The margin for error when releasing the asymmetric bars for dismounts

It has previously been shown that male gymnasts using the "scooped" giant circling technique were able to flatten the path followed by their mass center, resulting in a larger margin for error when releasing the high bar (Hiley and Yeadon, 2003a). The circling technique prior to performing double layout somersault dismounts from the asymmetric bars in women's artistic gymnastics appears to be similar to the "traditional" technique used by some male gymnasts on the high bar. It was speculated that as a result the female gymnasts would have margins for error similar to those of male gymnasts who use the traditional technique. However, it is unclear how the technique of the female gymnasts is affected by the need to avoid the lower bar. A 4-segment planar simulation model of the gymnast and upper bar was used to determine the margins for error when releasing the bar for 9 double layout somersault dismounts at the Sydney 2000 Olympics. The elastic properties of the gymnast and bar were modeled using damped linear springs. Model parameters, primarily the inertia and spring parameters, were optimized to obtain a close match between simulated and actual performances in terms of rotation angle (1.2 degrees), bar displacement (0.011 m), and release velocities (<1%). Each matching simulation was used to determine the time window around the actual point of release for which the model had appropriate release parameters to complete the dismount successfully. The margins for error of the 9 female gymnasts (release window 43-102 ms) were comparable to those of the 3 male gymnasts using the traditional technique (release window 79-84 ms).     

The effect of cost function on optimum technique of the undersomersault on parallel bars

The undersomersault, or felge, to handstand on parallel bars has become an important skill in Men's Artistic Gymnastics as it forms the basis of many complex variations. To receive no deductions from the judges, the undersomersault must be performed without demonstrating the use of strength to achieve the final handstand position. Two male gymnasts each performed nine undersomersaults from handstand to handstand while data were recorded using an automatic motion capture system. The highest and lowest scoring trials of each gymnast, as determined by four international judges, were chosen for further analysis. Three optimization criteria were used to generate undersomersault technique during the swing phase of the skill using a computer simulation model: minimization of peak joint torques, minimization of horizontal velocity before release, and maximization of angular momentum. The techniques used by both gymnasts could be explained using the second optimization criterion which facilitated further skill development. The first optimization criterion generated a technique advocated for beginners where strength might be expected to be a limiting factor. The third optimization criterion resulted in a different type of undersomersault movement of greater difficulty according to the FIG Code of Points.     

On the organizing role of nonmuscular forces during performance of a giant circle in gymnastics

Five elite gymnasts performed giant circles on the high bar under different conditions of loading (without and with 6-kg loads attached to the shoulders, waist or ankles). Comparing the gymnasts' kinematic pattern of movement with that of a triple-pendulum moving under the sole influence of nonmuscular forces revealed qualitative similarities, including the adoption of an arched position during the downswing and a piked position during the upswing. The structuring role of nonmuscular forces in the organization of movement was further reinforced by the results of an inverse dynamics analysis, assessing the contributions of gravitational, inertial and muscular components to the net joint torques. Adding loads at the level of the shoulders, waist or ankles systematically influenced movement kinematics and net joint torques. However, with the loads attached at the level of the shoulders or waist, the load-induced changes in gravitational and inertial torques provided the required increase in net joint torque, thereby allowing the muscular torques to remain unchanged. With the loads attached at the level of the ankles, this was no longer the case and the gymnasts increased the muscular torques at the shoulder and hip joints. Together, these results demonstrate that expert gymnasts skillfully exploit the operative nonmuscular forces, employing muscle force only in the capacity of complementary forces needed to perform the task.     

Mechanical energetic processes during the giant swing exercise before dismounts and flight elements on the high bar and the uneven parallel bars.

The purposes of this study were as follows: (1) To study the energy exchange between the body of the gymnast and the high bar and uneven parallel bars during forward and backward giant swings. (2) To examine the differences between the mechanical energy produced and the mechanical energy absorbed by the muscles during forward and backward giant swings on the high bar and the uneven parallel bars. The data were gathered during the gymnastic world championships in 1994. The experimental set up consisted of two video cameras (50 Hz) and two force measurement bars (500 Hz). A total of 101 giant swings before dismounts and flight elements performed by 33 male and 34 female gymnasts were analyzed. There are characteristically two main phases during forward and backward giant swings before dismounts and flight elements. During the first phase energy is transferred from the gymnast's body into the bar. During this phase of the backward giant swing the energy of the system decreases because the amount of energy decrease of the gymnast's body is more than the energy transferred into the high bar. An exception can be seen during the giant swings in which the gymnast used the power technique. During forward giant swings the energy of the system increases during the first phase. This occurs through active flexion of the hipjoint which produced the extra muscular energy. During the second phase energy is transferred from the bar back into the gymnast's body whose total energy increases. An increase in the energy of the system can only be achieved through muscular work. During the second phase of the backward giant swing the energy of the system increases. The forward giant swings performed on the uneven parallel bars showed a large energy loss during this phase. The energy deficit seen during the first phase of the backward giant swing can be improved by using the power technique. To achieve this the athlete must be in a bent position at the start of the giant swing exercise. Through extension at the shoulder and hip joints muscular energy can be put into the system.     

Kinetic mechanism of initiation by RepD as a part of asymmetric, rolling circle plasmid unwinding

Some bacterial plasmids carry antibiotic resistance genes and replicate by an asymmetric, rolling circle mechanism, in which replication of the two strands is not concurrent. Initiation of this replication occurs via an initiator protein that nicks one DNA strand at the double-stranded origin of replication. In this work, RepD protein from the staphylococcal plasmid pC221 carries this function and allows PcrA helicase to bind and begin unwinding the plasmid DNA. This work uses whole plasmid constructs as well as oligonucleotide-based mimics of parts of the origin to examine the initiation reaction. It investigates the phenomenon that nicking, although required to open a single-stranded region at the origin and so allow PcrA to bind, is not required for another function of RepD, namely to increase the processivity of PcrA, allowing it to unwind plasmid lengths of DNA. A kinetic mechanism of RepD initiation is presented, showing rapid binding of the origin DNA. The rate of nicking varies with the structure of the DNA but can occur with a rate constant of >25 s(-1) at 30 °C. The equilibrium constant of the nicking reaction, which involves a transesterification to form a phosphotyrosine bond within the RepD active site, is close to unity.     

Optimised performance of the backward longswing on rings

Many elite gymnasts perform the straight arm backward longswing on rings in competition. Since points are deducted if gymnasts possess motion on completion of the movement, the ability to successfully perform the longswing to a stationary final handstand is of great importance. Sprigings et al. (1998) found that for a longswing initiated from a still handstand the optimum performance of an inelastic planar simulation model resulted in a residual swing of more than 3 degrees in the final handstand.For the present study, a three-dimensional simulation model of a gymnast swinging on rings, incorporating lateral arm movements used by gymnasts and mandatory apparatus elasticity, was used to investigate the possibility of performing a backward longswing initiated and completed in handstands with minimal swing. Root mean square differences between the actual and simulated performances for the orientations of the gymnast and rings cables, the combined cable tension and the extension of the gymnast were 3.2 degrees, 1.0 degrees, 270N and 0.05m respectively.The optimised simulated performance initiated from a handstand with 2.1 degrees of swing and using realistic changes to the gymnast's technique resulted in 0.6 degrees of residual swing in the final handstand. The sensitivity of the backward longswing to perturbations in the technique used for the optimised performance was determined. For a final handstand with minimal residual swing (2 degrees) the changes in body configuration must be timed to within 15 ms while a delay of 30 ms will result in considerable residual swing (7 degrees).     

Shape changes of giant liposomes induced by an asymmetric transmembrane distribution of phospholipids.

The influence of a phospholipid transmembrane redistribution on the shape of nonspherical flaccid vesicles was investigated at a fixed temperature by optical microscopy. In a first series of experiments, a transmembrane pH gradient was imposed on egg phosphatidylcholine (EPC)-egg phosphatidylglycerol (EPG) (100:1) giant vesicles. The delta pH induced an asymmetric distribution of EPG. Simultaneously, discoid vesicles were transformed into tubular or a series of connected small vesicles. The fraction of phospholipid transfer necessary for a shape change from discoid to two connected vesicles was of the order of 0.1% of the total phospholipids. Additional lipid redistribution was accompanied by a sequence of shape changes. In a second series of experiments, lyso phosphatidylcholine (L-PC) was added to, or subtracted from, the external leaflet of giant EPC vesicles. The addition of L-PC induced a change from discoid to a two-vesicle state without further evolution, suggesting that lipid transfer and lipid addition are not equivalent. L-PC depletion from the outer leaflet generated stomatocyte-like vesicles. Whenever possible, we have determined whether the giant vesicles undergoing shape changes were unilamellar or multilamellar by measuring the elastic area compressibility modulus, K, by the micropipette assay (Kwok and Evans, 1981). Shape transformations triggered by phospholipid modification of the most external bilayer were indeed influenced by the presence of other underlying membranes that played a role comparable to that of a passive cytoskeleton layer. It appears that in real cells, invaginations of the plasma membrane or budding of organelles could be triggered by a phospholipid transfer from one leaflet to the other caused, for instance, by the aminophospholipid translocase which is present in eukaryotic membranes.     

Optimization of asymmetric polymerase chain reaction for rapid fluorescent DNA sequencing

A high-throughput method for the preparation of single-stranded template DNA, which is suitable for sequence analysis using fluorescent labeling chemistry, is described here. In this procedure, the asymmetric polymerase chain reaction is employed to amplify recombinant plasmid or bacteriophage DNA directly from colonies or plaques. The use of amplification primers located at least 200 base pairs 5' to the site of sequencing primer annealing removes the need for extensive purification of the asymmetric polymerase chain reaction product. Instead, the single-stranded product DNA is purified by a simple isopropanol precipitation step and then directly sequenced using fluorescent dye-labeled oligonucleotides. This method significantly reduces the time and labor required for template preparation and improves fluorescent DNA sequencing strategies by providing a much more uniform yield of single-stranded DNA.     

Reexamination of the double sucrose gap technique for the study of lobster giant axons. Theory and experiments

The double sucrose gap technique for the study of lobster giant axons has been reexamined. The leakage behavior of the system cannot be successfully modeled by conventional sucrose gap theory, but is accounted for by the McGuigan-Tsien model that takes into account the cable properties of membrane under sucrose. The facts of high-leakage conductance and the ability to maintain large resting potentials in the face of low sucrose gap resistance lead to a hypothesis that membrane resistance under sucrose is very low because of a large negative surface potential. Computer simulations of the leakage behavior of the conventional gap model and the McGuigan-Tsien model were compared with experimental measurements on lobster axons using normal sucrose or sucrose doped with Na+, Ca2+ or La3+ ions. As the concentration of doping ion increased, the leakage rose, but the species of doping ion had more influence on leakage than gap resistance. At equal gap resistance, leakage decreased with an increase in valence of the doping species. Leakage was even lower in La-doped sucrose at 20 M omega gap resistance than in normal sucrose at 200 M omega gap resistance. Resting potentials decreased with decreasing gap resistance and increasing valence of the doping species. Resting potential behavior was successfully simulated with a hybrid model consisting of a point node flanked by infinite cables and a shunt between ground and the voltage-measuring pool. The data support the hypothesis that the membrane resistance under sucrose is low and that it can be raised by doping the sucrose with multivalent cations, with La3+ being particularly effective.(ABSTRACT TRUNCATED AT 250 WORDS)     

Fault bars timing and duration: the power of studying feather fault bars and growth bands together

Growth bands and fault bars, widespread features of feathers that form during regeneration, have largely been studied independently. Growth bands result from normal regeneration: each pair of dark/light bands forms every 24 h. Fault bars are a response to stress during regeneration, creating a translucent line that can break the feather. We studied the relative position and width of these two structures in feathers of nestling and adult white storks Ciconia ciconia. We first confirmed that one growth band represents 24 h of feather regeneration. Fault bars did not occur at random within growth bands: 65.7% (in nestlings) and 45.6% (in adults) of them occurred in one out of six defined segments within a growth band, namely that segment corresponding to the first one‐third of night time hours. The width of fault bars relative to growth bands suggested that fault bars were produced during a median (range) of 7.0 h (2.7–27.0) in nestlings and 3.7 h (1.8–7.9) in adults. Fault bars were concentrated at feather tips in nestlings, but at central locations in adult feathers. Our results suggest that, in general, fault bars are a discrete event of a finite duration occurring mainly during the night (particularly in nestlings). This, along with current knowledge, suggests that acute stressors, rather than chronic ones, are responsible for fault bar formation. Thus, such acute punctual stressors (a matter of minutes) can have long‐lasting (months?years) physiological effects due to the wing load increase from feather breakage caused by fault bars.     

Types of the cerebral arterial circle (circle of Willis) in a Sri Lankan Population

Background  

The variations of the circle of Willis (CW) are clinically important as patients with effective collateral circulations have a lower risk of transient ischemic attack and stroke than those with ineffective collaterals. The aim of the present cadaveric study was to investigate the anatomical variations of the CW and to compare the frequency of prevalence of the different variations with previous autopsy studies as variations in the anatomy of the CW as a whole have not been studied in the Indian subcontinent.     

Effect of guanidine on the squid giant synapse

Effects of guanidine on pre- and postsynaptic activities in the untreated or tetrodotoxin-treated squid giant synapses were examined by externally perfusing with various concentrations (423 mM, 42 mM, 21 mM, and 4.2 mM), or by iontophoretic injection of guanidine into the presynaptic terminal. In 423 mM guanidine (Na-free), the pre- and postsynaptic spikes together with PSP were completely abolished. In concentrations of 42 mM or lower of guanidine media the following changes related to the concentration used were observed: reduction of delayed rectification of both axon membranes without significant alteration of resting membrane resistances; a few millivolts decrease in the resting membrane potentials; small decrease in amplitude of pre- and post-synaptic spikes without marked increase of spike duration; enhancement of synaptic activity as manifested by increases in the amplitude and duration of the PSP. Iontophoretically injected guanidine also reduced delayed rectification of the presynaptic membrane. Input-output relation was modified in a way similar to externally applied guanidine and an “Off-PSP” was demonstrated shortly after application of an inside positive presynaptic polarization. Thus, a comparison of the augmentation of synaptic transmission by the extracellular and intracellularly applied guanidine demonstrates that the primary effect is at the presynaptic terminal.