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Pressure temperature changes

In a final use of another (or the same) airtight enclosed vapor degreaser, one could perform cyclic operations — an increase of pressure (hence temperature) followed in some time hy a reduction of pressure (hence temperature). The purpose of the pressure/temperature change would he to subject soil structures to thermal stresses, thereby weakening them, or their bonds to surfaces. An example is plotted in Figure 2.3 where the pressure is cycled about (2/3) of an atmosphere around atmospheric pressure over a time period of about two and one-half minutes (Box 2.2). [Pg.69]

Skin responds to pressure, temperature changes and various stimuii reiated to pain >- The skeietai structure receptors in our joints, tendons and muscies are sensitive to body movement and position. [Pg.241]

Integration of this equation at constant pressure would give a relation for AG for a constant-pressure temperature change. [Pg.178]

Using the data in Table 3.1, find the amount of heat absorbed by 2.0 mol of carbon monoxide in an isobaric (constant-pressure) temperature change from 400 to 1000 K. [Pg.79]

Reduction of reactor inventory by increasing temperature or pressure, by changing catalyst, or by better mixing... [Pg.271]

The main component of sandstone reservoirs ( siliciclastic reservoirs ) is quartz (Si02). Chemically it is a fairly stable mineral which is not easily altered by changes in pressure, temperature or acidity of pore fluids. Sandstone reservoirs form after the sand grains have been transported over large distances and have deposited in particular environments of deposition. [Pg.13]

Dissolution and replacement. Some minerals, in particular carbonates, are not chemically stable over a range of pressures, temperatures and pH. Therefore there will be a tendency over geologic time to change to a more stable variety as shown in Figure 5.12. [Pg.87]

The research activity here presented has been carried out at the N.D.T. laboratory of l.S.P.E.S.L. (National Institute for Occupational Safety and Prevention) and it is aimed at the set up of the Stress Pattern Analysis by Measuring Thermal Emission technique [I] applied to pressure vessels. Basically, the SPATE system detects the infrared flux emitted from points resulting from the minute temperature changes in a cyclically stressed structure or component. [Pg.408]

The enthalpy change AH for a temperature change from to T2 can be obtained by integration of the constant pressure heat capacity... [Pg.1901]

The previous subsection described single-experiment perturbations by J-jumps or P-jumps. By contrast, sound and ultrasound may be used to induce small periodic perturbations of an equilibrium system that are equivalent to periodic pressure and temperature changes. A temperature amplitude 0.002 K and a pressure amplitude 5 P ss 30 mbar are typical in experiments with high-frequency ultrasound. Fignre B2.5.4 illustrates the situation for different rates of chemical relaxation with the angular frequency of the sound wave... [Pg.2121]

By subjecting boron nitride (a white powder) to high pressure and temperature small crystals of a substance harder than diamond, known as borazon, are obtained. This pressure-temperature treatment changes the structure from the original graphite-like layer structure (p. 163) to a diamond-like structure this hard form can withstand temperatures up to 2000 K. [Pg.156]

It is a well-known fact that substances like water and acetic acid can be cooled below the freezing point in this condition they are said to be supercooled (compare supersaturated solution). Such supercooled substances have vapour pressures which change in a normal manner with temperature the vapour pressure curve is represented by the dotted line ML —a continuation of ML. The curve ML lies above the vapour pressure curve of the solid and it is apparent that the vapour pressure of the supersaturated liquid is greater than that of the solid. The supercooled liquid is in a condition of metastabUity. As soon as crystallisation sets in, the temperature rises to the true freezing or melting point. It will be observed that no dotted continuation of the vapour pressure curve of the solid is shown this would mean a suspended transformation in the change from the solid to the liquid state. Such a change has not been observed nor is it theoretically possible. [Pg.23]

The connections between simulation and thermodynamics can be carried further. Simulations can be set up to be constant volume, pressure, temperature, and so on. Some of the most sophisticated simulations are those involving multiple phases or phase changes. These techniques are discussed further in Chapter 7. [Pg.15]

This expression describes the variation of the pressure-temperature coordinates of a first-order transition in terms of the changes in S and V which occur there. The Clapeyron equation cannot be applied to a second-order transition (subscript 2), because ASj and AVj are zero and their ratio is undefined for the second-order case. However, we may apply L Hopital s rule to both the numerator and denominator of the right-hand side of Eq. (4.47) to establish the limiting value of dp/dTj. In this procedure we may differentiate either with respect to p. [Pg.246]

An extraction plant should operate at steady state in accordance with the flow-sheet design for the process. However, fluctuation in feed streams can cause changes in product quaUty unless a sophisticated system of feed-forward control is used (103). Upsets of operation caused by flooding in the column always force shutdowns. Therefore, interface control could be of utmost importance. The plant design should be based on (/) process control (qv) decisions made by trained technical personnel, (2) off-line analysis or limited on-line automatic analysis, and (J) control panels equipped with manual and automatic control for motor speed, flow, interface level, pressure, temperature, etc. [Pg.72]

Most thermometry using the KTTS direcdy requites a thermodynamic instmment for interpolation. The vapor pressure of an ideal gas is a thermodynamic function, and a common device for reali2ing the KTTS is the helium gas thermometer. The transfer function of this thermometer may be chosen as the change in pressure with change in temperature at constant volume, or the change in volume with change in temperature at constant pressure. It is easier to measure pressure accurately than volume thus, constant volume gas thermometry is the usual choice (see Pressure measurement). [Pg.396]


See other pages where Pressure temperature changes is mentioned: [Pg.965]    [Pg.788]    [Pg.277]    [Pg.169]    [Pg.969]    [Pg.211]    [Pg.8]    [Pg.8153]    [Pg.965]    [Pg.788]    [Pg.277]    [Pg.169]    [Pg.969]    [Pg.211]    [Pg.8]    [Pg.8153]    [Pg.345]    [Pg.344]    [Pg.1914]    [Pg.73]    [Pg.3]    [Pg.142]    [Pg.273]    [Pg.388]    [Pg.108]    [Pg.221]    [Pg.94]    [Pg.95]    [Pg.512]    [Pg.511]    [Pg.165]    [Pg.193]    [Pg.131]    [Pg.148]    [Pg.315]    [Pg.364]    [Pg.368]    [Pg.396]    [Pg.473]    [Pg.503]    [Pg.563]    [Pg.518]    [Pg.631]   
See also in sourсe #XX -- [ Pg.411 ]




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Changing temperature

Changing the Pressure and Temperature

Pressure and temperature changes with a single-component system qualitative discussion

Pressure, Temperature and Phase Changes

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