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Leak aperture

Thermal radiation s influence range of jet fire is proportional to leak aperture size and pipeline operating pressure. The farthest influence distance of thermal radiation is about 86 m in large aperture leak, while in complete rupture, thermal radiation s influence distance will be up to 1570 m, and the death radius is also increased significantly. [Pg.1203]

In case of a limited current sensor with a leak aperture according to Fig. 4 the flux J of the gaseous component to be measured to the working electrode can be calculated from the following equation ... [Pg.67]

Moisture from Air Leaks through Cracks and Apertures... [Pg.430]

Building areas separated by physical walls (e.g., halls, rooms, booths) located on the same level. The wall has either intentional apertures or leaks (Fig. 7.107c2). [Pg.591]

Limited aperture releases are conceptualized in Figure 4-2. For these releases material is ejected from holes and cracks in tanks and pipes, leaks in flanges, valves, and pumps, and severed or ruptured pipes. Relief systems, designed to prevent the overpressuring of tanks and process vessels, are also potential sources of released material. [Pg.111]

Volatile or volatilizable compounds may be introduced into the spectrometer via a pinhole aperture or molecular leak which allows a steady stream of sample molecules into the ionization area. Non-volatile or thermally labile samples are introduced directly by means of an electrically heated probe inserted through a vacuum lock. Numerous methods of sample ionization are available of which the most important are electron impact (El), chemical ionization (CY), field ionization (FI), field desorption (FD), fast atom bombardment (FAB), and radio-frequency spark discharge. [Pg.427]

Figure 6. Diagram of our 1-atm ion mobility spectrometer (IMS) apparatus (a) stainless steel source gas dilution volume, (b) septum inlet, (c) needle valve, (d) Nj source gas supply, (e) source and drift gas exhaust, (f) flow meter, (g) pressure transducer, (h) insulated box, (i) drift tube, (j) ion source, (k) Bradbury-Nielson gate, (I) Faraday plate/MS aperture, (m) drift gas inlet, (n) universal joint, (o) electrostatic lens element, (p) quadrupole mass filter, (q) 6"-diffusion pump, (r) first vacuum envelope, (s) channeltron electron multiplier, (t) second vacuum envelope, (u) 3"-dif-fusion pump, (v) Nj drift gas, (w) leak valve, (x) on/off valves, (y) fused silica capillary, (z) 4-liter stainless steel dilution volume, (aa) Nj gas supply. Figure 6. Diagram of our 1-atm ion mobility spectrometer (IMS) apparatus (a) stainless steel source gas dilution volume, (b) septum inlet, (c) needle valve, (d) Nj source gas supply, (e) source and drift gas exhaust, (f) flow meter, (g) pressure transducer, (h) insulated box, (i) drift tube, (j) ion source, (k) Bradbury-Nielson gate, (I) Faraday plate/MS aperture, (m) drift gas inlet, (n) universal joint, (o) electrostatic lens element, (p) quadrupole mass filter, (q) 6"-diffusion pump, (r) first vacuum envelope, (s) channeltron electron multiplier, (t) second vacuum envelope, (u) 3"-dif-fusion pump, (v) Nj drift gas, (w) leak valve, (x) on/off valves, (y) fused silica capillary, (z) 4-liter stainless steel dilution volume, (aa) Nj gas supply.
For gas systems The pressure inside the vessel should be well controlled and kept low. An example of a gas-containing vessel is given in Figure 3-5a [22]. Apertures serve as a differentially evacuating system and sample gas is admitted into the chamber through an automatically controlled leak valve. The pressure is... [Pg.46]

Typical leak size is usually divided into small, medium, large and extra-large level. In this simulation, in order to determine the consequences of the accident in the ordinary and extreme cases, main consideration is taken into pipeline medium aperture leak and large aperture leak. According to the criteria recommended by DNV (TNO 1997, TNO 1992, TNO 1988, TNO 1999), this paper determines the representation of aperture 100 mm (large aperture) and 1200 mm (complete rupture). [Pg.1201]

At 1219 mm diameter, 11 MPa pressure and large aperture leak (100 mm), thermal radiation influence range of jet fire is shown in Figure 2. Under complete rupture (1200 mm) condition, thermal radiation influence range of jet fire is shown in Figure 3. [Pg.1202]

Figure 3. Thermal radiation influence range of jet fire under 4>1200 aperture leak (d = 1219, P = 11 MPa). Figure 3. Thermal radiation influence range of jet fire under 4>1200 aperture leak (d = 1219, P = 11 MPa).
As shown in Figure 4, if large aperture leaks, minor injuries zone s maximum distance is about 156 m on one side of the pipe when AP > 0.017 MPa. As shown in Figure 5, in complete rupture, minor injuries zone s maximum distance is about 520 m on one side of the pipe and 200 m along the pipeline route when AP > 0.017 MPa. [Pg.1203]

In all cases a circular aperture is assumed. This is not necessarily in line with reality. The contraction of flow on discharge and different degrees of friction depending on the roughness and shape of the leak contours are accounted for by the discharge coefficient p. Values between 0.595 and 0.62 are used they increase with increasing smoothness of the leak contours [13]. [Pg.449]

The released fluid may be a gas or a vapour, a liquid, a two-phase mixture, a mixture of several components or a fluid in supercritical state (vid. Example 10.19). If the release is from a vessel storing a liquefied gas, liquid is released if the leak is below the liquid level. If the leak is above the level either vapour or a mixture of liquid and vapour is released. For a given difference of pressures across the leak usually higher mass flow rates are reached if a liquid or liquid/vapour mixture is released than in case of a gas or vapour. The equipment from which the release takes place can be a vessel or a heat exchanger, a pump or a pipe. The maximum released quantity depends on the material inventory and the possibility of isolating the leak. The size of the leak may vary between a large portion of the vessel surface and a limited aperture as that of a hole. [Pg.450]

Vacuum is effective in collecting ISF firom skin that has been mechanically penetrated or had the stratum comeum removed. As with blood collection studies, large site-to-site and person-to-person variability is observed. A large vacuum headspace in the collection devise results in a decrease in volume due to evaporation and an increase in analyte concentrations. Outgassing of dissolved gas in the ISF and leaks between the skin and vacuum source lead to the formation of bubbles in the ISF stream over time. The application of one-half atmosphere vacuum through a harvesting head with an aperture of 2.5 mm over a 1 mm pattern of micropores produced by laser ablation of a black dye yields straw-colored interstitial fiuid at fiow rates of 5-15 pL/h for several days [4]. Vacuum collection over a much larger area (about 1 cm ) is required to collect similar amounts of ISF from low-frequency ultrasound-treated skin [8]. [Pg.1309]

DRIE is essential in fabrication of small features. DRIE is capable of reproducing accurately practically any features that have been defined by lithography. Fluid dynamics studies of microflows utilize DRIE for making accurately dimensioned microchannels and orifices. Membrane stmctures with small holes are useful in many drug delivery, fuel ceU, and cell probing applications. In a patch clamp application, submicrometer apertures have been etched in 20 pm thick silicon membrane. In catalysis studies a small DRIE fabricated capillary leak into a mass spectrometer enabled increased sensitivity and fast respmise times. Integration of... [Pg.2919]

An alternative technique is offered by the Charge-Free Anti-contamination System (CFAS) which was used to produce the series of micrographs shown in Figs. 16-21. In this system, the specimen chamber of the SEM is isolated from the main instrument vacuum pumps. A mechanical roughing pump with controlled leak is used to evaluate the specimen chamber. The objective aperture requires to be mounted in the electron optical column, in such a way that a pressure differential can be maintained across it. Thus, the electron gun and path between the electron source and the... [Pg.568]

The basic idea is that the object under study itself forms the bottom of the cell. Modeling Plasticine (Flair Leisure Products pic, Sutton, UK) was applied around the aperture to prevent gas leaks. Antique silver objects of different sizes could be directly analyzed in this simple way to minimize sample damage. [Pg.870]


See other pages where Leak aperture is mentioned: [Pg.485]    [Pg.581]    [Pg.67]    [Pg.67]    [Pg.485]    [Pg.581]    [Pg.67]    [Pg.67]    [Pg.101]    [Pg.610]    [Pg.113]    [Pg.611]    [Pg.1036]    [Pg.251]    [Pg.228]    [Pg.151]    [Pg.247]    [Pg.303]    [Pg.160]    [Pg.1202]    [Pg.15]    [Pg.195]    [Pg.529]    [Pg.326]    [Pg.628]    [Pg.2495]    [Pg.248]    [Pg.47]   
See also in sourсe #XX -- [ Pg.2 , Pg.413 ]




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