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Null cycle

These reactions would produce a net e /h recombination and, conse-quendy, net null cycles, decreasing the rate of degradation [37]. As for salicylic acid cited earlier, the formation of surface-adsorbed cation radicals was invoked to increase the charge-carrier recombination rate and thus lower the quantum yields for degradation [27]. Added redox reagents can also act as recombination sites, so that the overall photocatalytic rate could increase, decrease, or remain unchanged [40]. [Pg.218]

The products of reaction (2.2) recombining via reaction (2.20) to reform ozone. This form of cycle (2.24, 2.2, 2.89) is often referred to as a null cycle. The fraction of the XO tied up in null cycles is ineffective as a... [Pg.60]

The most important reaction in the initiation of smog formation is the production of ozone, a strong oxidant generated through the N02 photodissociation cycle known as the null cycle. ... [Pg.176]

Thus, the sequence of these two reactions is a null cycle with no net chemical effect. [Pg.233]

This ultimately leads to the regeneration of ozone by the three-body reaction (R2), resulting in another null cycle. Occasionally, however, 0( D) collides with water to generate two hydroxyl radicals ... [Pg.234]

As a result, if a molecule of HO2 reacts with NO before it has a chance to react with either O or 03, the result is a do-nothing (null) cycle with respect to removal of O3. Each time a molecule of H02 follows the bottom path and reacts with O or 03, two molecules of odd oxygen are removed ... [Pg.159]

Because the O atom rapidly reforms 03, this is a null cycle with respect to 03 removal. The rate of net 03 removal by the CIO, cycle of reactions 1 and 2 is... [Pg.163]

Since the ground-state O atom then just reacts with 02 by reaction 2 to replenish 03, this path, consisting of reactions lb, 3, and 2, is just another null cycle. Occasionally, however, O D) collides with a water molecule and produces two OH radicals ... [Pg.206]

The photolysis rate by channel 4.24a is about eight times that for channel 4.24b. The second channel 4.24b is that which leads to an overall loss of odd oxygen and is the one involved in the above cycle. In addition to these there is the null cycle ... [Pg.176]

Null cycles can also result from the coupling of species from the catalytic cycles ... [Pg.183]

Photolysis of NO2, which completes each of these null cycles, competes with reaction 4.22,... [Pg.183]

When the both sides of the equations are summed up, they are cleared to leave nothing, which means nothing happens. This kind of chain reaction is called null cycle , where null means zero in German. In the null cycle neither net production nor destruction of ozone occurs. Furthermore in the lower stratosphere, the reactions. ... [Pg.394]

Lemma 4 If N is a multiple of 3, there are exactly four distinct fixed points (i.e. cycles of length one) otherwise, only the null configuration is a fixed point. [Pg.241]

Proof We prove this statement by showing that all trees rooted on cycles are equal to the tree rooted on the null configuration. Let A(x) represent the configuration that evolves into the null state after exactly t iterations i.e. T x)YA x) = 0 mod x — 1). Let R x) and be two states on the same cycle so that... [Pg.241]

The previous discussion has shown us how to calculate the total number of possible cyclic states. We also know, from Lemma 2, that all cycle lengths must divide the maximal cycle length Hiv obtain the exact number of distinct cycles and their lengths takes a little bit more work. If flw prime, we know that the only possible cyclic lengths are 1 and It can then be shown that only the null configuration is a fixed point unless N is some multiple of 3, it which case there are exactly four distinct cycles of length one. If Hat i ot prime, there can exist as many cycles as there are divisors of Although there is no currently known closed form... [Pg.242]

Here we are interested in escape out of the domain L specified by a single cycle of the potential that is out of a domain of length n that is the domain of the well. Because the bistable potential of Eq. (5.42) has a maximum at x = n/2 and minima at x = 0, x = 7t, it will be convenient to take our domain as the interval —7t/2 < x < n/2. Thus we will impose absorbing boundaries at x = —n/2, x = n/2. Next we shall impose a second condition that all particles are initially located at the bottom of the potential well so that x0 = 0. The first boundary condition (absorbing barriers at —n/2, n/2) implies that only odd terms in p in the Fourier series will contribute to Y (x). While the second ensures that only the cosine terms in the series will contribute because there is a null set of initial values for the sine terms. Hence... [Pg.388]

Fig. 7. MR detection of ultrasonic waves oscillating at 515 kHz. (a) Phase image of a phantom without insonation. (b) Phase image with 40 W peak power insonation. In the NMR sequence 50,000 cycles of synchronized sine-shaped motion-sensitizing gradient were applied. Arrows indicate the null-gradient positions of the dedicated gradient coil system. Wavelength is around 2.9 mm and peak matter displacement is around 120 nm. From Ref. 30, reprinted by permission of Wiley-Liss, Inc., a subsidiary of John Wiley Sons, Inc. Fig. 7. MR detection of ultrasonic waves oscillating at 515 kHz. (a) Phase image of a phantom without insonation. (b) Phase image with 40 W peak power insonation. In the NMR sequence 50,000 cycles of synchronized sine-shaped motion-sensitizing gradient were applied. Arrows indicate the null-gradient positions of the dedicated gradient coil system. Wavelength is around 2.9 mm and peak matter displacement is around 120 nm. From Ref. 30, reprinted by permission of Wiley-Liss, Inc., a subsidiary of John Wiley Sons, Inc.
An autoregressive time series model (16) seems to be less suitable for cumulative distribution data. This technique is primarily designed for finding trends and/or cycles for data recorded in a time sequence, under the null-hypothesis that the sequence has no effect. [Pg.275]

The classical cure 131,132), apart from special probe construction precautions, is a pulse sequence using a phase device detection cycle in which one exploits the fact that acoustic ringing increases linearly with pulse width while NMR signal follows the sinusoidal nutation-angle curve. In its most elementary form, the cycle is composed of four steps (ideally with null 5) ... [Pg.460]

The same logic can be applied in multidimensional spectroscopy, to decrease -noise in favourable cases -noise can be reduced by an order of magnitude, allowing weak cross-peaks to be detected [9]. The 2D experiments for which -noise poses the greatest problem are those which require strong signals to be nulled, either by phase cycling or by the use... [Pg.309]


See other pages where Null cycle is mentioned: [Pg.349]    [Pg.144]    [Pg.206]    [Pg.183]    [Pg.246]    [Pg.533]    [Pg.533]    [Pg.396]    [Pg.400]    [Pg.349]    [Pg.144]    [Pg.206]    [Pg.183]    [Pg.246]    [Pg.533]    [Pg.533]    [Pg.396]    [Pg.400]    [Pg.227]    [Pg.242]    [Pg.93]    [Pg.16]    [Pg.136]    [Pg.73]    [Pg.327]    [Pg.233]    [Pg.111]    [Pg.34]    [Pg.80]    [Pg.131]    [Pg.184]    [Pg.238]    [Pg.239]    [Pg.240]    [Pg.257]   
See also in sourсe #XX -- [ Pg.176 ]

See also in sourсe #XX -- [ Pg.394 , Pg.396 , Pg.400 ]




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