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Pressure changing steps

By using the method of characteristics, the propagation velocity of the concen-hation front can be expressed. The two pressure-changing steps can be accounted for using ideal gas law and assuming zero axial pressure drop. [Pg.39]

But another approach to multi-step cooling [8, 9] involves dealing with the turbine expansion in a manner similar to that of analysing a polytropic expansion. Fig. 4.4 shows gas flow (1 + ijj) at (p,T) entering an elementary process made up of a mixing process at constant pressure p, in which the specific temperature drops from temperature T to temperature T, followed by an isentropic expansion in which the pressure changes to (p dp) and the temperature changes from T to (7 - - dT). [Pg.53]

This is a quantitative thermod mamics problem that asks us to determine entropy under nonstandard conditions using standard thermod3mamic data, so we apply the seven-step approach. The problem asks for two quantities the molar entropy of O2 gas in the pressurized tank and the entropy change when a sample of that gas undergoes a pressure change. [Pg.998]

The second method for the study of relaxation in spin-state equilibria makes use of the rapid change of pressure. Single-step pressure-jump relaxation requires an observation time of about lO s which is too slow. However, the... [Pg.69]

In a chemical process, the transformation of raw materials into desired chemical products usually cannot be achieved in a single step. Instead, the overall transformation is broken down into a number of steps that provide intermediate transformations. These are carried out through reaction, separation, mixing, heating, cooling, pressure change, particle size reduction or enlargement. Once individual steps have been selected, they must be interconnected to carry out the... [Pg.4]

A Met Glass sample was tested at 400°C with a varying mixture of He and Hj. The desired test gas was introduced into the test chamber and a mass spectrometer was used to monitor breakthrough and gas composition on the test side of the permeation apparatus. The results of the test are shown in Fig. 8. The step pressure changes for the He introduction do not result in He being detected on the sampling side, whereas, when H2 is introduced a pressure is detected by the mass spectrometers almost immediately. [Pg.157]

In a case of the PCX absorption curve after evacuation, the system must be heated up to a test temperature and thermally stabilized. Then by gradually increasing pressure we will observe hydrogen absorption related to a particular pressure of hydrogen. It is important that the time of visible pressure change at every step is closely connected with the kinetics of process at an applied temperature. [Pg.69]

For overall Arrhenius parameters (based on measurements of the overall rate constant as a function of temp), there are no normal values if the reaction involves several elementary steps of comparable rates. Indiscriminate use of such parameters in assessing detonation phenomena (eg, hot spots) can lead to gross errors. The reader is reminded that much of the existing kinetic data for explosives are based on the measurement of the overall pressure changes in the system under study. Unless the detailed reaction sequence, usually called the reaction mechanism, is known, Arrhenius parameters based on pressure change measurement can be most unreliable... [Pg.545]

This second step is accomplished using the coefficient of isothermal compressibility. Methods of estimating values of this compressibility coefficient will be discussed later in this chapter. However, we now will show the use of compressibility in computing density changes corresponding to pressure changes. [Pg.316]

Step 3 Write the equilibrium molar concentrations or partial pressures by adding the change in molar concentration or partial pressure (from step 2) to the initial value for each substance (from step 1). [Pg.569]

In applying Le Chatelier s principle to a heterogeneous equilibrium, the effect of pressure changes on solids and liquids can be ignored because the volume (and concentration) of a solid or a liquid is nearly independent of pressure. Consider, for example, the high-temperature reaction of carbon with steam, the first step in converting coal to gaseous fuels ... [Pg.553]

Thus the pressure of any shock wave generated in a pipeline would continue to rise if it were not for the fact that at a time 2Lie a return unloading pressure wave reaches the valve and stops the pressure rise at a value of about 53 ft, as contrasted with about three times that value if this were not the case. Subsequent pressure changes as elastic waves travel back and forth are very complex and require a detailed step-by-step analysis that is beyond the scope of this text. In brief, the method consists of assuming that the valve movement takes place in a series of steps each of which produces a pressure p proportional to each V. Other texts contain details of computing successive pressures for slow valve closure and further explanation of much of this condensed treatment [47-49]. [Pg.506]

SYSMAC-mini, OMRON). The operation of solenoid valves and the pressure change of the system are schematically shown in Figure 5. When the solenoid valves S1-S4-S5-S8 were opened while the others represented by S2-S3-S6-S7 remained close, left column was in the adsorption step and right column was in the desorption step, and vice versa. [Pg.306]

Select an observation period equilibrium will be considered to be reached if, over that period, the pressure changes by less than the minimum pressure step determined above. [Pg.86]

Uptake is measured by following the response of a step function change in the gas-phase concentration of a probe molecule to be adsorbed on the sample. Various techniques have been developed to follow such a response, such as gravimetric measurements of the mass change of the solid (99,100) and volumetric measurements of the pressure change in a constant volume caused by molecular adsorption (101). [Pg.369]

Gas pressures in vacuum applications are usually either recorded via membrane transducers, systems that monitor the gas density via partial ionisation of the gas or sensors that make use of the fact that the thermal conductivity or diffusivity of a gas is pressure dependent. The first type of transducer is sensitive to the total gas pressure while the other methods yield gas dependent signals. In terms of application properties such as the response time of the sensor, the sensitivity and the pressure range that the sensor covers are important technical specifications. The response of a membrane pressure sensor to a step-like pressure change is essentially an exponential function characterized by a relaxation time r for a MKS transducer, type Baratron 220 [1], r was determined to be 0.227 s (see Fig. 1), the actual pressure and the value as recorded by the transducer therefore do not match within the error bars given for the sensor until more than a second passed. [Pg.443]

Notice that the pressure change term in the first step (V AP = -0.0782 kJ/mol) accounts for less than 0.1% of the overall process enthalpy change. We will generally neglect the effects of pressure changes on A/ unless AP is on the order of 50 atm or more. [Pg.380]


See other pages where Pressure changing steps is mentioned: [Pg.177]    [Pg.31]    [Pg.161]    [Pg.177]    [Pg.31]    [Pg.161]    [Pg.1]    [Pg.513]    [Pg.788]    [Pg.738]    [Pg.93]    [Pg.118]    [Pg.113]    [Pg.222]    [Pg.456]    [Pg.143]    [Pg.216]    [Pg.62]    [Pg.110]    [Pg.202]    [Pg.299]    [Pg.81]    [Pg.449]    [Pg.62]    [Pg.83]    [Pg.143]    [Pg.81]    [Pg.612]    [Pg.91]    [Pg.202]    [Pg.455]    [Pg.447]    [Pg.368]    [Pg.158]   
See also in sourсe #XX -- [ Pg.161 ]




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