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Modulation parameters selection

From a technical point of view, intensity-modulated radiation therapy (IMRT) optimizes several parameters selection of multiple beams and, for each beam, optimization of dose, dose rate, size and shape, etc. Tomotherapy optimizes the dose distribution by IMRT in successive sections with immediate verification gamma knife, cyberknife, and radiosurgery concentrate high radiation doses in well-defined small volumes. [Pg.746]

Figure 6 Effect of volume of distribution (Vd) on pulmonary (upper line) and systemic (lower line) receptor occupancies. Simulations, A, B, and C are shown for increasing Vd values of 150, 400, and 1500L, respectively, whereas the other parameters, such as clearance and dose, remain unchanged. An increase in Vd (100-1500L) produces only a slight increase in the difference (AUC pulmonary-AUC systemic) between pulmonary and systemic receptor occupancies, thus indicating that Vd does not seem to be that significant in modulating pulmonary selectivity. As a result, drugs with similar clearance but different half-lives due to differences in Vd will produce approximately equivalent degrees of pulmonary and systemic effects. Figure 6 Effect of volume of distribution (Vd) on pulmonary (upper line) and systemic (lower line) receptor occupancies. Simulations, A, B, and C are shown for increasing Vd values of 150, 400, and 1500L, respectively, whereas the other parameters, such as clearance and dose, remain unchanged. An increase in Vd (100-1500L) produces only a slight increase in the difference (AUC pulmonary-AUC systemic) between pulmonary and systemic receptor occupancies, thus indicating that Vd does not seem to be that significant in modulating pulmonary selectivity. As a result, drugs with similar clearance but different half-lives due to differences in Vd will produce approximately equivalent degrees of pulmonary and systemic effects.
Using the configuration file ch5612.cfg open the parameter optimizer (Utiiities I Optimize parameter), select the options Show resuit as 1D series, N 6, Step 10, Seiected optimized parameter d3, d3 0.002 and in3 0.2m in the dialog boxes and start the calculation for the ID HETCOR experiment. To compare the intensity modulation for each type of CHp group, change the multiplicity factor in the spin system for proton b from 3 to 2 to 1. [Pg.324]

The Beam Calculator Module generates the instrument beam as a function of the FTS and interferometric input parameters selected by the user, and the telescope parameters. The first derived parameter required is the interferometric angular resolution, AOj. For an interferometer with a maximum baseline bmax, the maximum... [Pg.82]

After the candidate downstream gene modules are selected by GA, FSO is proposed to determine the parameters in the NN model. Particle swarm optimization is motivated by the behavior of bird flocking or fish blocking, originally intended to explore optimal or near-optimal solutions in sophisticated continuous spaces (Kennedy and Eberhart 1995). Its main difference from other evolutionary algorithms (e.g., GA) is that PSO relies on cooperation rather than competition. Good solutions in the problem set are shared with their less-fit ones so that the entire population improves. [Pg.227]

Module 6, Column Diagnosis (COLDIAG). This module uses chromatographic parameters such as efficiency, asymmetry, retention time, selectivity and operating pressure, to detect failures of the column or other chromatographic hardware. Table II lists the types of column failure which the module can currently handle. Note that the module will also correctly diagnose some problems which are NOT column malfunctions but which might be interpreted as such by a user. [Pg.292]

Expansion of Module 3 to include rules for selection of detectors and detector parameters. The rules will handle optical absorbance and fluorescence (including pre- and post-column deri-vatization) and electrochemical detection. [Pg.293]

Eortunately, for most photon device photodetectors, the dependence on modulation frequency is fairly flat across most of the region likely to be encountered with conventional NIR analyzer technology. Provided the D is satisfactory at the required measurement wavelengths, it is one useful parameter for detector selection. [Pg.118]

Tie are also expected to be field-dependent. Their field dependence can be described by two parameters the electron relaxation time at low fields Tso, and the correlation time for the electron relaxation mechanism Ty (see Eq. (14) of Chapter 2) (5). However, Tso usually depends on (see Eq. (52) of Chapter 2). Therefore, it is preferable to select two different parameters for describing the field dependence of electron relaxation. For S > 1/2 systems, in case the electron relaxation is due to modulation of a time dependent transient zero-field splitting, A, (pseudorotational model), the Bloembergen-Morgan equations are obtained 5,6) ... [Pg.108]


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Parameters, selection

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