Freeze fracture imaging and computer simulation of liposome structure: Membrane geometry and defects

Author(s):  
Joseph A. Zasadzinski

At low weight fractions, many surfactant and biological amphiphiles form dispersions of lamellar liquid crystalline liposomes in water. Amphiphile molecules tend to align themselves in parallel bilayers which are free to bend. Bilayers must form closed surfaces to separate hydrophobic and hydrophilic domains completely. Continuum theory of liquid crystals requires that the constant spacing of bilayer surfaces be maintained except at singularities of no more than line extent. Maxwell demonstrated that only two types of closed surfaces can satisfy this constraint: concentric spheres and Dupin cyclides. Dupin cyclides (Figure 1) are parallel closed surfaces which have a conjugate ellipse (r1) and hyperbola (r2) as singularities in the bilayer spacing. Any straight line drawn from a point on the ellipse to a point on the hyperbola is normal to every surface it intersects (broken lines in Figure 1). A simple example, and limiting case, is a family of concentric tori (Figure 1b).To distinguish between the allowable arrangements, freeze fracture TEM micrographs of representative biological (L-α phosphotidylcholine: L-α PC) and surfactant (sodium heptylnonyl benzenesulfonate: SHBS)liposomes are compared to mathematically derived sections of Dupin cyclides and concentric spheres.

Polymers ◽  
2020 ◽  
Vol 12 (2) ◽  
pp. 356 ◽  
Author(s):  
Ivan Budagovsky ◽  
Aleksey Kuznetsov ◽  
Sergey Shvetsov ◽  
Mikhail Smayev ◽  
Alexander Zolot’ko ◽  
...  

Dye-doped nematic side-chain liquid-crystalline polymers possess extraordinary large optical nonlinearity and ability to store the induced orientational deformations in a glassy state, which makes them a very promising material for photonic applications. In this study, the phase structures were generated and recorded in the bulk of a 50-μm layer of a nematic liquid-crystalline side-chain polymer, containing polyacrylate backbone, spacer having five methylene groups, and phenyl benzoate mesogenic fragment. The polymer was doped with KD-1 azodye. The director field deformations induced by the light beam close to the TEM01 mode were studied for different geometries of light–polymer interaction. The phase modulation depth of 2π was obtained for the 18-μm spacing between intensity peaks. The experimental data were analyzed based on the elastic continuum theory of nematics. The possibility to induce and record positive and negative microlenses in the polymer bulk was shown experimentally.


1954 ◽  
Vol 50 (4) ◽  
pp. 623-627 ◽  
Author(s):  
W. R. Dean

1. An expression in finite terms is found in §§2,3 for the small displacement of a thin elastic plate due to the application of a transverse force at an arbitrary point; the plate is infinite and is bounded internally by an ellipse along which it is clamped. The limiting case in which the ellipse degenerates to a straight line is considered in §4, and the other limiting case of a circular boundary in §5.


Author(s):  
Chang Dae Han

Volume 1 presents first fundamental principles of the rheology of polymeric fluid including kinematics and stresses of a deformable body, the continuum theory for the viscoelasticity of flexible homogeneous polymeric liquids, the molecular theory for the viscoelasticity of flexible homogeneous polymeric liquids, and the experimental methods for the measurement of the rheological properties of poylmeric liquids. The materials presented are intended to set a stage for the subsequent chapters by introducing the basic concepts and principles of rheology, from both phenomenological and molecular perspectives, ofstructurally simple flexible and homogeneous polymeric liquids. Next, this volume presents the rheological behavior of structurally complex polymeric materials including miscible polymer blends, block copolymers, liquid-crystalline polymers, thermoplastic polyurethanes, immiscible polymer blends, perticulare-filled polymers, organoclay nanocomposites, molten polymers with dissolved gas, and thermosts.


Author(s):  
Gleb L. Kotkin ◽  
Valeriy G. Serbo

This chapter addresses chain of particles connected by springs as the simplest models used in theory of solids, the travelling and standing waves on a chain, and the free and forced oscillations of N particles which are connected by springs and which can move either along a straight line or along a ring. The chapter also addresses the free and forced oscillations of 2N particles, alternating either with masses or with elastic constants; the free and forced oscillations of the artificial line with inductances and capacitors; and the elastic rod as the limiting case of the system of N particles connected by spring in the limit N tends to infinity.


1991 ◽  
Vol 46 (10) ◽  
pp. 858-864 ◽  
Author(s):  
M. Mitra ◽  
S. Paul ◽  
R. Paul

AbstractThe refractive indices (no, ne) and densities of two mesogens have been measured in their liquid crystalline and liquid phases. The molecular polarizabilities (xo, xe) were evaluated by Vuks' and Neugebauer's relations. The polarizabilities thus obtained are compared with those estimated from the bond polarizabilities, and the orientational order parameters, <P2>, are compared with the mean field theory of Maier and Saupe, the modified mean field theory of Humphries, James and Luckhurst. and the continuum theory suggested by T. E. Faber. We have also calculated the three order parameters (<P2), τ, σ) describing the smectic A phase following McMillan's model. Possible causes of the discrepancy are discussed.


Author(s):  
S. A. Walker ◽  
J. A. Zasadzinski

Nanostructured zeolites are ubiquitous throughout chemistry as catalysts and sorption media' A new variety of zeolites, constructed by templating inorganic silica on surfactant liquid crystalline phases, consist of ordered arrays of cylindrical pores with diameters ranging from 20 Å to greater than 500 Å. The nanostructure of these materials can be tailored to a variety of applications, each of which makes use of the zeolite network's large surface area and prescribed microstructure. Recent studies indicate that the initial step in the nanophase formation is a cooperative self-assembly of inorganic silicate species and organic surfactant species, dictated by ionic interaction between silicate anions and cationic surfactants. Freeze-fracture transmission electron microscopy (FF-TEM) is the only technique that can visualize this self-assembly process in situ to determine phase boundaries and examine the formation mechanism.The nanophases form on mixing aqueous cetyl trimethylammonium bromide (CTAB) with silicate (SiO2; prepared from CAB-O-SIL M-5, tetramethylammonium hydroxide (TMA-OH), trimethyl benzene (TMB), methanol (CH3OH), and water).


Author(s):  
Janet L. Burns ◽  
Matthew H. Chestnut ◽  
Richard J. Spontak

Freeze-fracture transmission electron microscopy (FF/TEM) is a well-established and highly-valued technique, often employed in the study of biological systems which are extremely sensitive to structural alteration (e.g., membranes and tissues). The technique relies on rapid specimen cooling to immobilize detailed microstructure, usually in a hydrated environment, prior to fracture and subsequent surface replication. As Zasadzinski and Bailey point out, though, the principle governing this technique is general and can be applied with equal success to the study of “microstructured” or “complex” fluids, i.e., fluids consisting of self-organized supramolecular structures. In this vein, FF/TEM constitutes a powerful means of characterizing the structural attributes of dispersions, emulsions, gels, and liquid crystalline assemblies at relatively high spatial resolution. Such morphological information can prove valuable in the development of the structure-viscosity relationships needed in processing. Here, we demonstrate the utility of FF/TEM in elucidating the role of self-associated structures in three different systems: a chemical reaction environment, a high-internal-phase emulsion, and a nonaqueous gel.


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