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Lambda parameter

Cellsim s universe consists of a 512 x 512 array. The program itself is completely menu-driven and includes these features (1) 256-state computed-function rules, in addition to lookup-tables, on both the Sun and CM (2) creation of look-up tables using Langton s lambda parameter (see section 3.2) (3) the ability to save images in Sun raster format and (4) the ability to generate lookup tables with standalone C code. Cellsim can be obtained via anonymous ftp on the Internet to think.com. [Pg.719]

In Section 2.5 the lambda parameter has been described, i.e., the dimensionless air-to-fuel ratio parameter that controls exhaust catalysis chemistry to a significant extent. [Pg.220]

Fig. 5. Lambda parameters that define the shape of current-voltage characteristics A is measured on a single filament and A on the composite (4675-NbTi filament composite of Fig. 2). Fig. 5. Lambda parameters that define the shape of current-voltage characteristics A is measured on a single filament and A on the composite (4675-NbTi filament composite of Fig. 2).
On the Role of the Lambda Parameter in Simulator Wear of Metal-on-Metal Hip Implants... [Pg.235]

On the role of the lambda parameter in simulator wear of metal-on-metal hip implants... [Pg.281]

Paper VII (v) On The Role of the Lambda Parameter in Simulator Wear of Metal-on-Metal Hip Implants by Mr P Par6, Professor J B Medley, Dr F W Chan and Mr S Young, (University of Waterloo, Waterloo, Ontario, Canada). [Pg.877]

The simulations were carried out on a Silicon Graphics Iris Indigo workstation using the CERIUS molecular modeling and the associated HRTEM module. The multislice simulation technique was applied using the following parameters electron energy 400 kV (lambda = 0.016 A) (aberration coefficient) = 2.7 mm focus value delta/ = 66 nm beam spread = 0.30 mrad. [Pg.106]

Wiedermatm (1986b) presents an alternative method for calculating work done by a fluid. The method uses the lambda model to describe isentropic expansion, and permits work to be expressed as a function of initial conditions and only one fluid parameter, lambda. Unfortunately, this parameter is known for very few fluids. [Pg.201]

Thermal distributions of NO(u 2, J, A Ej,) states were observed, wherein the population in any level was determined by the internal energy and the parameter Tr. and independent of spin-orbit state or lambda doublet species. This is in contrast to the rotational rainbows, the propensities for preferential population in the Il(A ) lambda doublet species and the Fj spin orbit state which were observed in direct inelastic scattering of NO/Ag(l 11). [Pg.56]

The helium spectrum of the WN5 star HD 50896 (EZ Canis Majoris, WR6) is studied. Our aim is to establish a technique which allows the determination of the parameters of a Wolf-Rayet star from a systematic analysis of its spectral lines. Since the method of "iteration with approximate Lambda operators" became available for application to expanding atmospheres (Hamann, 1986, 1987), we are now able to compare observed... [Pg.145]

Figure 13.9 shows plots of this behavior for both the order parameter and the heat capacity of /3-brass. Notice that the heat capacity tends to infinity at the critical transition temperature with the characteristic lambda shape. Above this temperature, further heating produces no more disorder, and the heat capacity falls back to a finite value. [Pg.88]

Table 7.1. Comparison of main parameters of an excimer laser Coherent Lambda Physik LPX305iF [32], and of a pulsed solid state Nd YAG laser Quantel YG981E [33], both suitable for research PLD systems... Table 7.1. Comparison of main parameters of an excimer laser Coherent Lambda Physik LPX305iF [32], and of a pulsed solid state Nd YAG laser Quantel YG981E [33], both suitable for research PLD systems...
The existence of a critical point in the pressure-volume-temperature (PVT) diagram (actually, a point in the planar PV projection, but a critical line in a three-dimensional representation), a critical point (Curie temperature) in ferromagnetism, a critical point (Neel point) in antiferromagnetism, a critical temperature in superconductivity, and a critical point (lambda point) in liquid 2He4 are physical descriptions of the onset of a sudden macroscopic collective transition. If one approaches the critical point very closely, dimensionless parameters, defined to describe this approach, are common to all these disparate phenomena the approach to criticality, or to a phase transition, are really the same. [Pg.334]

Box plots were generated for each scenario comparing the performance of the two imputation methods. Area under the curve extrapolated to infinity (AUCo-inf), % area extrapolated, and terminal half-life (Lambda Z HL) were plotted and compared across different methods. Also the bias and precision associated with the estimation of each of these parameters were compared for the two methods. [Pg.257]

FIGURE 9.1 Performance of the conditional multiple imputation and fractional single multiple imputation (LLOQ/ ) methods under the fourth scenario (i.e., assuming 45% interindividual variability and 25% residual variability) for the following parameters (A) AUCo-inf, (B) %AUC extrapolated, and (C) terminal half-life (Lambda Z HL). [Pg.258]

For He below the lambda point, v(r) represents the velocity of the superfluid. The wavefunction [Eq. (11)] corresponds to a complex local order parameter [130-135] associated with the macroscopic occupation of the Bose-Einstein condensate. [Pg.261]


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See also in sourсe #XX -- [ Pg.220 ]




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