Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Decay rate constant function

Figure 5. The areal exhalation rate from the porous sample in Figure 2, enclosed in three different exhalation cans. Two of them ( a1 and 0 ) are completely radon-tight and the third Cb1) has a radon leak rate constant v, numerically equal to the radon decay rate constant (v=A= 2.1 10" s" ). The cans are closed at time zero. The radon exhalation evolution as a function of time is discussed in the text (theory). Figure 5. The areal exhalation rate from the porous sample in Figure 2, enclosed in three different exhalation cans. Two of them ( a1 and 0 ) are completely radon-tight and the third Cb1) has a radon leak rate constant v, numerically equal to the radon decay rate constant (v=A= 2.1 10" s" ). The cans are closed at time zero. The radon exhalation evolution as a function of time is discussed in the text (theory).
The electron-spin time-correlation functions of Eq. (56) were evaluated numerically by constructing an ensemble of trajectories containing the time dependence of the spin operators and spatial functions, in a manner independent of the validity of the Redfield limit for the rotational modulation of the static ZFS. Before inserting thus obtained electron-spin time-correlation functions into an equation closely related to Eq. (38), Abernathy and Sharp also discussed the effect of distortional/vibrational processes on the electron spin relaxation. They suggested that the electron spin relaxation could be described in terms of simple exponential decay rate constant Ts, expressed as a sum of a rotational and a distortional contribution ... [Pg.85]

It is found that carotenoids with carbonyl functional groups increase the triplet decay rate constants of the porphyrins TPP or TPPS in frozen toluene/ethanol glasses possibly by triplet-triplet transfer. The triplet-triplet transfer could be facilitated by the presence of hydrogen bonding between carotenoids containing carbonyl groups and the prophyrins. Carotenoids with no polar functional groups like 3 Totene do not interact with porphyrin so as to affect the triplet life time of the latter. [Pg.138]

Figure 1 Transient absorption spectra of c-S and t-S (S = r -4 ) recorded at time t after eT during PR of c-S and t-S (S = 1-4) with [S] = 5.0 x 10 M in DCE at r.t. Insets kinetic traces illustrating the time profiles of the D2 band at 1 as a function of t. Both t and the observed decay rate constant (kobs) and are mentioned in the figure. Figure 1 Transient absorption spectra of c-S and t-S (S = r -4 ) recorded at time t after eT during PR of c-S and t-S (S = 1-4) with [S] = 5.0 x 10 M in DCE at r.t. Insets kinetic traces illustrating the time profiles of the D2 band at 1 as a function of t. Both t and the observed decay rate constant (kobs) and are mentioned in the figure.
FIGURE 5.10 Plots of ozone pseudo-first-order decay rate constant as a function of the o-cresol concentration using U.S. EPA protocol for determining 03 rate constants (adapted from Pitts et al., 1981). [Pg.149]

Thus we have an explicit formula in this case for the Hopf bifurcation points as a function of the decay rate constant for k2 = 20, Tres = 39.25 for k2 = Tres = 163.2. Figure 8.5 shows how the bifurcation point moves to longer residence times as k2 decreases, along with the locations of the extinction points t s from eqn (8.27). [Pg.224]

Figure 5. Hydrogen peroxide decay rate constants in surface-water samples from Sharpes Bay (in June and September), Jacks Lake, Ontario, Canada, from the East (Station 23), Central (Station 84), and West Basin (Station 357) of Lake Erie and the Chesapeake Bay, plotted as a function of bacteria... Figure 5. Hydrogen peroxide decay rate constants in surface-water samples from Sharpes Bay (in June and September), Jacks Lake, Ontario, Canada, from the East (Station 23), Central (Station 84), and West Basin (Station 357) of Lake Erie and the Chesapeake Bay, plotted as a function of bacteria...
Figure 147 The relative cascade-like pattern of the increase of triplet exciton monomolecular decay rate constant (/ = t 1) as a function of charge-injecting voltage in anthracene crystal. Consecutive trap-filled limits are indicated by C/TFL (1), /TFL(2) and C/TFL (3). Dotted line indicates the averaged (linear) dependence of A/ // 0 as resulted from the standard interpretation assuming a continuous increase in the charge density proportional to the injecting voltage [334]. Adapted from Ref. 240. Figure 147 The relative cascade-like pattern of the increase of triplet exciton monomolecular decay rate constant (/ = t 1) as a function of charge-injecting voltage in anthracene crystal. Consecutive trap-filled limits are indicated by C/TFL (1), /TFL(2) and C/TFL (3). Dotted line indicates the averaged (linear) dependence of A/ // 0 as resulted from the standard interpretation assuming a continuous increase in the charge density proportional to the injecting voltage [334]. Adapted from Ref. 240.
In the absence of a magnetic field, the radical pair decay can be represented by a single exponential function as shown by Eq. (7-6). Here, the decay rate constant is given by ko-From Eq. (7-8), the feo value should show no MCE. This prediction explains well results (4) shown in Section 7.1. [Pg.102]

Fig. 24.2. Single-molecule recording of T4 lysozyme conformational motions and enzymatic reaction turnovers of hydrolysis of an E. coli B cell wall in real time, (a) This panel shows a pair of trajectories from a fluorescence donor tetramethyl-rhodamine blue) and acceptor Texas Red (red) pair in a single-T4 lysozyme in the presence of E. coli cells of 2.5mg/mL at pH 7.2 buffer. Anticorrelated fluctuation features are evident. (b) The correlation functions (C (t)) of donor ( A/a (0) Aid (f)), blue), acceptor ((A/a (0) A/a (t)), red), and donor-acceptor cross-correlation function ((A/d (0) A/d (t)), black), deduced from the single-molecule trajectories in (a). They are fitted with the same decay rate constant of 180 40s. A long decay component of 10 2s is also evident in each autocorrelation function. The first data point (not shown) of each correlation function contains the contribution from the measurement noise and fluctuations faster than the time resolution. The correlation functions are normalized, and the (A/a (0) A/a (t)) is presented with a shift on the y axis to enhance the view, (c) A pair of fluorescence trajectories from a donor (blue) and acceptor (red) pair in a T4 lysozyme protein without substrates present. The acceptor was photo-bleached at about 8.5 s. (d) The correlation functions (C(t)) of donor ((A/d (0) A/d (t)), blue), acceptor ((A/a (0) A/a (t)), red) derived from the trajectories in (c). The autocorrelation function only shows a spike at t = 0 and drops to zero at t > 0, which indicates that only uncorrelated measurement noise and fluctuation faster than the time resolution recorded (Adapted with permission from [12]. Copyright 2003 American Chemical Society)... Fig. 24.2. Single-molecule recording of T4 lysozyme conformational motions and enzymatic reaction turnovers of hydrolysis of an E. coli B cell wall in real time, (a) This panel shows a pair of trajectories from a fluorescence donor tetramethyl-rhodamine blue) and acceptor Texas Red (red) pair in a single-T4 lysozyme in the presence of E. coli cells of 2.5mg/mL at pH 7.2 buffer. Anticorrelated fluctuation features are evident. (b) The correlation functions (C (t)) of donor ( A/a (0) Aid (f)), blue), acceptor ((A/a (0) A/a (t)), red), and donor-acceptor cross-correlation function ((A/d (0) A/d (t)), black), deduced from the single-molecule trajectories in (a). They are fitted with the same decay rate constant of 180 40s. A long decay component of 10 2s is also evident in each autocorrelation function. The first data point (not shown) of each correlation function contains the contribution from the measurement noise and fluctuations faster than the time resolution. The correlation functions are normalized, and the (A/a (0) A/a (t)) is presented with a shift on the y axis to enhance the view, (c) A pair of fluorescence trajectories from a donor (blue) and acceptor (red) pair in a T4 lysozyme protein without substrates present. The acceptor was photo-bleached at about 8.5 s. (d) The correlation functions (C(t)) of donor ((A/d (0) A/d (t)), blue), acceptor ((A/a (0) A/a (t)), red) derived from the trajectories in (c). The autocorrelation function only shows a spike at t = 0 and drops to zero at t > 0, which indicates that only uncorrelated measurement noise and fluctuation faster than the time resolution recorded (Adapted with permission from [12]. Copyright 2003 American Chemical Society)...
Figure 5 (a) The structure of T4 lysozyme with the two dye labels schematically shown, (b) Fluorescence intensity trajectories of the TM R donor (blue) and the Texas Red acceptor (red) of a single T4 lysozyme in the presence of E coli B cell wall, (c) Distribution of the decay rate constants (/t) of the donor intensity autocorrelation functions. Reproduced with permission from Y. Chen D. Hu E. R. Vorpagel H. P. Lu, J. Phys. Chem. B. 2003,107, 7947-7956. Copyright (2003) American... [Pg.761]

In the absence of extraneous spin relaxation effects, the decay of a radical signal is attributed to chemical reaction. Since the muon in a radical is usually at a site remote from the reaction center, it functions merely as a tracer. This is potentially a very valuable application of ftSR to the field of chemical kinetics, since it is very difficult to accurately determine radical rate constants by other means. A pilot study has demonstrated the feasibility of such a determination, using radical line widths from Fourier transform spectra to measure decay rates as functions of the concentration of an added substrate.26... [Pg.374]

Figure 4 Total decay rate constants of internal energy-selected benzene cations C6D5H and C6D6 as a function of their internal energy. Figure 4 Total decay rate constants of internal energy-selected benzene cations C6D5H and C6D6 as a function of their internal energy.
Because the shape of the fall-off curve (which we can calculate quite well) is determined directly by the dispersion of the function it would seem that we can safely assume the Boltzmann averaged decay rate constant to be known and, therefore, that the observed centre of the fall-off defines the effective relaxation rate constant r<. If, for the moment, we accept that the relaxation rate constant is about the same for all reactant molecules, the conclusion from Section 5.7 that the simpler the molecule, the larger is the numerical magnitude of the k E) function, immediately places any set of fall-off curves in the correct sequence, as found in Figure... [Pg.111]

Fig. 4.32 Entropy change (ASa) associated with excitation of an absorber as a function of the excitation rate constant (k = J/(v)cr(v)dv), with the decay rate constant kg fixed at either 10 ° dashed curve) or 10 s solid curve). The entropy is expressed relative to hvjT for absorption at 500 nm (/iv = 2.48 eV = 3.98 x 10 J) and T= 300 K. Possible contributions from degeneracy of the excited state (/15 ) are neglected. The values of kg were chosen on the assumption that the excited absorber enters into a productive non-radiative reaction with a rate constant k that is on the order of 100 times greater than typical values of the rate constant for fluorescence (fc/), as is necessary for efficient photochemistry. To put the abscissa scale in perspective, consider excitation in an absorption band at 500 nm with a mean extinction coefficient of 10 M cm , which is equivalent to a mean absorption cross section of 3.82 x 10 cm. Suppose the absorber is exposed to full sunlight, which has an irradiance at 500 mn of approximately 1.35 W nm at the earth s surface, assuming a clear atomosphere and a solar zenith angle of 60°. If the absorption band has a width of 10 run, the total irradiance is 1.35 x 10 J cm s ot 3.40 X 10 photons cm s, giving 1.30 excitations per second, AS = 2.16 x lO eVK, ... Fig. 4.32 Entropy change (ASa) associated with excitation of an absorber as a function of the excitation rate constant (k = J/(v)cr(v)dv), with the decay rate constant kg fixed at either 10 ° dashed curve) or 10 s solid curve). The entropy is expressed relative to hvjT for absorption at 500 nm (/iv = 2.48 eV = 3.98 x 10 J) and T= 300 K. Possible contributions from degeneracy of the excited state (/15 ) are neglected. The values of kg were chosen on the assumption that the excited absorber enters into a productive non-radiative reaction with a rate constant k that is on the order of 100 times greater than typical values of the rate constant for fluorescence (fc/), as is necessary for efficient photochemistry. To put the abscissa scale in perspective, consider excitation in an absorption band at 500 nm with a mean extinction coefficient of 10 M cm , which is equivalent to a mean absorption cross section of 3.82 x 10 cm. Suppose the absorber is exposed to full sunlight, which has an irradiance at 500 mn of approximately 1.35 W nm at the earth s surface, assuming a clear atomosphere and a solar zenith angle of 60°. If the absorption band has a width of 10 run, the total irradiance is 1.35 x 10 J cm s ot 3.40 X 10 photons cm s, giving 1.30 excitations per second, AS = 2.16 x lO eVK, ...
Since the decay is associated with passing through the barrier, the quantity a t) is nothing but the step function a = Q[x — x). Differentiating (3.93) and finally setting r = 0 one obtains [Chandler 1987] the expression for the rate constant. [Pg.56]

Another useful technique for measuring the rates of certain reactions involves measuring the quantum yield as a function of quencher concentration. A plot of the inverse of the quantum yield versus quencher concentration is then made Stern-Volmer plot). Because the quantum yield indicates the fraction of excited molecules that go on to product, it is a function of the rates of the processes that result in other fates for the excited molecule. These processes are described by the rate constants (quenching) and k (other nonproductive decay to ground state). [Pg.747]

From this expression, it is obvious that the rate is proportional to the concentration of A, and k is the proportionality constant, or rate constant, k has the units of (time) usually sec is a function of [A] to the first power, or, in the terminology of kinetics, v is first-order with respect to A. For an elementary reaction, the order for any reactant is given by its exponent in the rate equation. The number of molecules that must simultaneously interact is defined as the molecularity of the reaction. Thus, the simple elementary reaction of A P is a first-order reaction. Figure 14.4 portrays the course of a first-order reaction as a function of time. The rate of decay of a radioactive isotope, like or is a first-order reaction, as is an intramolecular rearrangement, such as A P. Both are unimolecular reactions (the molecularity equals 1). [Pg.432]


See other pages where Decay rate constant function is mentioned: [Pg.153]    [Pg.90]    [Pg.128]    [Pg.132]    [Pg.163]    [Pg.367]    [Pg.291]    [Pg.370]    [Pg.91]    [Pg.45]    [Pg.3253]    [Pg.479]    [Pg.98]    [Pg.82]    [Pg.260]    [Pg.269]    [Pg.225]    [Pg.31]    [Pg.370]    [Pg.82]    [Pg.316]    [Pg.299]    [Pg.475]    [Pg.183]    [Pg.141]    [Pg.206]    [Pg.56]    [Pg.133]   


SEARCH



Decay constant

Decay rate constant

Rating function

© 2024 chempedia.info