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Balanced samples

As the number of conformations increases exponentially with the number of rotatable bonds, for most molecules it is not feasible to take all possible conformations into account. However, a balanced sampling of the conformational space should be ensured if only subsets arc being considered. In order to restrict the number of geometries output, while retaining a maximum of conformational diversity, ROTATE offers the possibility of classifying the remaining conformations, i.c., similar conformations can be combined into classes. The classification is based on the RMS deviation between the conformations, either in Cartesian (RMS y 7if [A]) or torsion space in [ ], The RMS threshold, which decides whether two... [Pg.111]

Similarly to LEAP1, the top 20 similar molecules per reaction component list are used, as a default setting, to ensure balanced sampling of reactants for each reaction component and the reasonable performance. This is user adjustable. [Pg.263]

The reference test was performed using the standard ASTM method for determining grain loadings to electrostatic precipitators. This test was used to verify the adequacy of the number of samples secured for mass balance calculations. Comparison of grain loading calculations using TVA standard probes and ORNL fabricated probes show that the mass balance samples are representative. [Pg.186]

It is assumed for the remainder of this entry that the same number of units is tested from each of the sampled locations (i.e., it is a balanced sampling plan). Regardless of what sampling plan is used to determine testing, multiple units are normally collected at each of the sample locations during validation to serve as contingency samples for possible later testing. [Pg.701]

Undecane was added as an internal standard to follow the reaction kinetics and to calculate the mass balance. Samples were taken periodically and analysed by gas chromatography in order to quantify conversion and selectivity of the reaction. In all reactions presented here, a ratio of 1 mol dodecene to 10 mol of benzene was used. [Pg.243]

The DSC data were obtained with a Du Pont cell base and a Model 990 thermal analyzer. An aluminum pan containing the sample was placed on the raised platform in the DSC cell, and an empty pan was placed on the reference platform. DSC scans for the samples were obtained from 150° to 600°C at a linear heating rate of 20°C/min. During the run, a slight flow of nitrogen was maintained. The TGA data was taken with a Du Pont 951 TGA balance in conjunction with a Model 990 thermal analyzer. A platinum boat containing the sample was suspended from the quartz beam of the balance. Samples were heated to 900°C at 20°C/min with a constant nitrogen flow. [Pg.344]

FIGURE 37.1 A Une plot of the effect of sample size and intersubject variability on the precision (expressed as percent mean absolute error—%MAE) with which central volume of distribution (VI) was estimated in a simulated population pharmacokinetic study in which a balanced sampling design was used. [Pg.929]

Got] Thermomagnetie balance, sample vibrating magnetometer teehniques Magnetic transition point saturation magnetic moment... [Pg.295]

The heart of this system is a pair of parallel, balanced sample support arms which oscillate freely around flexture pivots. Designed for low friction and precise balance, the natural frequency of the sample support system is less than 3 Hz, minimizing system contributions to damping. A schematic of this device is shown in Fig. 1. To make a measurement, a material of known dimensions is clamped between the two sample arms. The sample-arm-pivot system is oscillated at its resonant frequency by an electromechanical transducer. Frequency and amplitude of this oscillation are detected by a linear variable differential transformer (LVDT) positioned at the opposite end of the active arm. The LVDT provides a signal to an electromechanical transducer, which in turn keeps the sample oscillating at constant amplitude. [Pg.382]

Figure 4. Arrhenius plots of pure and supported La gSrQ 2Mn03. (LSM). Reactant gas composition 1% CH4, 4% O2, He (balance) sample weight 0.1 g, GHSV 135 000 h heating rate 10 K/min. Figure 4. Arrhenius plots of pure and supported La gSrQ 2Mn03. (LSM). Reactant gas composition 1% CH4, 4% O2, He (balance) sample weight 0.1 g, GHSV 135 000 h heating rate 10 K/min.
The mode of assembly of the components varies for example, the furnace might be above, below, or in line with the balance. Sample containers also vary widely in design cylindrical pans are common, typically 5-8 mm in diameter and 2-10 mm high, though flat plates and semisealed containers may be used to investigate the effects of atmospheric access to a sample. Compatibility between the construction materials and the system under investigation must be carefully considered. Materials commonly available include aluminum, platinum, alumina, and silica. Temperature indication is normally provided by a thermocouple located near the sample container. Because of inevitable thermal gradients within the apparatus, an indicated temperature can never be taken as an accurate reflection of the temperature of the sample. Reproducible location of the thermocouple is vital recommended calibration procedures have been described in [8]. Only in simultaneous TG-DTA instruments is direct measurement of the temperature possible. [Pg.829]

In a typical exanq, to prepare a stokhiometrically balanced sample of P (MDA/ MDiy, the evaporation temperatures of MDA and MDl were 100 C and TtfC, tespec tively. When the temperature of the substrate was room temperature, the deposition rate was about 1.8 pm/h and the pressure inside the chamber was about 3 X 10 Pa. [Pg.916]

Tkble 1 illustrates the results of elemental analysis of three as-deposited films at P (MDA/MDI) (12]. For these samples, the evaporation temperature of MDA was maintained at 100 C and the evaporation temperature of MDI was 6S C for the MDA-rich sample. 7(fC for the balanced sample, and 80 C far the MDI-rich sample. The ideal molecular structures supposed for these samples are given in Figure 7. [Pg.919]

Figure 8 Spiels the results (rf differential scanning calorimetry (DSQ for the three samples (12]. For the balanced sample, an exothermic peak U observed over 100 C for the first run of heating curve. The peak appears neither in the second run for the balanced sample nor in the first and second runs for the unbalanced samples. This exothermic peak for the balanced sample should represent the heat of polymerizalkm of oUgomers. Figure 8 Spiels the results (rf differential scanning calorimetry (DSQ for the three samples (12]. For the balanced sample, an exothermic peak U observed over 100 C for the first run of heating curve. The peak appears neither in the second run for the balanced sample nor in the first and second runs for the unbalanced samples. This exothermic peak for the balanced sample should represent the heat of polymerizalkm of oUgomers.
When the balanced samples are subjected to an electric field at elevated temperatores. a residual polarizatioo due to the dipolar orienutioo is produced, which leads to piezoelectric and pyroelectric activities. [Pg.921]


See other pages where Balanced samples is mentioned: [Pg.164]    [Pg.161]    [Pg.323]    [Pg.258]    [Pg.224]    [Pg.255]    [Pg.189]    [Pg.107]    [Pg.183]    [Pg.353]    [Pg.314]    [Pg.544]    [Pg.32]    [Pg.60]    [Pg.108]    [Pg.200]    [Pg.2048]    [Pg.2048]    [Pg.173]    [Pg.626]    [Pg.115]    [Pg.406]    [Pg.217]    [Pg.14]   
See also in sourсe #XX -- [ Pg.107 , Pg.155 ]




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