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Shape changes

Actin filaments are dynamic polymers whose assembly and disassembly in the cell cytoplasm drives shape changes (Small, 1989), cell locomotion (Theriot et al, 1992), and chemotactic migration (Theriot et al., 1992)Devreotes and... [Pg.46]

An outstanding feature of the adsorption of water vapour on silica is its sensitivity to the course and subsequent treatment of the silica sample, in particular the temperature to which it has been heated. Figure 5.15 shows the strong dependence of the isotherm for a particular silica gel on the temperature of its heat treatment the isotherm is progressively lowered as the temperature increases, especially above 400°C, and the shape changes from Type II for the lower temperatures to Type III for 600°C, 800°C and 1000°C. [Pg.269]

Cell Activation. Several studies have shown that platelets and white cells undergo shape changes when adhering to filter media. The cells are activated by contact with the filter media and form pseudopods which attach to the filter media. The cells membranes may need a certain degree of viabihty to be able to actively attach to the filter media. When white cells are treated with metaboHc inhibitors, the capabiUty of leukocyte reduction by the filter is reduced. [Pg.524]

Fig. 2. The shape-memory process, where Tis temperature, (a) The cycle where the parent phase undergoes a self-accommodating martensite transformation on cooling to the 24 variants of martensite. No macroscopic shape change occurs. The variants coalesce under stress to a single martensite variant, resulting in deformation. Then, upon heating, they revert back to the original austenite crystallographic orientation, and reverse transformation, undergoing complete recovery to complete the cycle, (b) Shape deformation. Strain recovery is typically ca 7%. Fig. 2. The shape-memory process, where Tis temperature, (a) The cycle where the parent phase undergoes a self-accommodating martensite transformation on cooling to the 24 variants of martensite. No macroscopic shape change occurs. The variants coalesce under stress to a single martensite variant, resulting in deformation. Then, upon heating, they revert back to the original austenite crystallographic orientation, and reverse transformation, undergoing complete recovery to complete the cycle, (b) Shape deformation. Strain recovery is typically ca 7%.
Martensite transformations are not limited just to metals. Some ceramics, like zirconia, have them and even the obscure system of (argon + 40 atom% nitrogen) forms martensite when it is cooled below 30 K. Helical protein crystals in some bacteria undergo a martensitic transformation and the shape change helps the bacteria to burrow into the skins of animals and people ... [Pg.86]

Chen, S. et al. Eocation of a folding protein and shape changes in GroEL-GroES complexes imaged by cryo-electron microscopy. Nature 371 261-264, 1994. [Pg.119]

In principle all the X-ray emission methods can give chemical state information from small shifts and line shape changes (cf, XPS and AES in Chapter 5). Though done for molecular studies to derive electronic structure information, this type of work is rarely done for materials analysis. The reasons are the instrumental resolution of commercial systems is not adequate and the emission lines routinely used for elemental analysis are often not those most useftil for chemical shift meas-ure-ments. The latter generally involve shallower levels (narrower natural line widths), meaning longer wavelength (softer) X-ray emission. [Pg.337]

Fig. 9. The possible tip structure with cone shape, in which the pentagons are included. As a function of the number of pentagons, the cone shape changes. The shaded one with 19.2° tip angle is the most frequently observed in PCNTs. Fig. 9. The possible tip structure with cone shape, in which the pentagons are included. As a function of the number of pentagons, the cone shape changes. The shaded one with 19.2° tip angle is the most frequently observed in PCNTs.
The body temperature limits for health in terms of internal or core temperature are fairly limited. The limits are basically related to the function of nervous tissue. Body temperatures around 28 °C or less can result in cardiac fibrillation and arrest. Temperatures of 43 °C and greater can result in heat stroke, brain damage, and death. Often, too high a temperature causes irreversible shape changes to the protein molecules of nervous tissue. That is, cooling overheated tissue to normal temperatures may not restore its original function. [Pg.176]

The consequences of shape change are densification and loss of electrode porosity, increased current density caused by loss of zinc surface area, and finally earlier passivation. Two different forms of pasi-vation can stop the discharge of a zinc electrode before the active material is exhausted. "Spontaneous" passivation occurs... [Pg.203]

Lithium is consumed by reaction with the electrolyte which forms a protective film [6]. During the deposition and stripping of lithium, the surface shape changes and a fresh lithium surface is formed, with a new protection film on it lithium is consumed in the process. [Pg.343]

One of these is the "shape change" phenomenon, in which the location of the electrodeposit is not the same as that of the discharge (deplating) process. Thus, upon cycling, the electrode metal is preferentially transferred to new locations. For the most part, this is a problem of current distribution and hydrodynamics rather than being a materials issue, therefore it will not be discussed further here. [Pg.360]

Thermal-mechanical analysis (TMA) has proven a more reproducible measure of melt integrity [20]. The TMA test involves measuring the shape change of a separator under load while the temperature is linearly increased. Typically, separators show some shrinkage, then start to elongate, and finally break (see Fig. 5). [Pg.561]

Fig. 29. Observed and calculated 2H NMR spectra for the mesogenic groups of a) the nematic (m = 2), b) the smectic (m = 6) liquid crystalline polymer in the glassy state, showing the line shape changes due to the freezing of the jump motion of the labelled phenyl ring. The exchange frequency corresponds to the centre of the distribution of correlation times. Note that the order parameters are different, S = 0.65 in the frozen nematic, and S = 0.85 in the frozen smectic system, respectively... Fig. 29. Observed and calculated 2H NMR spectra for the mesogenic groups of a) the nematic (m = 2), b) the smectic (m = 6) liquid crystalline polymer in the glassy state, showing the line shape changes due to the freezing of the jump motion of the labelled phenyl ring. The exchange frequency corresponds to the centre of the distribution of correlation times. Note that the order parameters are different, S = 0.65 in the frozen nematic, and S = 0.85 in the frozen smectic system, respectively...

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See also in sourсe #XX -- [ Pg.20 , Pg.74 , Pg.118 , Pg.173 , Pg.182 , Pg.207 , Pg.209 ]

See also in sourсe #XX -- [ Pg.121 ]

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Algorithms shape change

Analytical Functions Wrapped Around Spheres Shape Change

Cell shape change

Changing shape

Changing size and shape

Changing the Shape of Toolbars

Dendrimer Shape Changes

Dendrimers shape changes

Electrode shape change

How does a receptor change shape

Indirect Actuation of Thermally-Triggered Shape-Changing Effect

Kinetics of shape change

Martensitic transformations macroscopic shape change

Micelles shape change

Molecular distortion shape change

Molecular shape change

Photoresponsive shape changes

Pore shape change

Shape change due to relaxation

Shape change kinetics

Shape memory polymers phase change materials

Shape memory polymers phase change properties

Shape-Changing CNT-Polymer Composites

Shape-changing CNT-polymers

Shape-changing capability

Shape-changing gels

Shape-changing polymers

Shape-changing polymers physical stimuli

Simulation shape change

Spout shapes changes

Subject shape-changing

Subject shape-changing composites

The Change in Micellar Shape

Thermosensitive Shape-Changing Polymers

Vertical shape change

Vesicle shape change

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