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Temperature Dependence of Effects

A relationship exists for the dependence of reaction rate on temperature. It is expressed by an equation of Arrhenius  [Pg.131]

Activation energy Ea and activation enthalpy AH are linked with each other as follows  [Pg.132]

E k is known for any temperature, AG can be calculated according to equation 2.90. Furthermore, the following is valid  [Pg.132]

Using plots of log k against 1 /T, the activation energy of the Arrhenius equation can be determined. For ewyme catalyzed reactions, Ea is 10-60, for chemical reactions this value is 50-150 and for the inactivation of enz)mes, the unfolding of proteins, and the killing of microorganisms, 250-350 kJ/mol are required. [Pg.132]

For enzymes which are able to convert more than one substrate or compound into product, the activation energy may be dependent on the substrate. One example is alcohol dehydrogenase, an important enzyme for aroma formation in semiripened peas (Table 2.13). In this case the activation energy for the reverse reaction is only slightly influenced by substrate. [Pg.132]


The possible role of nickel formate as an intermediate in the breakdown of formic acid on nickel has been extensively discussed (3, 232, 240b, 244) this is another catalytic reaction in which there is compensation behavior (Table III, R). While the observed obedience to Eq. (2) does not identify the reaction mechanism, it is probably significant that catalytic activity becomes apparent in the temperature range of onset of salt instability. Again it may be envisaged that the temperature dependence of effective concentration of nickel formate intermediate may vary with reaction conditions. [Pg.293]

Fig. 8.32. Temperature dependence of effective magnetic moments for the 4Tlg term at different applied fields m—based on the mean magnetic susceptibility d—based on the differential magnetic susceptibility (solid) a—based on the approximate magnetic susceptibility via the van Vleck equation. Fig. 8.32. Temperature dependence of effective magnetic moments for the 4Tlg term at different applied fields m—based on the mean magnetic susceptibility d—based on the differential magnetic susceptibility (solid) a—based on the approximate magnetic susceptibility via the van Vleck equation.
Figure 11-2 The temperature dependences of effective magnetic moment, of polycrystalline samples of nitroxide radicals 14 (A) and 22 ( ) observed at 0.2 and 0.1 T, respectively. The best-fit theoretical curves are based on an interacting dimer model and a one-dimensional Heisenberg model, respectively (34]. Figure 11-2 The temperature dependences of effective magnetic moment, of polycrystalline samples of nitroxide radicals 14 (A) and 22 ( ) observed at 0.2 and 0.1 T, respectively. The best-fit theoretical curves are based on an interacting dimer model and a one-dimensional Heisenberg model, respectively (34].
Fig. 7. (a) Temperature dependence of effective dissociative attachment cross section in N2O (A) temperature dependence of dissociative attachment rate coefficient. [Pg.98]

Effect of the enthalpy change for exothermic chemical reaction on the effectiveness factor when the temperature dependence of effective intrapellet diffusion coefficients is neglected in the mass transfer equation. [Pg.738]

The temperature dependence of effective intrapeUet diffusion coefficients is neglected in the mass transfer equation. [Pg.740]

R. Agarwal, N.S. Saxena, K.B. Sharma, S. Thomas, and M.S. Sreekala, Temperature dependence of effective thermal conductivity and thermal diffusivity of treated and untreated polymer composites. J. Appl. Polym. Sci. 89,1708-1714 (2003). [Pg.211]

Table I. Temperature Dependence of Effects of Rapidly Relaxing Spin on... Table I. Temperature Dependence of Effects of Rapidly Relaxing Spin on...
Table 1 Temperature dependence of effective Henry s Law constants for several species in H2SO4. standard state correction was used to convert AS = -30 cal/mol-K to an intercept. Assuming a standard state of 1 atm, the intercept is equ to (AS/4.58 + log [solvent]), where [solvent] is the molarity of the sulfuric acid. ( )A standard state correction was used to convert AS = -21 cal/mol-K to an intercept. Same as in (a). )A standard state correction was used to convert AS = -27 cal/mol-K to an intercept. Same as in (a). Table 1 Temperature dependence of effective Henry s Law constants for several species in H2SO4. standard state correction was used to convert AS = -30 cal/mol-K to an intercept. Assuming a standard state of 1 atm, the intercept is equ to (AS/4.58 + log [solvent]), where [solvent] is the molarity of the sulfuric acid. ( )A standard state correction was used to convert AS = -21 cal/mol-K to an intercept. Same as in (a). )A standard state correction was used to convert AS = -27 cal/mol-K to an intercept. Same as in (a).
Fig. 5. Temperature dependence of effective spin-lattice Tj and spin-spin Ti relaxation times calculated from Eqs. 8 as well as of intrachain and interchain diffusion rates calculated from Eq. 10 for neutral solitons diffusing in trans-PA along and between randomly oriented chains and chains oriented with their c-axis with respect to an external magnetic field by / = 90°, 60°, 30°, and 0°. [From Refs. 12(b) and 61 with permission.]... Fig. 5. Temperature dependence of effective spin-lattice Tj and spin-spin Ti relaxation times calculated from Eqs. 8 as well as of intrachain and interchain diffusion rates calculated from Eq. 10 for neutral solitons diffusing in trans-PA along and between randomly oriented chains and chains oriented with their c-axis with respect to an external magnetic field by / = 90°, 60°, 30°, and 0°. [From Refs. 12(b) and 61 with permission.]...
Relaxation and dynamics properties of charge carriers depend not only on the polymer stmcture, but also on its doping level. The temperature dependence of effective Did aod D3D calculated from Eqs. 10 for PC in PTTF samples with different structure and iodine content are shown in Fig. The Did parameter increases... [Pg.323]

The temperature dependences of effective Djd and D y> calculated from Eqs. 10 for both types of PC in the PANI-EB and some slightly doped PANI were also determined (Fig. io).2 44,45,48 reasonable that the anisotropy of the spin... [Pg.324]

Fig. 10. Temperature dependence of effective coefficients for intrachain and interchain D3D polaron diffusion in the PANI-EB and slightly S A- and HCA-doped PANI samples. [From Refs. 12(b), 44(b), and 45(a) with permission.]... Fig. 10. Temperature dependence of effective coefficients for intrachain and interchain D3D polaron diffusion in the PANI-EB and slightly S A- and HCA-doped PANI samples. [From Refs. 12(b), 44(b), and 45(a) with permission.]...
In principle, the reaction cross section not only depends on the relative translational energy, but also on individual reactant and product quantum states. Its sole dependence on E in the simplified effective expression (equation (A3.4.82)) already implies unspecified averages over reactant states and sums over product states. For practical purposes it is therefore appropriate to consider simplified models for tire energy dependence of the effective reaction cross section. They often fonn the basis for the interpretation of the temperature dependence of thennal cross sections. Figure A3.4.5 illustrates several cross section models. [Pg.776]

Figure B3.6.3. Sketch of the coarse-grained description of a binary blend in contact with a wall, (a) Composition profile at the wall, (b) Effective interaction g(l) between the interface and the wall. The different potentials correspond to complete wettmg, a first-order wetting transition and the non-wet state (from above to below). In case of a second-order transition there is no double-well structure close to the transition, but g(l) exhibits a single minimum which moves to larger distances as the wetting transition temperature is approached from below, (c) Temperature dependence of the thickness / of the enriclnnent layer at the wall. The jump of the layer thickness indicates a first-order wetting transition. In the case of a conthuious transition the layer thickness would diverge continuously upon approaching from below. Figure B3.6.3. Sketch of the coarse-grained description of a binary blend in contact with a wall, (a) Composition profile at the wall, (b) Effective interaction g(l) between the interface and the wall. The different potentials correspond to complete wettmg, a first-order wetting transition and the non-wet state (from above to below). In case of a second-order transition there is no double-well structure close to the transition, but g(l) exhibits a single minimum which moves to larger distances as the wetting transition temperature is approached from below, (c) Temperature dependence of the thickness / of the enriclnnent layer at the wall. The jump of the layer thickness indicates a first-order wetting transition. In the case of a conthuious transition the layer thickness would diverge continuously upon approaching from below.
In order to Introduce thermal effects into the theory, the material balance equations developed in this chapter must be supplemented by a further equation representing the condition of enthalpy balance. This matches the extra dependent variable, namely temperature. Care must also be taken to account properly for the temperature dependence of certain parameters In... [Pg.156]

NMR signals of the amino acid ligand that are induced by the ring current of the diamine ligand" ". From the temperature dependence of the stability constants of a number of ternary palladium complexes involving dipeptides and aromatic amines, the arene - arene interaction enthalpies and entropies have been determined" ". It turned out that the interaction is generally enthalpy-driven and counteracted by entropy. Yamauchi et al. hold a charge transfer interaction responsible for this effect. [Pg.89]

For adsorption from the vapor phase, Kmay be very large (sometimes as high as 10 ) and then clearly the effective diffusivity is very much smaller than the pore diffusivity. Furthermore, the temperature dependence of K follows equation 2, giving the appearance of an activated diffusion process with... [Pg.260]

With the Monte Carlo method, the sample is taken to be a cubic lattice consisting of 70 x 70 x 70 sites with intersite distance of 0.6 nm. By applying a periodic boundary condition, an effective sample size up to 8000 sites (equivalent to 4.8-p.m long) can be generated in the field direction (37,39). Carrier transport is simulated by a random walk in the test system under the action of a bias field. The simulation results successfully explain many of the experimental findings, notably the field and temperature dependence of hole mobilities (37,39). [Pg.411]

Its value at 25°C is 0.71 J/(g-°C) (0.17 cal/(g-°C)) (95,147). Discontinuities in the temperature dependence of the heat capacity have been attributed to stmctural changes, eg, crystaUi2ation and annealing effects, in the glass. The heat capacity varies weakly with OH content. Increasing the OH level from 0.0003 to 0.12 wt % reduces the heat capacity by approximately 0.5% at 300 K and by 1.6% at 700 K (148). The low temperature (<10 K) heat capacities of vitreous siUca tend to be higher than the values predicted by the Debye model (149). [Pg.505]

Effect of Temperature and pH. The temperature dependence of enzymes often follows the rule that a 10°C increase in temperature doubles the activity. However, this is only tme as long as the enzyme is not deactivated by the thermal denaturation characteristic for enzymes and other proteins. The three-dimensional stmcture of an enzyme molecule, which is vital for the activity of the molecule, is governed by many forces and interactions such as hydrogen bonding, hydrophobic interactions, and van der Waals forces. At low temperatures the molecule is constrained by these forces as the temperature increases, the thermal motion of the various regions of the enzyme increases until finally the molecule is no longer able to maintain its stmcture or its activity. Most enzymes have temperature optima between 40 and 60°C. However, thermostable enzymes exist with optima near 100°C. [Pg.288]

The temperature dependence of the effective charges and dipole moment of water... [Pg.422]

Figure 1 Temperature dependence of the reorganization energy and effective charges on... Figure 1 Temperature dependence of the reorganization energy and effective charges on...

See other pages where Temperature Dependence of Effects is mentioned: [Pg.153]    [Pg.744]    [Pg.66]    [Pg.131]    [Pg.153]    [Pg.744]    [Pg.66]    [Pg.131]    [Pg.423]    [Pg.913]    [Pg.2115]    [Pg.2122]    [Pg.2125]    [Pg.2882]    [Pg.202]    [Pg.324]    [Pg.144]    [Pg.146]    [Pg.133]    [Pg.394]    [Pg.354]    [Pg.507]    [Pg.115]    [Pg.332]    [Pg.172]   


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