Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Hydrostatic shift

Hydrostatic Transmissions. The most recent use of hydrauhc power has been in hydrostatic transmissions which are used in many self-propelled harvesting machines and garden tractors and in large tractors and constmction machines. Apphcations in tmcks for highway operation also are being developed. No clutch is used and no gear shifting is involved, thus this type of transmission could be called automatic, but in all other respects the hydrostatic transmission has no similarity to the hydrokinetic automatic transmission (16). [Pg.270]

From this relatively simple test, therefore, it is possible to obtain complete flow data on the material as shown in Fig. 5.3. Note that shear rates similar to those experienced in processing equipment can be achieved. Variations in melt temperature and hypostatic pressure also have an effect on the shear and tensile viscosities of the melt. An increase in temperature causes a decrease in viscosity and an increase in hydrostatic pressure causes an increase in viscosity. Topically, for low density polyethlyene an increase in temperature of 40°C causes a vertical shift of the viscosity curve by a factor of about 3. Since the plastic will be subjected to a temperature rise when it is forced through the die, it is usually worthwhile to check (by means of Equation 5.64) whether or not this is signiflcant. Fig. 5.2 shows the effect of temperature on the viscosity of polypropylene. [Pg.373]

Bulk flow plays only a minor role in the exchange of specific solutes between blood and tissue cells. A far more important function of bulk flow is to regulate distribution of extracellular fluid between the vascular compartment (plasma) and the interstitial space. Maintenance of an appropriate circulating volume of blood is an important factor in the maintenance of blood pressure. For example, dehydration and hemorrhage will cause a decrease in blood pressure leading to a decrease in capillary hydrostatic pressure. As a result, net filtration decreases and net reabsorption increases, causing movement, or bulk flow, of extracellular fluid from interstitial space into the vascular compartment. This fluid shift expands the plasma volume and compensates for the fall in blood pressure. [Pg.223]

Barstow B, Ando N, Kim CU, Gruner SM (2008) Alteration of citrine structure by hydrostatic pressure explains the accompanying spectral shift. Proc Natl Acad Sci USA 105 13362-13366... [Pg.382]

FIGURE 9.2 EPR powder pattern of the [2Fe-2S]1+ cluster in spinach ferredoxin. Trace A shows an attempt to fit the spectrum with the diagonal linewidth Equation 9.1. In trace B the spectrum is fitted with the nondiagonal g-strain Equation 9.18. Trace C shows an experiment in which the spectral features are slightly shifted (solid trace) under the influence of an external hydrostatic stress. (Data replotted from Hagen and Albracht 1982.)... [Pg.155]

The figure also shows the effect of an externally applied hydrostatic pressure (using the method of Figure 9.2C) the two outermost lines are seen to be shifted in opposite direction (Hagen 1982a). [Pg.165]

The effect of an applied pressure on the UCFT has been investigated for polymer particles that are sterically stabilized by polyisobutylene and dispersed in 2-methy1-butane. It was observed that the UCFT was shifted to a higher temperature as the hydrostatic pressure applied to the system increased. There was also a qualitative correlation between the UCFT as a function of applied pressure and the 6 conditions of PIB + 2-methylbutane in (P,T) space. These results can be rationalized by considering the effect of pressure on the free volume dissimilarity contribution to the free energy of close approach of interacting particles. Application of corresponding states concepts to the theory of steric stabilization enables a qualitative prediction of the observed stability behaviour as a function of temperature and pressure. [Pg.317]

Most of the complexes to be described here have trigonal symmetry. For a trigonal center, the splitting of the spectral bands due to the lifting of orientational degeneracy is described by two parameters, A1 and A2. The parameter A is proportional to the hydrostatic component of the stress and gives rise to a shift in frequency that is independent of the stress direction, whereas A2 gives rise to a shift that depends on the orientation of the center. [Pg.157]

The influence of pressure has also been used to tune the ST properties of these ID chain compounds. Application of hydrostatic pressure ( 6 kbar) on [Fe(hyptrz)3] (4-chlorophenylsulfonate)2 H20 (hyptrz=4-(3 -hydroxypro-pyl)-l,2,4-triazole) provokes a parallel shift of the ST curves upwards to room temperature (Fig. 5) [41]. The steepness of the ST curves along with the hysteresis width remain practically constant. This lends support to the assertion that cooperative interactions are confined within the Fe(II) triazole chain. Thus a change in external pressure has an effect on the SCO behaviour comparable to a change in internal electrostatic pressure due to anion-cation interactions (e.g. changing the counter-anion). Both lead to considerable shifts in transition temperatures without significant influence on the hysteresis width. Several theoretical models have been developed to predict such SCO behaviour of ID chain compounds under pressure [50-52]. Figure 5 (bottom) also shows the pressure dependence of the LS fraction, yLS, of... [Pg.252]

Figure 14. (Upper panel) The ruby fluorescence spectrum measured in quasi-hydrostatic conditions at 7.7 GPa. (Lower panel) The empirical law describing ruby Ri line shift with pressure [96] is also reported. Figure 14. (Upper panel) The ruby fluorescence spectrum measured in quasi-hydrostatic conditions at 7.7 GPa. (Lower panel) The empirical law describing ruby Ri line shift with pressure [96] is also reported.
Polymerization leads to a contraction in the volume of the system so that the equilibrium of a monomer-polymer system shifts in the direction of the reaction as the hydrostatic pressure increases. This was demonstrated by Weale (40) in his studies of a-methylstyrene polymerization under high pressure. The ceiling temperature increased from 61° C at 1 atm to 170° C at 6480 atm. [Pg.491]

This is the first case in which epoprostenol has been successfully restarted. The authors commented that pulmonary edema during acute infusion of epoprostenol is considered a contraindication to its further use. They theorized that the pulmonary edema could have occurred secondary to the dramatic increase in pulmonary perfusion at 6 nanograms/kg/minute of epoprostenol and subsequent rapid shifts in vascular hydrostatic pressure. The slow increase in dosage during reinstitution may have averted the dramatic increase in pulmonary perfusion. [Pg.118]

Another luminescence sensor, SrlLOyiSm2"1" has been suggested by Lacam and Chateau (1989). The advantage of using Sm2+ instead of Sm3+ is the occurrence of the well-isolated singlet transition 5Do -> 7Fo at 685.41 nm at ambient conditions. Also in this case the pressure-induced shift was similar to ruby, whereas the temperature-induced shift was much smaller. The stability of the host was proven up to 108 GPa (Leger et al., 1990) and the shift of the 5Do -> 7Fo transition has been calibrated in a hydrostatic medium (helium) up to 124 GPa (Datchi et al., 1997). [Pg.554]

In the native state, the shift observed between 0 and 40° C is 3 nm, indicating that the structure around TNS is not loose. Hydrostatic pressure destabilizes the tertiary structure of the protein. In this case, between 0 and 40° C, there is no shift in the emission peak. [Pg.245]

The shift of the A line in the epilayers has been connected with the variation of the lattice parameters of GaN [1,11,12], The shift of this line was also measured in samples subjected to hydrostatic pressure (see Datareview A3.1). Combination of all these data permits one to obtain the whole series of excitonic deformation potentials [6,16], Two sets of data are available which are consistent with each other and are given in TABLE 1. The discrepancies between them are linked to the differences in the values of the stiflhess coefficients of GaN used by the authors. Gil and Alemu [6] in their work subsequent to the work of Shan et al [16] used data not available when Shan et al calculated their values. The notations are the same and are linked to the relationship with the quasi cubic model of Pikus and Bir [17], Deformation potentials as and a6 have been obtained by Alemu et al [8] who studied the anisotropy of the optical response in the growth plane of GaN epilayers orthorhombically distorted by growth on A-plane sapphire. For a detailed presentation of the theoretical values of deformation potentials of GaN we refer the reader to Suzuki and Uenoyama [20] who took the old values of the stiflhess coefficients of GaN [21]. [Pg.66]

Figures 20A and B show the PL spectra, recorded at 290 K, at 600 nm, and as a function of pressure, for Cs9(SmW10O36) and SmWi0O36-LDH, respectively (Park et al., 2002). For the sake of comparison, the line shapes are normalized and displaced along the vertical axis. In both cases, the peak position is red-shifted by 4—5 nm when the hydrostatic pressure increases from 1 bar to 61 kbar. It was shown that the red-shift from A to A lies solely in the deformation of the samarium complexes by the uniaxial stress exerted by the host layers, whereas the shift from B to B is also influenced by the change in the cation environment. Under the same conditions, B is not at the same position for the non-intercalated (HN (n -b u t y 1) 3) 9 (SmW10O3e) and Cs9(SmWi0O36) compounds (Park et al., 2002). Thus only peak A is available to measure the unixial stress. This observation can be used to determine the uniaxial stress, when the external pressure is zero. For the SmW10O36—LDH system, the uniaxial stress varies significantly from 75 at 28 K to 140 kbar at 290 K (Park et al., 2002). Figures 20A and B show the PL spectra, recorded at 290 K, at 600 nm, and as a function of pressure, for Cs9(SmW10O36) and SmWi0O36-LDH, respectively (Park et al., 2002). For the sake of comparison, the line shapes are normalized and displaced along the vertical axis. In both cases, the peak position is red-shifted by 4—5 nm when the hydrostatic pressure increases from 1 bar to 61 kbar. It was shown that the red-shift from A to A lies solely in the deformation of the samarium complexes by the uniaxial stress exerted by the host layers, whereas the shift from B to B is also influenced by the change in the cation environment. Under the same conditions, B is not at the same position for the non-intercalated (HN (n -b u t y 1) 3) 9 (SmW10O3e) and Cs9(SmWi0O36) compounds (Park et al., 2002). Thus only peak A is available to measure the unixial stress. This observation can be used to determine the uniaxial stress, when the external pressure is zero. For the SmW10O36—LDH system, the uniaxial stress varies significantly from 75 at 28 K to 140 kbar at 290 K (Park et al., 2002).
Fig. 33. Polarized emission spectra of single-crystal Ba[Pt(CN)4] 4 H20 at different hydrostatic pressures (T = 295 K)133). The emission intensities at different pressures cannot be compared. The excitation wavelength was varied with pressure to fit approximately the maximum of the E c polarized reflectance. For the high pressure investigations a modified sapphire cell of Bridgman s opposed anvil type was used. The pressure was determined by the amount of red-shift of the Rt- and R2-lines167) of ruby crystals placed around the sample... Fig. 33. Polarized emission spectra of single-crystal Ba[Pt(CN)4] 4 H20 at different hydrostatic pressures (T = 295 K)133). The emission intensities at different pressures cannot be compared. The excitation wavelength was varied with pressure to fit approximately the maximum of the E c polarized reflectance. For the high pressure investigations a modified sapphire cell of Bridgman s opposed anvil type was used. The pressure was determined by the amount of red-shift of the Rt- and R2-lines167) of ruby crystals placed around the sample...

See other pages where Hydrostatic shift is mentioned: [Pg.350]    [Pg.530]    [Pg.350]    [Pg.530]    [Pg.449]    [Pg.397]    [Pg.370]    [Pg.185]    [Pg.189]    [Pg.308]    [Pg.141]    [Pg.139]    [Pg.187]    [Pg.315]    [Pg.259]    [Pg.170]    [Pg.353]    [Pg.89]    [Pg.304]    [Pg.233]    [Pg.308]    [Pg.238]    [Pg.161]    [Pg.310]    [Pg.29]    [Pg.371]    [Pg.334]    [Pg.58]    [Pg.284]    [Pg.286]    [Pg.179]    [Pg.107]    [Pg.129]    [Pg.22]   
See also in sourсe #XX -- [ Pg.350 ]




SEARCH



Hydrostat

Hydrostatic

© 2024 chempedia.info