Location of the basal disk and a ringlike cytoplasmic structure, two additional structures of the flagellar apparatus of Wolinella succinogenes.

The basal body of Wolinella succinogenes consists of a central rod, a set of two rings (L and P rings), a basal disk from 70 to 200 nm in diameter, and a terminal knob. In negatively stained preparations of flagellar hook-basal body complexes, some disks remain fixed perpendicularly to the grid and show that such a disk is located on the distal side of the P ring. The basal disks have been isolated with and without the P ring; in both cases there is a hole in the center of the disk. The diameter of the disk is smaller in the presence of the P ring. The L-P ring complex is therefore assumed to be a bushing for the rod. Thin sections of whole bacteria and spheroplasts reveal that the disk is attached to the inner surface of the outer membrane. At the insertions of the flagellar hook-basal body-basal disk complexes, depressions are visible in negatively stained preparations of whole bacteria and spheroplasts. A new ringlike structure is connected to an elongation of the basal body into the cytoplasm in both preparations. Its diameter (60 nm) is larger than that of the M ring. A heavily stained compartment can be seen in between the new ringlike structure and the basal disk, which may be formed by the energy transducing units.     

Survismeter--type I and II for surface tension, viscosity measurements of liquids for academic, and research and development studies

For centuries surface tension (gamma) and viscosity (eta) data have been measured with individual instruments consuming much time and materials. Thus the two different types of survismeters have been designed and made of borosil glass material for surface tension and viscosity data to rationalize frictional and cohesive forces, respectively. Friccohesity (sigma (sm(-1), second per meter)) is derived from Fric of frictional and cohesity of cohesive forces of the liquid respectively, and denoted by rational coefficient a eta/gamma (sigma). The values of the friccohesity are correlated to the dipole moment of liquids and their plot gives a standard calibration curve along with an equation of the curve with definite values of the coefficients, the friccohesity values are put on the calibration curve to retrieve the dipole moment values. Here, the sigma values for each of dimethylformamide, dimethylsulfoxide and acetronitrile solvents along with their 0.05, 0.10 and 0.20 mol kg(-1) aqueous solutions, respectively, were determined at 293.15K and plotted against their dipole moment values for standard calibration curve. The range of the dipole moment values for calibration curve is pre-decided and the sigma values for homogenous solutions of compositions below their saturation point can be measured with +/-1 x 10(-5)sm(-1).     

Surface forces in lungs. I. Alveolar surface tension-lung volume relationships

Alveolar surface tension (gamma)-lung volume relationships were obtained for quasi-static and dynamic lung pressure-volume (PV) histories from measurements of PV curves of liquid- and air-filled excised rabbit lungs. PV relationships were measured at room temperature in lungs filled with test liquids with constant liquid-liquid interfacial tensions with alveolar surface-active materials; and air-filled lungs before and after the normal alveolar surface film was covered with test liquids with constant values of liquid- and air-liquid interfacial tensions. Interfacial tensions of test liquids were measured in a surface balance on monolayers of dipalmitoyl phosphatidylcholine. Values of gamma for the normal air-filled lung were obtained either from points of intersection between PV curves with the normal and test liquid interface or from a general relationship between gamma and the component of recoil pressure due to surface tension derived from the data. In contrast to previous analyses that have used PV measurements, this approach does not depend on assumptions about lung microstructural geometry. Surface tension-volume relationships for the normal air-filled lung show a prominent hysteresis with surface tension ranging from near 0 at low volumes during lung deflation to transiently high values near 40 dyn/cm during inflation; value of equilibrium surface tension (gamma EQ) near 28 dyn/cm; and characteristic transitions in surface film compressibility and associated transitions in film kinetic behavior in nonequilibrium film states where gamma deviates from gamma EQ. These features are consistent with the behavior predicted from current models of alveolar surface film behavior.     

Migration-Directing Liquid Properties of Embryonic Amphibian Tissues

Deep ectoderm, mesoderm and endoderm excised from gastrulatingamphibian embryos spontaneously undergo liquid-like movementsin organ culture. Cell populations of these tissues on nonadhesivesubstrata will round up into spheres, spread over one anotherand segregate (sort out) from one another just as immiscibleliquid droplets do. In ordinary liquids, movements like theseare controlled by surface tensions; perhaps surface tensionsalso control the similar movements of liquid-like tissues. Onenecessary condition for tissue surface tension analysis is thatthe tissue must be able (just as ordinary liquids are able)to spontaneously relax internal stretching forces (shear stresses).When cellular aggregates of the germ layers were deformed bygentle compression between parallel glass plates, cells withinthe aggregates were initially stretched. However, the cellssoon returned to their original undistorted shapes. Thus, cellstretching forces were gradually relaxed by cell rearrangements.The in vitro spreading movements of the deep germ layers implythat the surface tension of ectoderm should be greater thanthe surface tension of mesoderm which should be greater thanthe surface tension of endoderm. Quantitative measurements oftissue surface tensions made by parallel plate compression confirmprecisely that relationship. Furthermore, the surface tensionsof these tissues remain constant regardless of the amount ofaggregate flattening—another necessary condition for validsurface tension measurements. These results demonstrate thatamphibian deep germ layers possess fundamental liquid propertieswhich are sufficient to direct their liquid-like rearrangementsin organ culture. Furthermore, I also report that one of theseproperties, surface tension, displays a preliminary correlationwith density of cell surface charge (assessed by electrophoreticmobility) and with the onset of in vivo mesodermal involution.     

Differential scanning calorimetry of bovine rhodopsin in rod-outer-segment disk membranes.

Rhodopsin-containing retinal rod disk membranes from cattle have been examined by differential scanning calorimetry. Under conditions of 67 mM phosphate pH 7.0, unbleached rod outer segment disk membranes gave a single major endotherm with a temperature of denaturation (Tm) of 71.9 +/- 0.4 degrees C and a thermal unfolding calorimetric enthalpy change (delta Hcal) of 700 +/- 17 kJ/mol rhodopsin. Bleached rod outer segment disk membranes (membranes that had lost their absorbance at 498 nm after exposure to orange light) gave a single major endotherm with a Tm of 55.9 +/- 0.3 degrees C and a delta Hcal of 520 +/- 17 kJ/mol opsin. Neither bleached nor unbleached rod outer segment disk membranes gave endotherms upon thermal rescans. When thermal stability is examined over the pH range of 4-9, the major endotherms of both bleached and unbleached rod outer segment disk membranes were found to show maximum stability at pH 6.1. The observed delta Hcal values for bleached and unbleached rod outer segment disk membranes exhibit membrane concentration dependences which plateau at protein concentrations beyond 1.5 mg/mL. For partially bleached samples of rod outer segment disk membranes, the calorimetric enthalpy change for opsin appears to be somewhat dependent on the degree of bleaching, indicating intramembrane nearest neighbor interactions which affect the unfolding of opsin. Delta Hcal and Tm are particularly useful for assessing stability and testing for completeness of regeneration of rhodopsin from opsin. Other factors such as sample preparation and the presence of low concentrations of ethanol also affect the delta Hcal values while the Tm values remain fairly constant. This shows that the delta Hcal is a sensitive parameter for monitoring environmental changes of rhodopsin and opsin.     

Improvement of foam breaking and oxygen-transfer performance in a stirred-tank fermenter

This study examined a stirred-tank fermenter (STF) containing low-viscosity foaming liquids with an agitation impeller and foam-breaking impeller mounted on the same shaft. Results showed that the performance of the foam-breaking impeller can be improved by changing a conventional six-blade turbine impeller into a rod impeller as the agitation impeller. The volumetric oxygen-transfer coefficient, k _L a, in the mechanical foam-control method (MFM) using a six-blade vaned disk as the foam-breaking impeller in the STF with the rod impeller was approximately five times greater than that of the chemical foam-control method (CFM) adding an anti-foaming agent in the STF with the six-blade turbine impeller. Application of the present method to the cultivation of Saccharomyces cerevisiae K-7 demonstrated that the cultivation time up to the maximum cell concentration was remarkably shorter than that achieved using a conventional CFM.     

Mechanical control of foaming in a bubble column

This study was performed to evaluate the effects of the air sparge rate, working liquid volume, liquid feed rate onto the disk, and disk diameter on the foam-breaking performance of foam-breaking apparatus with a rotating disk (FARD) installed in the bubble column. Experimental results showed that the smaller the air sparge rate and working liquid volume were, and the larger the liquid feed rate and disk diameter, the lower the critical disk rotational speed required for reduced foam-breaking. The presence of the effective ranges of the disk diameter and liquid feed rate for foam breaking was also confirmed. Furthermore, the quantitative predictions of the upper limits of the liquid feed rate, foam-breaking regions, and the required foam-breaking power were carried out, based on the results obtained above. Comparison of the FARD with two conventional mechanical foam-breaking spray-type apparati also demonstrated the highest level of the FARD in respect not only to foam-breaking performance but also to power requirements.     

Penetration of stomata by liquids: dependence on surface tension, wettability, and stomatal morphology

Wettability of the leaf surface, surface tension of the liquid, and stomatal morphology control penetration of stomata by liquids. The critical surface tension of the lower leaf surface of Zebrina purpusii Brückn. was estimated to be 25 to 30 dyne cm⁻¹. Liquids having a surface tension less than 30 dyne cm⁻¹ gave zero contact angle on the leaf surface and infiltrated stomata spontaneously while liquids having a surface tension greater than 30 dyne cm⁻¹ did not wet the leaf surface and failed to infiltrate stomata. Considering stomata as conical capillaries, we were able to show that with liquids giving a finite contact angle, infiltration depended solely on the relationship between the magnitude of the contact angle and the wall angle of the aperture. Generally, spontaneous infiltration of stomata will take place when the contact angle is smaller than the wall angle of the aperture wall. The degree of stomatal opening (4, 6, 8, or 10 μm) was of little importance. Cuticular ledges present at the entrance to the outer vestibule and between the inner vestibule and substomatal chamber resulted in very small if not zero wall angles, and thus played a major role in excluding water from the intercellular space of leaves. We show why the degree of stomatal opening cannot be assessed by observing spontaneous infiltration of stomata by organic liquids of low surface tension.     

The impact of line tension on the contact angle of nanodroplets

The line tension for a Lennard–Jones (LJ) fluid on a (9, 3) solid of varying strength was calculated using Monte Carlo simulations. A new perturbation method was used to determine the interfacial tension between liquid–vapour, solid–liquid and solid–vapour phases for this system to determine the Young's equation contact angle. Cylindrical and spherical nanodroplets were simulated for comparison. The contact angles from the cylindrical drops and Young's equation agree very well over the range of surface strengths and cylindrical drop sizes, except on a very weak surface. Tolman length effects were not observable for cylindrical drops. This shows that quite small systems can reproduce macroscopic contact angles. For spherical droplets, a deviation between the contact angle of spherical droplets and Young's equation was evident, but decreased with increasing interaction strengths to be negligible for contact angles less than 90°. Linear fitting of the contact angle data for varying droplet sizes showed no clear effect by line tension on contact angle. All calculated line tension values have a magnitude less than 4 × 10^? 12 J/m with both negative and positive signs. The best estimate of line tension for this system of LJ droplets was 1 × 10^? 13 J/m, which is smaller than the reported estimations in the literature, and is too small to be conclusively positive or negative in value.     

Micropipette aspiration of living cells

The mechanical behavior of living cells is studied with micropipette suction in which the surface of a cell is aspirated into a small glass tube while tracking the leading edge of its surface. Such edges can be tracked in a light microscope to an accuracy of +/-25 nm and suction pressures as small as 0.1-0.2 pN/microm2 can be imposed on the cell. Both soft cells, such as neutrophils and red cells, and more rigid cells, such as chondrocytes and endothelial cells, are studied with this technique. Interpretation of the measurements with basic continuum models leads to values for a cell's elastic and viscous properties. In particular, neutrophils are found to behave as a liquid drop with a cortical (surface) tension of about 30 pN/microm and a viscosity on the order of 100 Pa s. On the other hand, chondrocytes and endothelial cells behave as solids with an elastic modulus of the order of 500 pN/microm2 (0.5 kPa).     

Thermodynamic aspects of plant cell adhesion to polymer surfaces

Summary A thermodynamic model of particle adhesion from a suspension onto a solid surface is used to predict the extent of adhesion of suspension-cultured Catharanthus roseus cells to the following polymer substrates: fluorinated ethylene-propylene (FEP), polystyrene (PS), polyethylene terephthalate (PET), sulphonated polystyrene (SPS), and glass. According to this model, the extent of adhesion is determined by the surface tensions of the plant cells, the polymer substrates, and the suspending liquid medium. Experimentally, adhesion of the washed plant cells was found to decrease with increasing substrate surface tension, following the sequence FEP>PS>PET>SPS>glass, when the surface tension of the liquid was greater than that of the plant cells, in agreement with the model. However, adhesion increased with increasing substrate surface tension when the liquid surface tension was lower than the cellular surface tension, also in agreement with the model. When the liquid and cellular tensions were equal the extent of adhesion was independent of the substrate surface tension. This also agrees with model predictions and leads to a value for the surface tension of C. roseus cells of approximately 54 ergs/cm² which is in agreement with a value obtained from contact angle measurements on layers of cells and sedimentation volume analysis. The cellular surface tension determined by the sedimentation volume method showed a biphasic alteration during growth cycles of C. roseus cell cultures. These variations (between 55 and 58 ergs/cm²) agree with the pattern of adhesion previously described.     

Metastability of a supercompressed fluid monolayer

Previous studies showed that monomolecular films of extracted calf surfactant collapse at the equilibrium spreading pressure during quasi-static compressions but become metastable at much higher surface pressures when compressed faster than a threshold rate. To determine the mechanism by which the films become metastable, we studied single-component films of 1-palmitoyl-2-oleoyl phosphatidylcholine (POPC). Initial experiments confirmed similar metastability of POPC if compressed above a threshold rate. Measurements at different surface pressures then showed that rates of collapse, although initially increasing above the equilibrium spreading pressure, reached a sharply defined maximum and then slowed considerably. When heated, rapidly compressed films recovered their ability to collapse with no discontinuous change in area, arguing that the metastability does not reflect transition of the POPC film to a new phase. These observations indicate that in several respects, the supercompression of POPC monolayers resembles the supercooling of three-dimensional liquids toward a glass transition.     

Surfaces of rod photoreceptor disk membranes: light-activated enzymes

The light-activated GTP-binding protein (GBP) in toad rod outer segments has been located on the cytoplasmic surface (CS) of rod disk membranes by correlating biochemical results with images of quick- frozen, freeze-fractured, and deep-etched rod outer segments. This has been accomplished by selectively removing and replacing the 8-12-nm particles that are found on the CS of disk membranes, exactly in parallel with the GBP. In contrast, the large particles are not correlated with another major disk enzyme, the light-activated cGMP phosphodiesterase. We have been unable to visualize this protein. The surface density of large particles, one particle per eleven rhodopsins in isolated rod outer segments and one particle per nine rhodopsins in intact retina, correlates well with previous biochemical estimates of GBP numbers based on enzyme activity. After the identification of the large particles, we tested the effects of light on the density of particles on the surface of disk membranes in intact retinas. Retinas quick-frozen at various intervals after a bright flash of light show a modest increase (approximately 30%) in particle density by 10 s after the flash but no increase before 1 s. The number of particles on the disk membrane returns to dark levels between 1 and 10 min after the flash. The 1-s latency in the change of particle binding would appear to rule out this process as a mechanism for initiating phototransduction in the rod.     

Surfaces of rod photoreceptor disk membranes: integral membrane components

The membrane surfaces within the rod outer segment of the toad, Bufo marinus, were exposed by rapid-freezing followed by freeze-fracture and deep-etching. Platinum-carbon replicas of disk membranes prepared in this way demonstrate a distinct sidedness. The membrane surface that faces the lumen of the disk shows a fine granularity; particles of approximately 6 nm are packed at a density of approximately 30,000/micron 2. These dimensions suggest that the particles represent protrusions of the integral membrane protein, rhodopsin, into the intradisk space. In addition, when rhodopsin packing is intentionally perturbed by exhaustive digestion with phospholipase C, a concomitant change is observed in the appearance of the luminal surface granularity. The cytoplasmic surface of the disk rarely displays this rough texture; instead it exhibits a collection of much larger particles (8-12 nm) present at approximately 10% of the concentration of rhodopsin. This is about the size and concentration expected for certain light-regulated enzymes, cGMP phosphodiesterase and GTP-binding protein, which are currently thought to localize on or near the cytoplasmic surface of the disk. The molecular identity of the 8-12-nm particles will be identified in the following companion paper. A further differentiation of the cytoplasmic surface can be seen around the very edge, or rim, of each disk. This rim has relatively few 8-12- nm particles and instead displays short filamentlike structures connecting it to other membranes. These filaments extend between adjacent disks, across disk incisures, and from disk rims to the nearby plasma membrane.     

A method of removing gels from narrow-diameter glass tubes as part of a mini-two-dimensional electrophoresis procedure

A glass chamber that facilitates the removal of polyacrylamide gels from narrow glass tubes after the completion of isoelectric focusing is described. The tube is firmly held at one end of the glass chamber and a syringe is connected to the other end. By slowly forcing water from the syringe into the glass chamber, sufficient pressure can be generated to cause the rod gel to move slowly out of the glass tube. The rod gel is then used for the second stage of a mini-two-dimensional electrophoresis technique. Rod gels of 1.7-mm diameter have been used most extensively and can be removed from the glass tubes with almost 100% success.     

Orientation of the rhodopsin sugar moiety in bovine disk membrane.

Rhodopsin from the bovine rod outer segment contains a covalently linked carbohydrate moiety (Heller, J. & Lawrence, M.A. (1973) Biochemistry 9, 864--868). We studied the location of this carbohydrate moiety on the disk membrane by using ferritin-conjugated concanavalin A and concanavalin A labelled with fluorescein isothiocyanate. Electron microscopic observation of sonicated disk membrane that was labelled with ferritin-concanavalin A revealed the electron-dense image of ferritin on the inner surface of the disk membrane and not on its outer surface. Intact disk membrane that was similarly treated with ferritin-concanavalin A showed a complete absence of ferritin molecules on its surface. In an independent series of experiments we confirmed that the sonicated disk membrane bound three to five times more fluorescein-labelled concanavalin A than the intact disk membrane did. From these experiments we conclude that the carbohydrate moiety of bovine rhodopsin is located on the inner surface of the disk membrane, in agreement with the report by Rohlich on the frog rod outer segment disk membrane (Rohlich, P. (1976) Nature 263, 789--791).     

Kinematic analysis of the snatch lift with elite female weightlifters during the 2010 World Weightlifting Championship

The objectives of this study were to determine the mechanical work, the power output, and the angular kinematics of the lower limb and the linear kinematics of the barbell during the first and second pulls in the snatch lift event of the 2010 Women's World Weightlifting Championship, an Olympic qualifying competition, and to compare the snatch performances of the women weightlifters to those reported in the literature. The heaviest successful snatch lifts of 7 female weightlifters who won gold medals were analyzed. The snatch lifts were recorded using 2 Super-Video Home System cameras (50 fields·s), and points on the body and the barbell were manually digitized using the Ariel Performance Analysis System. The results revealed that the duration of the first pull was significantly greater than the duration of the transition phase, the second pull, and the turnover under the barbell (p < 0.05). The maximum extension velocities of the lower limb in the second pull were significantly greater than the maximum extension velocities in the first pull. The fastest extensions were observed at the knee joint during the first pull and at the hip joint during the second pull (p < 0.05). The barbell trajectories for the heaviest snatch lifts of these elite female weightlifters were similar to those of men. The maximum vertical velocity of the barbell was greater during the second pull than in the first pull (p < 0.05). The mechanical work performed in the first pull was greater than the second pull, and the power output during the second pull was greater than that of the first pull (p < 0.05). Although the magnitudes of the barbell's linear kinematics, the angular kinematics of the lower limb, and other energy characteristics did not exactly reflect those reported in the literature, the snatch lift patterns of the elite women weightlifters were similar to those of male weightlifters.     

A cytomechanical investigation of neurite growth on different culture surfaces

We have examined the relationship between tension, an intrinsic stimulator of axonal elongation, and the culture substrate, an extrinsic regulator of axonal elongation. Chick sensory neurons were cultured on three substrata: (a) plain tissue culture plastic; (b) plastic treated with collagen type IV; and (c) plastic treated with laminin. Calibrated glass needles were used to increase the tension loads on growing neurites. We found that growth cones on all substrata failed to detach when subjected to two to threefold and in some cases 5-10-fold greater tensions than their self-imposed rest tension. We conclude that adhesion to the substrate does not limit the tension exerted by growth cones. These data argue against a "tug-of-war" model for substrate-mediated guidance of growth cones. Neurite elongation was experimentally induced by towing neurites with a force-calibrated glass needle. On all substrata, towed elongation rate was proportional to applied tension above a threshold tension. The proportionality between elongation rate and tension can be regarded as the growth sensitivity of the neurite to tension, i.e., its growth rate per unit tension. On this basis, towed growth on all substrata can be described by the simple linear equation: elongation rate = sensitivity x (applied tension - tension threshold) The numerical values of tension thresholds and neurite sensitivities varied widely among different neurites. On all substrata, thresholds varied from near zero to greater than 200 mudynes, with some tendency for thresholds to cluster between 100 and 150 mudynes. Similarly, the tension sensitivity of neurites varied between 0.5 and 5.0 microns/h/mudyne. The lack of significant differences among sensitivity or threshold values on the various substrata suggest to use that the substratum does not affect the internal "set points" of the neurite for its response to tension. The growth cone of chick sensory neurons is known to pull on its neurite. The simplest cytomechanical model would assume that both growth cone-mediated elongation and towed growth are identical as far as tension input and elongation rate are concerned. We used the equation above and mean values for thresholds and sensitivity from towing experiments to predict the mean growth cone-mediated elongation rate based on mean rest tensions. These predictions are consistent with the observed mean values.     

The asymmetric transmembrane distribution of phosphatidylethanolamine,phosphatidylserine, and fatty acids of the bovine retinal rod outer segment disk membrane

Summary The transmembrane distribution of the major aminophospholipids in the bovine retinal rod outer segment disk membrane, phosphatidylethanolamine and phosphatidylserine, was determined using a novel pair of permeable and impermeable covalent modification reagents. The values for the percentages of phosphatidylethanolamine and phosphatidylserine in the outer monolayer were calculated from a simple expression which takes into account the leakage of impermeable reagent into the disk lumen as monitored by the extent of labeling of lysine entrapped in the lumen. We infer from our results that at least 73 to 87% of the disk phosphatidylethanolamine and 77 to 88% of the disk phosphatidylserine are in the outer disk membrane monolayer. The fatty acid composition of the inner aminophospholipids is slightly more saturated than the outer aminophospholipids. Calculations using the lateral surface areas occupied by the disk membrane lipids suggest that 65 to 100% of the disk phosphatidylcholine is on the inner membrane surface. Since the disk phosphatidylcholine is also somewhat more saturated than the phosphatidylethanolamine and phosphatidylserine of the outer monolayer, the total inner membrane monolayer fatty acid composition is more saturated than that of the outer monolayer fatty acid composition.