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Linear decompression

As far as the external pressure (p ) is concerned, thee are two simple cases (1) instantaneous decompression when is a constant, and (2) linear decompression with constant rate of decompression. The first case might occur in a sudden volcanic explosion or when a magma column is decompressed by sector collapse. The second case is an approximation to pressure evolution during magma ascent. [Pg.278]

In many circumstances during magma ascent the pressure decreases at a finite rate. Assuming the rate of decompression is a constant, the consequences for linear decompression using the thin shell model may be presented to express the bubble radius as a function of time in a constantly varying pressure field. The external pressure is expressed by [Pg.278]

Thick shell melt model during instantaneous decompression [Pg.279]

For a thick shell model (Fig. 13.2) where R S, we have R I MR. If we further ignore the surface tension (tT ). then Eq. (13.22) may be simplified as [Pg.279]

During instantaneous decompression, the external pressure (P ) is a constant. The solution of Eq. (13.63) with initial condition R 0) = Rq is given by (Barclay et al., 1995) [Pg.280]


In reality, the melt productivity, dF/dz (degree of melting per km decompression), is likely to be non-linear with depth (Asimow et al. 1997). Darcy s law can then be used to describe the flow of melt given a permeable matrix and a driving force ... [Pg.212]

During a 33 h continuous hydroformylation run using this set-up, no catalyst decomposition was observed and Rh leaching into the scC02/product stream was less than 1 ppm. The selectivity for the linear nonanal was found to be stable over the reaction time with n/iso = 3.1. During the continuous reaction, alkene, CO, H2 and C02 were separately fed into the reactor containing the ionic liquid catalyst solution. Products and unconverted feedstock dissolved in SCCO2 were removed from the ionic liquid. After decompression the liquid product was collected and analysed. [Pg.200]

The amorphous phase appearing above 20 GPa at room temperature (see above) has also recently been studied by X-ray diffraction [135] and Raman scattering [132,133]. Serebryanaya et al. [135] identify the structure as a three-dimensionally polymerized Immm orthorhombic lattice, but find that compression above 40 GPa gives a truly amorphous structure. In contrast to the orthorhombic three-dimensional polymer structure discussed in the last section, the best fit here is found for (2+2) cycloaddition in two directions, with (3+3) cycloaddition in the third, and thus some relationship to the tetragonal phase. From the in situ X-ray data a bulk modulus of 530 GPa is deduced, about 20% higher than for diamond. Talyzin et al. [132, 133] find that this phase depolymerizes on decompression into linear polymer chains, unless the sample is heated to above 575 K under pressure. A strong interaction with the diamond substrate is also noted, such that only films with a thickness of several hundred nm are able to polymerize fully [ 132]. Hardness tests were also carried out on the polymerized films, which were found to be almost as hard as diamond and to show an extreme superelastic response with a 90% elastic recovery after indentation [133]. [Pg.115]

Most commercial ELSDs employ a standard or modified HPLC nebulizer (Venturi flow type). It was believed that this nebulizer was not necessary for SFC because nebulization of the SFC mobile phase is accomphshed by gas expansion in a restrictor which controls pressure and mobile-phase flow rates. To counter the cooling effects of CO2 decompression in the linear fused-silica restrictor and improve heat transfer, Nizery et al., using a Cunow Clichy Model DDL 10 detector, placed the restrictor tip into a heated brass ring and applied heat to a small section of tubing between the restrictor and the drift tube... [Pg.1541]

Linear profiles are the simplest profiles to use for powder compressions. Typically, a sawtooth or v-shaped profile is used where the punch is extended at a constant velocity and retracts at a constant velocity. In theory, during a sawtooth profile, the punch reverses its motion instantaneously between the compression and a decompression strokes. At low speeds (e.g.. <1 mm/sec), the hydraulic response system can easily accommodate this discontinuity. However, at high speeds (>100mm/.sec), the control system may show a small lag in the position-time waveform (<10 milliseconds) as it attempts to rapidly reverse the direction of punch. The sawtooth waveform is commonly used for more fundamental compression studies (e.g.. Heckel analysis), where the desired powder volume reduction is proportional to time. It is also u.seful when evaluating instrument performance during factory acceptance testing. [Pg.469]

Figure 7. A linear variation of the sqnare of the symmetry breaking strain with pressnre implies second order character for the tetragonal orthorhombic transition in stishovite. Circles represent strains calcnlated nsing flo = (abf and the data of Andranlt et al. (1998) crosses represent strains calcnlated nsing the alternative variation of Oq shown by crosses in Fignre 6. Open sqnares are from single crystal X-ray diffraction data of Mao et al. (1994) D designates measnrements of the orthorhombic phase made dnring decompression. Figure 7. A linear variation of the sqnare of the symmetry breaking strain with pressnre implies second order character for the tetragonal orthorhombic transition in stishovite. Circles represent strains calcnlated nsing flo = (abf and the data of Andranlt et al. (1998) crosses represent strains calcnlated nsing the alternative variation of Oq shown by crosses in Fignre 6. Open sqnares are from single crystal X-ray diffraction data of Mao et al. (1994) D designates measnrements of the orthorhombic phase made dnring decompression.
Raman spectra were collected and examined as a function of pressure to detect possible phase transitions. On decompression from 40 to 1 GPa, changes in the room temperature Raman spectra appear to be steady and continuous. Moreover, the evolution of the peak positions with pressure is linear for V4, Vi, vi, Vno+ as well as the major lattice modes. Therefore, low-temperature Raman spectra were collected in the expectation that peaks would be better resolved and thereby respond more sensitively to pressure. Using liquid nitrogen as cryogen, we maintain the system at constant temperature 80 K. Under such conditions, the Raman spectra were measured as a function of pressure between 14 GPa and ambient and are plotted in Fig. 2. At such a low temperature, both the lattice and internal modes exhibit sharp profile and significant pressure shifts. These changes in the Raman spectrum can be interpreted as evidence for a phase transition in NO Os. ... [Pg.196]

Practical aspects. All compounds which contain oxidizable carbon can be detected. A linear range over seven decades and a detection limit of a few pg/s of carbon make this mass flow-sensitive detector very suitable for GC. It has also found increased application in SFC when CO2 is used as the mobile phase. Decompression from the supercritical state to atmospheric pressure is performed by a restriction capillary at the outlet of the separation column. [Pg.144]

Subaquatic activities External otitis, intertrigo, staphylococcal infections, burns, linear abrasions from wetsuit folds, pruritus and erythema from decompression, napkin eruption type dermatitis... [Pg.245]

The zero-meter screw is used to reduce the viscous heat generation (power consumption) in the melt conveying zone of the extruder by having a relatively deep channel in this portion of the screw, with the depth reducing linearly with distance. Another similar approach is the decompression screw shown in Fig. 8.36. [Pg.552]


See other pages where Linear decompression is mentioned: [Pg.278]    [Pg.278]    [Pg.1891]    [Pg.23]    [Pg.218]    [Pg.325]    [Pg.989]    [Pg.270]    [Pg.1650]    [Pg.21]    [Pg.2349]    [Pg.998]    [Pg.261]    [Pg.2332]    [Pg.599]    [Pg.601]    [Pg.858]    [Pg.1895]    [Pg.107]    [Pg.86]    [Pg.33]    [Pg.438]    [Pg.21]    [Pg.53]    [Pg.22]    [Pg.237]   


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