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Sampling model

Figure 1. Sampling models for estimating a population average. Figure 1. Sampling models for estimating a population average.
Resource (cost) information can be used in conjunction with the sampling models to obtain an optimum allocation of resources in an environmental sampling study. [Pg.88]

The powdery sample (e.g. a mortar) is mixed with 60 100 pi of trypsin solution (see above). Usually 5 10 mg of model fresh mortar, containing about 100 pg of proteins, is sufficient for a reliable identification. In the case of older samples (model samples aged for 9 months were tested) about 100 mg of the material was necessary. Similar amounts of samples from buildings of different age (Section 6.4.4) were needed. [Pg.174]

Valino, L. and C. Dopazo (1990). A binomial sampling model for scalar turbulent mixing. [Pg.424]

Figure 41. Evaluating the stability of the simple example pathway shown in Fig. 40 Metabolic states and the corresponding saturation parameters are sampled randomly and their stability is evaluated. For each sampled model, the largest positive part within the spectrum of eigenvalues is recorded. Shown is the probability of unstable models, as a function of (A) The size of the system. Here the number of regulatory interactions increases proportional to the length of pathway (number of metabolites). Other parameters are maximal reversibility ymax 1 and p 0.5. (B) An increasing number of regulatory interactions. The number of metabolites m 100 is constant. Maximal reversibility ymax 1 and p 0.5. (C) Maximal reversibility v /v . and p 0.5. Other... Figure 41. Evaluating the stability of the simple example pathway shown in Fig. 40 Metabolic states and the corresponding saturation parameters are sampled randomly and their stability is evaluated. For each sampled model, the largest positive part within the spectrum of eigenvalues is recorded. Shown is the probability of unstable models, as a function of (A) The size of the system. Here the number of regulatory interactions increases proportional to the length of pathway (number of metabolites). Other parameters are maximal reversibility ymax 1 and p 0.5. (B) An increasing number of regulatory interactions. The number of metabolites m 100 is constant. Maximal reversibility ymax 1 and p 0.5. (C) Maximal reversibility v /v . and p 0.5. Other...
Figure 42. The distribution of the largest real part within the spectrum of eigenvalues for the model of the Calvin cycle described in Section VIII. F. Only a minority of sampled models correspond to a stable steady state. See also Fig. 37 for convergence in dependence of the number of samples. Figure 42. The distribution of the largest real part within the spectrum of eigenvalues for the model of the Calvin cycle described in Section VIII. F. Only a minority of sampled models correspond to a stable steady state. See also Fig. 37 for convergence in dependence of the number of samples.
The most surprising result is that such simple non-linear relaxation behaviour can give rise to such complex behaviour of the stress with time. In Figure 6.3(b) there is a peak termed a stress overshoot . This illustrates that materials following very simple rules can show very complex behaviour. The sample modelled here, it could be argued, can show both thixotropic and anti-thixotropic behaviour. One of the most frequently made non-linear viscoelastic measurements is the thixotropic loop. This involves increasing the shear rate linearly with time to a given... [Pg.223]

Catalysts consisting of more than one component are often superior to monometallic samples. Model studies with potassium on Fe surfaces revealed, for example, the role of the electronic promoter in ammonia synthesis. A particularly remarkable case was recently reported for a surface alloy formed by Au on a Ni(lll) surface where the combination of STM... [Pg.66]

Intestinal Perfusion with Venous Sampling Models... [Pg.50]

Generic, Object-Oriented Innovation Process Modeling Method and Sample Model... [Pg.165]

GENERIC, OBJECT-ORIENTED INNOVATION PROCESS MODELING METHOD AND SAMPLE MODEL... [Pg.174]

Saving the spreadsheet as a sample model (.xlt) (this could only be performed if local use of the spreadsheet is intended)... [Pg.288]

Mix 0.1ml of the sample (model solution, blood serum, dialysis liquid) with 0.9 ml of 0.9% NaCl. [Pg.1214]

Figure 4.14. The block scheme of the sample model of water balance in a small territory. Figure 4.14. The block scheme of the sample model of water balance in a small territory.
Tea, 1 i g, respectively. However, in contrast to the case of identical atoms, these two channels of transitions are not independent and their decays are correlated through various off-diagonal terms. The decay rates Teai and 1 /g are much smaller than the decay rates 1 si, 1 jg involving the symmetric state and can be reduced to zero. This happens only for atomic separations much smaller than the optical wavelenght (the small sample model). In particular, the decay rate Taig... [Pg.230]

The pure state (113) is nonmaximally entangled state it reduces to a maximally entangled state for N l. The entangled state is analogous to the pairwise atomic state [22] or the multiatom squeezed state [23], (see also Ref. 24), predicted in the small sample model of two coupled atoms. [Pg.256]

Note that the states T4), T2) and T3) are the same as for the small sample model, discussed in the preceding section. This means that the presence of the antisymmetric state does not affect the two-photon entangled states, but it can affect the population distribution between the states and the purity of the system. In Fig. 10, we plot the populations P, of the states T,) as a function of the interatomic separation. The figure demonstrates that the atoms are driven into a mixed state composed of two states Tj) and a), and there is a vanishing probability that the system is in the states IT2) and s). [Pg.259]

These equations are quite different from Eqs. (114) that in the case of nonidentical atoms the symmetric and antisymmetric states are equally populated independent of the interatomic separation. These are, however, similar to the steady-state solutions for the small sample model that for small interatomic separations pM = paa 0 and then only the collective ground and the upper states are populated. [Pg.261]

However, the complete transfer of the correlations does not necessary mean that the two-photon correlations are stored in the pure TPE state. This happens only for the small sample model and two atoms with significantly different transition frequencies, where the steady state is the pure TPE state. For identical atoms separated by a finite distance r 2, a part of the correlations is stored in the antisymmetric state. This fact can lead to an interesting modification of the interference pattern of the fluorescence field. Using the steady-state solutions (114), we find that the visibility in the interference pattern is given by [58]... [Pg.262]


See other pages where Sampling model is mentioned: [Pg.287]    [Pg.398]    [Pg.83]    [Pg.83]    [Pg.86]    [Pg.86]    [Pg.165]    [Pg.165]    [Pg.116]    [Pg.359]    [Pg.286]    [Pg.224]    [Pg.317]    [Pg.317]    [Pg.344]    [Pg.436]    [Pg.211]    [Pg.257]    [Pg.293]    [Pg.35]    [Pg.341]    [Pg.44]    [Pg.112]    [Pg.366]    [Pg.224]    [Pg.410]    [Pg.111]   
See also in sourсe #XX -- [ Pg.190 ]




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