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CURVES internal loops

Simple static instability. Flow excursion (Ledinegg instability) involves a sudden change in the flow rate to a lower value. It occurs when the slope of the channel demand pressure drop-versus-flow rate curve (internal characteristic of the channel) becomes algebraically smaller than the loop supply pressure drop-versus-flow rate curve (external characteristic of the channel). The criterion for this first-order instability is... [Pg.488]

The different forms of dispersion profiles that are obtained from various types of connecting tubes used in LC are shown in figure 9. These dispersion curves were obtained using a low dispersion UV detector (cell volume, 1.4 pi) in conjunction with a sample valve with a 1 pi internal loop. All tubes were of the same length and a flow rate of 2 ml/min was employed. The peaks were recorded on a high speed... [Pg.51]

Figure 3 gives an example of a typical force profile. The force is increased continuously and reaches the point - at the end of the first part of the force profile - where the pectin preparations start to flow. The so-called yield point is reached. The further increase leads to the continuous destruction of the internal structure and the proceeding shear thinning. The applied stress in part 3 of the stress profile destroys the structure of the fruit preparations completely. Now the stress is reduced linearly, see part 4 and 5, down to zero stress. The resulting flow curves 2, 3 and 4 and the enclosed calculated area from the hysteresis loop give important evidence about the time-dependent decrease of viscosity and a relative measure of its thixotropy. [Pg.413]

In order to understand better what happens when a nucleation point, say x = Xo, is selected, let us focus on the small time behavior of the nontrivial self-similar solution. Consider a solution (2.5) at time t = At. It is convenient to parametrize the functions w(x,Ar) and v x,At) by x and present them as a curve in the (w,v) plane. It is not hard to see that one then obtains a loop, beginning and ending in a point (Wo,0) (see Fig. 8b) the details of the loop depend, of course, on the fine internal structures of shocks and kinks (see Fig. 8a). [Pg.194]

An important feature of filled elastomers is the stress softening whereby an elastomer exhibits lower tensile properties at extensions less than those previously applied. As a result of this effect, a hysteresis loop on the stress-strain curve is observed. This effect is irreversible it is not connected with relaxation processes but the internal structure changes during stress softening. The reinforcement results from the polymer-filler interaction which include both physical and chemical bonds. Thus, deforma-tional properties and strength of filled rubbers are closely connected with the polymer-particle interactions and the ability of these bonds to become reformed under stress. [Pg.69]

For the diagrams of Fig. 5.3 we, for instance, find n (5.3a) = 1. nt(5.3 ) = 2. 71 (5.3c) = 1. We may show that with each independent internal momentum we may associate a dosed curve on the graph, through which that momentum flows. This explains the notion of loop . A connected diagram without loops is called a tree . [Pg.65]

Figure 6. Air-water capillary pressure curves for treated Toray TGP-H-120 (10 wt%) showing internal withdrawal scanning loops obtained using the method... Figure 6. Air-water capillary pressure curves for treated Toray TGP-H-120 (10 wt%) showing internal withdrawal scanning loops obtained using the method...
By specifically and selectively reconstructing the total ion peak observed after a loop flow injection to display only the m/z values of interest, the area count for that ion can be extracted from the composite total ion peak. The measured area count can then be used to estimate the quantity of specific alkaloid by comparison to a calibration curve. Thus, component compounds in a mixture are separated by mass, as opposed to chromatography, for quantitation. To normalize the variability of the API response, an internal reference standard is added to the sample prior to loop injection. Alkaloids for which standards are not available are reported as equivalents of a closely related and available standard used to generate the calibration curve, for example, deltaline and methyllycaconitine have been used as calibration standards to represent the non-MSAL and MSAL types of alkaloids, respectively, in the plant material. Calibration curves for these two compounds were linear (r > 0.990) and there appears to be no selective suppression of lower-level alkaloids (figure 13.21). Multiple analyses of Delphinium barbeyi samples returned a level ofprecision that was less than 10 % (relative standard deviation) for all components [56]. [Pg.398]

For further discussion it is expedient to systematize pores (with respect to their sizes) and hysteresis curves (with respect to the sizes and shapes of the loops). Regarding the surface, it is often useful to distinguish between the internal and external surface. Regrettably, there is no unambiguous method of distinguishing between them, because different procedures may yield conflicting... [Pg.114]

By replacing the 125 xL sample loop with loops of identical internal diameter but of different lengths, that is, volumes (e.g., 75, 100, 150, and 200 xL), and in each case injecting samples of the same HCl standard, a plot of the obtained At versus log S, should, according to Eq. (6.3), yield a straight line of slope (Vm/0) In 10. Thus Vm might equally well be calculated from this curve and compared to the previously found value. [Pg.312]

DSC curves are represented in much the same form as DTA curves except that the integral of (the area beneath) the resulting peak is calculated by computer and is equivalent to the internal heat energy (enthalpy) change. In fact, the instrument has two separate control loops - one for average temperature control and the other for differential temperature control. The DSC response is based on the amount of power needed to correct any difference in temperature between the reference and the sample. [Pg.19]

The internal structure of another gel sample (Figure 3.54, curve 2) does not correspond to the loop JT vs Vi dependence, and its swelling curve shows no break. [Pg.402]


See other pages where CURVES internal loops is mentioned: [Pg.292]    [Pg.188]    [Pg.65]    [Pg.68]    [Pg.348]    [Pg.352]    [Pg.299]    [Pg.33]    [Pg.131]    [Pg.268]    [Pg.134]    [Pg.228]    [Pg.134]    [Pg.191]    [Pg.196]    [Pg.175]    [Pg.465]    [Pg.138]    [Pg.116]    [Pg.262]    [Pg.683]    [Pg.336]    [Pg.72]    [Pg.312]    [Pg.116]    [Pg.378]    [Pg.2206]    [Pg.350]    [Pg.89]    [Pg.38]    [Pg.39]    [Pg.429]    [Pg.289]    [Pg.1339]    [Pg.151]    [Pg.231]   
See also in sourсe #XX -- [ Pg.68 ]




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