domains progressively appear. For concentrations estimated to be above 100 mg/ml, typical textures and defects of cholesteric phases are obtained, at lower concentrations zig-zag extinction patterns and banded patterns are observed; all these textures are described and interpreted. The cholesteric packing of collagen fibrils in various extracellular matrices is known, and the relationship that can be made between the ordered phases obtained with collagen molecules in vitro and the related geometrical structures observed between fibrils in vivo is thoroughly discussed.