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Reversible phenomena

Boltzmann s H-Theorem. —One of the most striking features of transport theory is seen from the result that, although collisions are completely reversible phenomena (since they are based upon the reversible laws of mechanics), the solutions of the Boltzmann equation depict irreversible phenomena. This effect is most clearly seen from a consideration of Boltzmann s IZ-function, which will be discussed here for a gas in a uniform state (no dependence of the distribution function on position and no external forces) for simplicity. [Pg.17]

In the absence of viscosity, rarefaction waves are thermodynamically reversible phenomena, that is, no change in entropy is involved and the ordinary laws of adiabatic expansion can be applied. Shock waves, on the other hand, ate irreversible there is a continuous dissipation of energy into heat (Ref 1)... [Pg.501]

Scheme 61 Synthesis of mixed-alkylated yttrocene(III) tetraalkylaluminate complexes (top) and reversibility phenomena in aluminate chemistry (bottom) [24]... Scheme 61 Synthesis of mixed-alkylated yttrocene(III) tetraalkylaluminate complexes (top) and reversibility phenomena in aluminate chemistry (bottom) [24]...
The properties of nanocomposite systems, whose microstructures aim at reproducing real systems, have been examined in various numerical modelling studies [127, 128], In general, the essential features of the hysteresis cycles may be satisfactory reproduced. In particular, soft layer reversal is quantitatively accounted for, which is expected for reversible phenomena. By contrast, the calculated high-field irreversible reversal of the hard phase magnetization is not reproduced in general. Such discrepancy illustrates the already mentioned difficulty to describe irreversible processes. [Pg.351]

Joule s law is strictly accurate so long as the conductor in which the evolution of heat is measured is homogeneous and at a uniform temperature throughout. If these conditions are not complied with, deviations from the law are obtained, and the evolution of heat is found to be no longer completely irreversible. By raising the temperature of certain parts of the circuit, electric currents can now be obtained. These reversible phenomena are called thermoelectrical phenomena in the more restricted sense of the term. In common with all other reversible processes, they must follow certain regularities, which are deter-... [Pg.362]

In chemistry, equilibrium processes are the only reactions which can be treated as reversible phenomena. [Pg.33]

Nephrotoxins or ischemic disorders can initiate acute renal failure. Shock, hemorrhage, septicemia, or vasodilation due to hypertensive medication can precipitate ischemic acute renal failure. Systemic reactions to certain drugs and nephrotoxins such as aminoglycoside antibiotics and heavy metals lead to acute renal failure. The extent of retention of creatinine and urea in blood is directly related to the severity of acute renal failure. This condition is not readily reversible and, as such, should be distinguished from reversible phenomena such as prerenal or postrenal azotemia, in which there is also an increase in levels of plasma urea and creatinine (13). In volume-depleted states, for example, diarrhea, the kidney is hypoprefused. This results in increased back diffusion of urea into the circulation from the tubular fluid because of the reduced urine flow. In addition to an increase in urea levels in circulation, there is also a slow increase in creatinine levels. Plasma urea and creatinine levels can be restored to normal within 24 hours by appropriate fluid and electrolyte replacement in prerenal azotemia. In condi-... [Pg.136]

The temperature dependence of hole formation and hole profile is affected by four factors decrease in the Debye-Waller factor, broadening of the hole width, spectral diffusion, and laser-induced hole filling. The first two effects are reversible phenomena and recover at low temperatures. The latter two are irreversible and their influence cannot be eliminated by cooling the sample again. The temperature dependence of the Debye-Waller factor (DiV(T) — S0(T)/S 4)) for TPP/PMMA and TPP/phenoxy resin systems, shown in Table 2.13 by a dotted line, agrees well with the slope of 0 at 4-20 K. The temperature dependence of the Debye-Waller factor is smaller in poly(vinyl alcohol), which shows a higher Es value (23 cm4). Thus, hole formation efficiency is controlled by the temperature dependence of Debye-Waller factor for temperatures below T and, for temperatures above T it is affected mainly by the simultaneous occurrence of spectral diffusion and laser-induced hole filling due to structural relaxation. [Pg.100]

An elementary thermocouple circuit is shown in Fig. 16.16. The EMF generated in this circuit is a function of the materials used and the temperatures of the junctions. It is useful to describe briefly the basic thermoelectric phenomena or effects that are related to the Seebeck effect and are present in thermocouple measurements. They include two well-known irreversible phenomena—Joule heating and thermal conduction—and two reversible phenomena—the Peltier effect and the Thompson effect. [Pg.1181]

When the firing rate is lowered, the reverse phenomena take place Gases take longer to traverse the same path, and so each molecule of poc has more residence time during which to deposit its heat on the loads, but its coefficient of heat transfer is less (a function of velocity to only the 0.52 to 0.80 power). [Pg.184]

Certain performance losses of fuel cells during steady-state operation can be fully or partially recovered by stopping and then restarting the life test. These recoverable losses are associated to reversible phenomena, such as cathode catalyst surface oxidation, cell dehydration or incomplete water removal from the catalyst or diffusion layers [85]. Other changes are irreversible and lead to unrecoverable performance losses, such as the decrease in the ECSA of catalysts, cathode contamination with ruthenium, membrane degradation, and delamination of the catalyst layers. [Pg.343]

Moreover, by the second law of thermodynamics, the entropy production is always positive for irreversible phenomena and zero for reversible phenomena. If the Eqs. (7) are introduced into the expression (4) for ds. /dt one obtains a quadratic form which has to be non-negative. Hence, all principal minors of the quadratic form must be non-negative and we find... [Pg.373]

When the current is decreased, the combined effect of the changes in the partial pressures and the polarisation losses results in the increase of the cell voltage. It is observed that the cell voltage initially overshoots before settling to a steady-state value. The FU and the OU, which are proportional to the current, also decrease. The reverse phenomena are observed with the increase in the external load current. The sudden decrease in the load current results in the decrease in the rate of hydrogen and oxygen consumption and the rate of water vapour formation. In other words, the... [Pg.379]

The decrease in the current also results in the decrease in the polarisation losses and the decrease in the reaction entropy flow rate (5r) (due to reduced mass flow rates) and thereby results in the fall of the system temperature. The reverse phenomena are observed (at time 2000 s in Fig. 10.8) when the load current density is increased. [Pg.380]

Analogous results have been obtained with a large number of colloid dispersions and a variety of hydrolyzable ions. Since the hydrolysis products vary with the metal ion and the pH, their adsorption and charge reversal phenomena will differ in each case, as shown with ferric [15], chromium [16], zinc [17], and other ions. [Pg.855]

An important additive to NR compounds used for bonding rubber to brass is a cobalt salt, such as cobalt naphthenate. While this additive improves the stability of the rubber-brass bond, especially in a corrosive environment, it exerts a negative effect on the stability of the rubber network, in that it accelerates reversion phenomena especially in the presence of oxygen and at elevated temperatures. [Pg.164]

For the OCP, charge reversal phenomena can be ignored so that must remain positive. Consequently, by virtue of (29) and (31), the renormalisation factor is bounded... [Pg.136]

The curves of Fig. 11.1 are true equilibrium curves and therefore represent completely reversible phenomena. The conditions corresponding to point A on... [Pg.571]

Certain performance losses incurred by the cell during steady-state operation can be recovered, fuUy or in part, by stopping and then restarting a life test. Such recoverable performance losses are usually associated with reversible phenomena occurring in the fuel cell, for example, cathode catalyst surface oxidation, cell dehydration, and incomplete water removal from the catalyst layer and/or gas-diffusion layer (GDL). [Pg.105]

Flocculation and creaming are reversible phenomena, while coagulation is not. [Pg.235]

Physical aging and structural recovery are reversible phenomena. There is no change in chemical structure during physical aging. The changes in physical and mechanical properties that accompany structural recovery ai e caused by the... [Pg.102]

Reversible Modes of Physical Degradation Some modes of physical degradation are a result of reversible phenomena, including the following ... [Pg.356]

The C—H insertion of diazoalkanes to the allylic position is a competitive reaction to cyclopropanation. For example, the reaction of aryldiazoacetate 168 to silyl enol ether 169 catalyzed by Rh2(5-DOSP)4 160 gave chiral cyclopropane 171 selectively in 95% ee, while the use of Rh2(5-PTAD)4 170 led to a C—H insertion reaction to the same alkene to give 172 (Scheme 1.79) [125]. On the other hand, the reverse phenomena were observed in the reaction of dihydronaphthalene 173, where Rh2(5-DOSP)4 160 efficiently catalyzed asymmetric cyclopropanation to give 174, while Rh2(5-PTAD)4 170 promoted a C—H insertion reaction to give 175 (Scheme 1.80) [126]. [Pg.22]

As an alternative to a linear rate of temperature change it is possible to overlay a harmonic thermal oscillation over a linear temperature ramp. The net result is an average change of temperature equal to the linear temperature ramp with an observed temperature that fluctuates at a fixed frequency, each successive peak being a fixed increment in temperature higher or lower than the preceding one. The amplitude and frequency of the oscillation can be independently varied. This method was developed to distinguish reversible phenomena from nonrever-... [Pg.292]


See other pages where Reversible phenomena is mentioned: [Pg.350]    [Pg.106]    [Pg.508]    [Pg.211]    [Pg.256]    [Pg.710]    [Pg.177]    [Pg.579]    [Pg.137]    [Pg.136]    [Pg.786]    [Pg.15]    [Pg.95]    [Pg.384]    [Pg.122]    [Pg.122]    [Pg.403]    [Pg.4]    [Pg.120]    [Pg.164]    [Pg.64]    [Pg.320]    [Pg.83]    [Pg.2582]   
See also in sourсe #XX -- [ Pg.32 ]




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