A combined SAXS/WAXS investigation of the phase behaviour of di-polyenoic membrane lipids

AbstractReal-time measurements of the SAXS/WAXS diffraction patterns of aqueous dispersions (1:1 wt/wt) of the di-polyenoic lipids di-18:2 PC, di-18:3 PC, di-18:2 PE and di-18:3 PE were made over the temperature range 10° to about −80°C. The results of these measurements were compared to similar measurements performed on the corresponding di-18:0 and di-18:1 derivatives. SAXS measurements of the temperature dependence of lamellar repeat distances show that the di-polyenoic lipids undergo broad second-order transitions between their gel and liquid-crystal lamellar phases spanning 30–40°C. The di-18:1 and di-18:0 derivatives, in contrast, undergo abrupt first-order transitions. The gel phases of the di-18:0 derivatives are characterised by two-component WAXS patterns with a sharp component close to 0.42 nm and a broader component at narrower spacings. On cooling, these lipids appear to undergo an initial transition to an Lβ, phase followed by a conversion to an Lc phase. The gel phases of the di-18:1 derivatives also show two-component patterns but with the sharp component centred closer to 0.44 nm. The di-polyenoic lipids, in contrast, are characterised by a single broad peak centred at a spacing of about 0.42 nm, close to that of conventional Lβ, phases. The changes in lamellar repeat distance accompanying the transitions in the di-monoenoic and di-polyenoic lipids, all of which occur in the frozen state, are very similar, indicating that the acyl chains of the polyenoic lipids are close to their maximum extension in the gel state. The WAXS patterns of the polyenoic lipids suggest that the saturated upper parts of the acyl chains are packed on a regular hexagonal lattice while their polyunsaturated termini remain relatively disordered

The Effect of Temperature on the Structure of Vinblastine-induced Polymers of Purified Tubulin: Detection of a Reversible Conformational Change

Addition of the antimitotic drug vinblastine to solutions of purified tubulin induces the formation of helical polymers whose structure and type of aggregation is determined by the concentration of magnesium. While paracrystalline arrangements of single coils are observed at low concentrations of the ion, for concentrations higher than 6 mM free double-coiled spirals are obtained, which are indistinguishable from those obtained in the presence of microtubule-associated proteins (MAPs). This result is consistent with a similar effect of magnesium and MAPs in neutralizing negative charges on the tubulin molecule and so allowing for lateral contacts between protofilaments. The effects that temperature has on the structure of both types of polymers, free spirals or paracrystals, have been monitored using time-resolved X-ray solution scattering. This study shows that a temperature increase: (1) affects the length and lateral aggregation of the spirals in the paracrystalline sample; (2) induces a reversible increase of the helical pitch in both types of polymers that closely follows the temperature change; (3) produces an irreversible aggregation of some of the protein in both types of polymers; and (4) can induce a reversible transformation from one type of structure to the other when the concentration of Mg2+is in the boundary between the two ranges. We suggest that the changes in pitch are due to a temperature-induced conformational change of the tubulin molecule. This effect may be related to the structural modifications that result in the temperature-induced assembly of microtubulesin vitrounder normal conditions of assembly

W16.1: A new fixed wavelength diffraction station at the SRS Daresbury

Station W16.1 is a fixed wavelength (1.4 Å) x‐ray diffraction station recently constructed and commissioned at the SRS. It has been designed specifically for time‐resolved studies of noncrystalline and fibrous materials and optimized for low angle measurements. Wide angle diffraction will also be available with simultaneous small and wide angle scattering/diffraction a future facility. In order to perform dynamic (∼1 ms) low angle measurements on weakly scattering systems, the station design has had to incorporate several novel features so as to achieve the predicted 1×1013 photon/s at the specimen

Two-dimensional time resolved X-ray diffraction of muscle: Recent results

This report provides a preliminary sketch of the results obtained in a two-dimensional time resolved X-ray diffraction study of “live” frog sartorius muscles undergoing isometric tetani. These results demonstrate the recently developed capability to record time resolved (10 msec time resolution), two-dimensional X-ray diffraction diagrams throughout the cycle of contraction. The correlation between the time courses of the diffraction features in the whole of the diffraction diagram establishes a sequence of structural events, which suggest that during the transition from rest to the plateau of tension and the subsequent recovery, the following sequence of events takes place: 1. a) Following the activation phase, which is best monitored by the increase of intensity on the second actin layer line at 18.0 nm spacing (5), there is the onset of three dimensional disorder due to the filaments losing their axial alignment and the myosin heads rotating azimuthally and moving radially outwards. A set of low-angle layer lines, following the actin based spacings seen in rigor (i.e., at spacings of ca. 36.5–37.5, 24.0 and 18.0 nm) become visible and those at ca. 24.0 and 18.0 nm appear to increase in intensity during this phase with a time course that cannot be determined accurately because of the proximity of the neighbouring first, second and third myosin layer lines and the weakness of these diffraction features. Whether the first of these layer lines increases or not is difficult to ascertain. Moreover, proper account of the loss in crystallinity during the development of tension must be made before the comparisons in intensity between the rest and peak of tension states have any significance. Nevertheless, these features together with the behaviour of the equatorial reflections and the meridional region of the third myosin layer line indicate that a sizeable fraction of the crossbridges may become axially disposed with an actin based periodicity. The formation of this complex does not immediately result in the generation of tension. The labelling of the thin filaments is also reflected in the main actin layer lines at 5.9 and 5.1 nm. 2. b) The tension generating phase is monitored by the intensity changes in the meridional region of the third myosin layer line, which are best explained by a change in the orientation/conformation of the tension bearing crossbridges, (which probably adopt a more perpendicular orientation to the filament axis). 3. c) At the end of stimulation, the crossbridges return to an axial spacing and axial orientation (although not yet azimuthal) similar to the one at rest. This is followed by a very slow return to the azimuthal equilibrium position typical of the rest pattern

Time-resolved X-ray diffraction studies of myosin head movements in live frog sartorius muscle during isometric and isotonic contractions

Using the facilities at the Daresbury Synchrotron Radiation Source, meridional diffraction patterns of muscles at ca 8°C were recorded with a time resolution of 2 or 4 ms. In isometric contractions tetanic peak tension (P 0) is reached in ca 400 ms. Under such conditions, following stimulation from rest, the timing of changes in the major reflections (the 38.2 nm troponin reflection, and the 21.5 and 14.34/14.58 nm myosin reflections) can be explained in terms of four types of time courses: K 1, K 2, K 3 and K 4. The onset of K 1 occurs immediately after stimulation, but that of K 2, K 3 and K 4 is delayed by a latent period of ca 16 ms. Relative to the end of their own latent periods the half-times for K 1, K 2, K 3 and K 4 are 14–16, 16, 32 and 52 ms, respectively. In half-times, K 1, K 2, K 3 lead tension rise by 52, 36 and 20 ms, respectively. K 4 parallels the time course of tension rise. From an analysis of the data we conclude that K 1 reflects thin filament activation which involves the troponin system; K 2 arises from an order-disorder transition during which the register between the filaments is lost; K 3 is due to the formation of an acto-myosin complex which (at P 0) causes 70% or more of the heads to diffract with actin-based periodicities; and K 4 is caused by a change in the axial orientation of the myosin heads (relative to thin filament axis) which is estimated to be from 65–70° at rest to ca 90° at P 0. Isotonic contraction experiments showed that during shortening under a load of ca 0.27 P 0, at least 85% of the heads (relative to those forming an acto-myosin complex at P 0) diffract with actin-based periodicities, whilst their axial orientation does not change from that at rest. During shortening under a negligible load, at most 5–10% of the heads (relative to those forming an acto-myosin complex at P 0) diffract with actin-based periodicities, and their axial orientation also remains the same as that at rest. This suggests that in isometric contractions the change in axial orientation is not the cause of active tension production, but rather the result of it. Analysis of the data reveals that independent of load, the extent of asynchronous axial motions executed by most of the cycling heads is no more than 0.5–0.65 nm greater than at rest. To account for the diffraction data in terms of the conventional tilting head model one would have to suppose that a few of the heads, and/or a small part of their mass perform the much larger motions demanded by that model. Therefore we conclude either that the required information is not available in our patterns or that an alternative hypothesis for contraction has to be developed

Two-dimensional time-resolved X-ray diffraction studies of live isometrically contracting frog sartorius muscle

Results were obtained from contracting frog muscles by collecting high quality time-resolved, two-dimensional, X-ray diffraction patterns at the British Synchrotron Radiation Source (SERC, Daresbury, Laboratory). The structural transitions associated with isometric tension generation were recorded under conditions in which the three-dimensional order characteristic of the rest state is either present or absent. In both cases, new layer lines appear during tension generation, subsequent to changes from activation events in the filaments. Compared with the decorated actin layer lines of the rigor state, the spacings of the new layer lines are similar whereas their intensities differ substantially. We conclude that in contracting muscle an actomyosin complex is formed whose structure is not like that in rigor, although it is possible that the interacting sites are the same. Transition from rest to plateau of tension is accompanied by approximately 1.6% increase in the axial spacing of the myosin layer lines. This is explained as arising from the axial disposition of the interacting myosin heads in the actomyosin complex. Model calculations are presented which support this view. We argue that in a situation where an actomyosin complex is formed during contraction, one cannot describe the diffraction features as being either thick or thin filament based. Accordingly, the layer lines seen during tension generation are referred to as actomyosin layer lines. It is shown that these layer lines can be indexed as submultiples of a minimum axial repeat of approximately 218.7 nm. After lattice disorder effects are taken into account, the intensity increases on the 15th and 21st AM layer lines at spacings of approximately 14.58 and 10.4 nm respectively, show the same time course as tension rise. However, the time course of the intensity increase of the other actomyosin layer lines and of the spacing change (which is the same for both phenomena) shows a substantial lead over tension rise. These findings suggest that the actomyosin complex formed prior to tension rise is a non-tension-generating state and that this is followed by a transition of the complex to a tension-generating state. The intensity increase in the 15th actomyosin layer line, which parallels tension rise, can be accounted for assuming that in the tension-generating state the attached heads adopt (axially) a more perpendicular orientation with respect to the muscle axis than is seen at rest or in the non-tension-generating state. This suggests the existence of at least two structurally distinct interacting myosin head conformations. The results of comparing the meridional intensities between the myosin layer lines at rest and the actomyosin layer lines at the plateau of tension (measured to a resolution of approximately 2.6 nm) are interpreted to indicate that the majority of the myosin heads in the actomyosin complex do not perform random axial rotations with a mean value greater than approximately 3.0 nm. From this we conclude that the extent of axial order in the interacting heads must be at least as high as is that of resting heads. Fulltext Previe