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Single rate-determining modes

Ultimately, it is seen that pure kinetic modes (with only a single rate determining step) make it possible to explain the laws that we called single laws in section 15.2.1.2. They do not give any explanation for the paralinear law and the con lete parabolic law. [Pg.577]

We saw that the pure modes with a single rate determining step, if they made it possible to explain a certain number of laws, did not cover all of them, in particular the paralinear law and the complete parabolic law (see section 15.2.1.2). From this the idea to complex the solutions utilizing mixed modes in which the kinetics is governed by two rate determining steps, others being constantly at equilibrium. [Pg.578]

We will solve the mechanisms by adopting the approach of the prevalent Wagner defect and considering only pure modes with only a single rate determining step. The experimental conditions are in general far from equilibrium and we will not have to take into accounts the reverse reaction of the rate determining step. [Pg.597]

It was shown that the mode was a pseudo-steady state one and tliat there was only a single rate-determining step. [Pg.714]

Sinee the system is, according to the preeeding question, in a pseudo-steady state mode, it means that one has a pine mode with only a single rate-determining step or a mixed mode with several rate-determining steps taking place in zones of same sizes (same spaee function). We will thus have three rate-limiting zones ... [Pg.772]

We assume now that we are within the framework of pseudo-steady step modes with a single rate-determining step. This step can be one of the two steps that produces the vacancies or a condensation step, for example, the one leading to the... [Pg.823]

The simplest method for the mathematical formulation of such a mode is the following and it is based on the one that has been used for pure modes with a single rate-determining step. [Pg.185]

Modes with a single rate-determining step... [Pg.210]

The rate coefficients of one of the elementaiy steps of the growth reaction are much lower than the other steps (approximation of a pseudo-steady state mode with a single rate-determining step). [Pg.358]

Finally, the applieation of the same relation [14.3] limits us to growth modeling considering pseudo-steady state modes and a single rate-determining step. [Pg.386]

It was pointed out in Section 4.2 that most polyatomic molecules show only a single relaxation process, owing to rapid intramolecular vibration-vibration transfer between modes. This corresponds to a state of affairs where Vibrational energy enters the molecule via process (a), which is rate-determining,... [Pg.220]

Figure 1.7 Chromatogram of iodate and iodide in seawater by nonsuppressed 1C with inductively coupled plasma mass spectrometric detection. The main speoiation of iodine in seawater, iodate (IO3) and iodide (l ), could be determined simultaneously. Conditions column, Agilent G3154A/101 (150 X 4.6 mm inner diameter) column temperature = 20°C injection volume = 10(il mobile phase, 20.0mmol 1 of NH4NO3 at pH 5.6 flow rate = 1.0ml min The ICP-MS conditions flow rate of plasma gas (Ar) = 151 min flow rate of auxiliary gas (Ar) = 1.01- min flow rate of oarrier gas (Ar) = 1.151- min sampling depth = 7.5mm integration time = 1 s dwell time = 0.5s. The 2 1 was seleoted for deteotion by single-ion monitoring mode. Reprinted from Chen etal., (2007) with permission from Elsevier. Figure 1.7 Chromatogram of iodate and iodide in seawater by nonsuppressed 1C with inductively coupled plasma mass spectrometric detection. The main speoiation of iodine in seawater, iodate (IO3) and iodide (l ), could be determined simultaneously. Conditions column, Agilent G3154A/101 (150 X 4.6 mm inner diameter) column temperature = 20°C injection volume = 10(il mobile phase, 20.0mmol 1 of NH4NO3 at pH 5.6 flow rate = 1.0ml min The ICP-MS conditions flow rate of plasma gas (Ar) = 151 min flow rate of auxiliary gas (Ar) = 1.01- min flow rate of oarrier gas (Ar) = 1.151- min sampling depth = 7.5mm integration time = 1 s dwell time = 0.5s. The 2 1 was seleoted for deteotion by single-ion monitoring mode. Reprinted from Chen etal., (2007) with permission from Elsevier.
The fourth-order dependence of this rate on is to be expected from the appearance of a single time derivative along with four spatial derivatives in eqn [17]. This relaxation rate determines, among other things, the couelation time for the fluctuating bending modes. Spedfically, in the absence of an applied tension. [Pg.195]

First, study the two modes with steps [19.EG.1] and [19.EG.2], respeetively, as the rate-determining step. All the steps of condensation can be in both cases merged in only a single reaction [19.EG.3] at equiUbrium such as... [Pg.832]


See other pages where Single rate-determining modes is mentioned: [Pg.153]    [Pg.272]    [Pg.28]    [Pg.429]    [Pg.208]    [Pg.948]    [Pg.133]    [Pg.153]    [Pg.186]    [Pg.226]    [Pg.272]    [Pg.83]    [Pg.281]    [Pg.583]    [Pg.239]    [Pg.109]    [Pg.333]    [Pg.213]    [Pg.86]    [Pg.11]    [Pg.397]    [Pg.323]    [Pg.245]    [Pg.881]    [Pg.8293]    [Pg.376]    [Pg.239]    [Pg.293]    [Pg.348]    [Pg.860]    [Pg.198]    [Pg.165]    [Pg.1540]    [Pg.1]   
See also in sourсe #XX -- [ Pg.210 ]




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