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Time Interval Adaptation

There are some simpler strategies that might do, and are easier to program. If an experiment such as double pulse or square wave voltammetry is simulated, the sharp changes occur at predictable times, and simple sequences of time intervals, such as exponentially expanding intervals, can be satisfactory, repeating the sequence at the onset of each pulse. [Pg.117]

If there are unpredictable changes, the answer might be to use a professional package that is, either a simulation package (see Chap. 17), or the method of lines (Chap. 9) and a professional routine for solving the resulting set of odes, making use of the adaptive time intervals feature, which these routines normally offer. [Pg.139]

Noye J (1982) Finite difference methods for partial differential equations. In Noye J (ed) Proceedings of the 1981 conference on the numerical solution of partial differential equations, Queen s College, Melbourne, Australia. North Holland, Amsterdam, pp 3-137 [Pg.140]

Hunter 1C, Jones IP (1981) Numerical experiments on the effects of strong grid stretching in finite difference calculations. Technical Report AERE R-10301, United Kingdom Atomic Energy Authority, Harwell [Pg.140]

Crowder HJ, Dalton C (1971) Errors in the use of nonuniform mesh systems. J Comput Phys [Pg.140]


Fig. 1. Association and dissociation plots for ethylene binding to 6-day-old pea epicotyls. The association plot ( ) was produced by incubating 10 g F.W. of pea epicotyls in 40 nl P C-ethylene 20 p.1 P C-ethylene for various time intervals. The dissociation plots were produced by incubation in 31 or 34 nl P C-ethylene 20 pi P C-ethylene for 1 ( ) or 20 ( ) hours, respectively, before the introduction of 20 pi P C-ethylene (indicated by arrows). Binding of C-ethylene was then measured after various time intervals. Adapted from Sanders et al. [21]. Fig. 1. Association and dissociation plots for ethylene binding to 6-day-old pea epicotyls. The association plot ( ) was produced by incubating 10 g F.W. of pea epicotyls in 40 nl P C-ethylene 20 p.1 P C-ethylene for various time intervals. The dissociation plots were produced by incubation in 31 or 34 nl P C-ethylene 20 pi P C-ethylene for 1 ( ) or 20 ( ) hours, respectively, before the introduction of 20 pi P C-ethylene (indicated by arrows). Binding of C-ethylene was then measured after various time intervals. Adapted from Sanders et al. [21].
Figure Cl.5.8. Spectral jumping of a single molecule of terrylene in polyethylene at 1.5 K. The upper trace displays fluorescence excitation spectra of tire same single molecule taken over two different 20 s time intervals, showing tire same molecule absorbing at two distinctly different frequencies. The lower panel plots tire peak frequency in tire fluorescence excitation spectmm as a function of time over a 40 min trajectory. The molecule undergoes discrete jumps among four (briefly five) different resonant frequencies during tliis time period. Arrows represent scans during which tire molecule had jumped entirely outside tire 10 GHz scan window. Adapted from... Figure Cl.5.8. Spectral jumping of a single molecule of terrylene in polyethylene at 1.5 K. The upper trace displays fluorescence excitation spectra of tire same single molecule taken over two different 20 s time intervals, showing tire same molecule absorbing at two distinctly different frequencies. The lower panel plots tire peak frequency in tire fluorescence excitation spectmm as a function of time over a 40 min trajectory. The molecule undergoes discrete jumps among four (briefly five) different resonant frequencies during tliis time period. Arrows represent scans during which tire molecule had jumped entirely outside tire 10 GHz scan window. Adapted from...
Prior to the degradation of many organic compounds, a period is noted in which no destruction of the compound is evident. This time interval is designated as an acclimation period or, sometimes, an adaptation or lag period [93-98]. It may be defined as the length of time between the addition or entry of the compound into an environment and evidence of its detectable loss. During this interval, no change in concentration is noted, but then the disappearance becomes evident and the rate of destruction often becomes rapid. [Pg.340]

FIGURE 8.12 Percentage of S02 converted to sulfate after a time interval At in small haze particles, fogs, and clouds as a function of the aqueous reaction volume note that the time intervals for each one are different, reflecting how long they typically last in the atmosphere (adapted from Lamb et al., 1987). [Pg.310]

Figure 12.12 Images of the motility of the actin/Au-wire/actin filaments on a glass surface modified with myosin, upon the addition of ATP. Images were recorded by reflectance microscopy (a), (b), (c), and (d) correspond to the same imaged frame at time intervals of 5 s. Adapted with permission from Ref. 56. Copyright Nature Publishing Group, 2004. Figure 12.12 Images of the motility of the actin/Au-wire/actin filaments on a glass surface modified with myosin, upon the addition of ATP. Images were recorded by reflectance microscopy (a), (b), (c), and (d) correspond to the same imaged frame at time intervals of 5 s. Adapted with permission from Ref. 56. Copyright Nature Publishing Group, 2004.
Fig. 26. STM images of the oxygen pre-covered platinum(l 1 1) surface during reaction with hydrogen. Images were recorded at a temperature of T = 111 K with a time interval of 625 K. The white ring in the upper right corner is associated with a reaction front of OH intermediates from the autocatalytic reaction. The outside is characterized by an oxygen-terminated surface, whereas water molecules from the reaction are identified inside the ring. Adapted with permission from Reference (757). Fig. 26. STM images of the oxygen pre-covered platinum(l 1 1) surface during reaction with hydrogen. Images were recorded at a temperature of T = 111 K with a time interval of 625 K. The white ring in the upper right corner is associated with a reaction front of OH intermediates from the autocatalytic reaction. The outside is characterized by an oxygen-terminated surface, whereas water molecules from the reaction are identified inside the ring. Adapted with permission from Reference (757).
Another CE separation method that has been adapted to on-line NMR detection for trace level separations is capillary isotachophoresis [22]. In this case, after the separation, the analyte bands are slowly moved through the capillary until they lie directly within the coil. Precise positioning of the analyte bands in the NMR detection coil can be difficult. A recent enhancement is the use of several NMR detection coils on a single separation capillary [23], In this way, the first coil acts as a scout coil and is optimized for sensitivity (not necessarily linewidth) to locate the analyte band as it moves through the coil. After an analyte band is detected, the flow is stopped after the appropriate time-interval so that the analyte bands are now located in the second coil, which is used to acquire high-resolution NMR spectra. [Pg.276]

When these requirements are met, the intensity Iexp(Ekin, pass = fUsp) of a photoline with nominal energy °in, obtained by scanning the spectrometer voltage Usp in equal steps and for equal time intervals across the adapted value U°p follows from equ. (2.30) to be... [Pg.67]

Changes in the atmospheric fields happen on different time scales and with different speed. Therefore, we adapt the time intervals for writing the model results (that are the forcing data for nested simulations) to the time scales, in which the atmospheric fields change, instead of using short but constant time intervals. If significant changes happen on short time scales, the results should be written more often than for more or less steady conditions. [Pg.202]

Fig. 5.4.4 Pulsed-field gradient NMR. (a) The Hahn echo is attenuated by translational diffusion during the time interval A between two short gradient pulses applied in the dephasing and in the rephasing periods of the echo (top). By use of flie gradient pulses initial position T and final position Tj of the magnetization are labelled to identify migrating magnetization components (bottom), (b) The sensitivity of the method towards slower processes can be increased if the stimulated echo is used in place of the Hahn echo. Adapted from [Cal2] with permission from Oxford University Press. Fig. 5.4.4 Pulsed-field gradient NMR. (a) The Hahn echo is attenuated by translational diffusion during the time interval A between two short gradient pulses applied in the dephasing and in the rephasing periods of the echo (top). By use of flie gradient pulses initial position T and final position Tj of the magnetization are labelled to identify migrating magnetization components (bottom), (b) The sensitivity of the method towards slower processes can be increased if the stimulated echo is used in place of the Hahn echo. Adapted from [Cal2] with permission from Oxford University Press.
Given that producers and consumers have already adapted so as to minimize their prospective losses, or to maximize their prospective gains. Figure 2 depicts for a predetermined time interval one example of the changes an air pollution increase can have upon consumer surplus and producer quasi-rent. The air pollution increase reduces the desirable properties of the output, making smaller the consumer s w llingijiess-to-pay and causing his demand... [Pg.373]


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