T,-divide

Divaricatinsaure,/. divaricatinic acid. Divaricatsaure,/. divaricatic acid, divergierend, p.a. diverging, divergent, dividieren, v.t. divide. 

Teildruck, m. partial pressure, teilen, ti.t, divide graduate share, participate io. — v.T. divide share. 

Eeevers I think it is more likely that there is a link between protein synthesis, growth rate and the production of a specific cell cycle regulator. This is a great mechanism to ensure a minimum cell size, making sure that cells don t divide until they are growing at a certain rate and producing everything they will need to divide at a reasonable level. 

T divided by the viscosity of the solvent r s. For n-octane this number is 837 K/cP at T = 323 K. The results of the fitting process are all below this theoretical value. This is not surprising, since even in the case of dilute solutions of unattached linear chains, the theoretical values are never reached (see Sect. 5.1.2). In addition the experimental T/r s values differ considerably for the different labelling conditions and the different partial structure factors. Nevertheless, it is interesting to note that T/r s for the fully labelled stars is within experimental error the arithmetic mean of the corresponding core and shell values. 

Sample the initial distribution function P x,p,t = Q) by a set of random walkers. The ith random walker carries the information of its phase-space position (xi,pi), density-matrix component (nm)-, weight VF(xi, Pi, t), and phase a(xi, pi, t). Divide the whole time interval into N small enough pieces such that the desired accuracy of the Trotter scheme is guaranteed. 

When dash pot and spring elements are connected in parallel they simulate the simplest mechanical representation of a viscoelastic solid. The element is referred to as a Voigt or Kelvin solid, and it is shown in Fig. 3.10(c). The strain as a function of time for an applied force for this element is shown in Fig. 3.11. After a force (or stress) elongates or compresses a Voigt solid, releasing the force causes a delay in the recovery due to the viscous drag represented by the dash pot. Due to this time-dependent response the Voigt model is often used to model recoverable creep in solid polymers. Creep is a constant stress phenomenon where the strain is monitored as a function of time. The function that is usually calculated is the creep compliance/(f) /(f) is the instantaneous time-dependent strain e(t) divided by the initial and constant stress o. ... 

We first assume that the tube has constant diameter D and also that the density does not vary with position (either liquids or gases with no mole number change, pressure drop, or temperature change with gases). In this case the linear velocity u with which the fluid flows through the tube is equal to the volumetric flow rate t divided by the cross-sectional tube area At (At = 7t j A for a cylindrical tube),... 

When making a table or chart, you want to be as systematic as possible so you don t miss anything - especially if that anything is the correct answer. After you ve determined a variable to represent a quantity in the problem, you need to go up in logical steps — by ones or twos or halves or whatever is appropriate. In Table 1-2, in the preceding section, you can see that I went up in steps of 1 until I got to the 6. One more than 6 is 7, but 7 doesn t divide into 60 evenly, so I skipped it. Even though the work isn t shown here, I mentally tried 7, 8, and 9 and discarded them, because they didn t work in the problem. When you re working with more complicated situations, you don t want to skip any steps — show them all. 

B looked so crest-fallen at having his grand exposition so preempted that A felt compelled to add, I like your analogy to peotry. But I don t see a naturally occurring number to divide your population by. You can t divide by zero or infinity, if I remember rightly, and the initial population is quite arbitrary. ... 

Conversion factors for various pressure units and flow units are given in Table VI.1. Table VI.2 lists values of the ratio d,/do (the density of mercury at a temperature t divided by the density of mercury at 0°C) over the temperature range 0-99°C. Capillary depression corrections for mercury in glass tubes are given in Table VI.3. The complete set of corrections for a pressure measurement is made as follows ... 

While we can t divide 1 by infinity (00), the mathematical limit of dividing 1 by an increasingly large number is zero. Thus, the l/R2 drops out. 

Detailed high-frequency (terahertz) dynamical studies of glasses have been probed by inelastic X-ray scattering (IXS) [139], The advantage of this technique is that with reliable measurements it allows determination of the so-called nonergodicity parameter f(q, T) as a function of wavevector q this quantity is defined by the long time limit of the density-density correlation function F(q, t) divided by the static structure factor [15],... 

Bartholomew and co-workers also measured the loss of catalytic activity with time of Ni and Co bimetallics (157, 194), Ni-molybdenum oxide (23, 113), and borided Ni and Co catalysts (161) during methanation in the presence of 10 ppm H2S. Typical activity versus time plots are shown in Figs. 25 and 26. Activity is defined as the ratio of the mass-based rate of methane production at any time t divided by the initial rate. The activitytime curves are generally characteristic of exponential decay some catalysts decay more slowly than others, but all catalysts suffer at least two orders of magnitude loss in activity within a period of 100-150 hr. Accordingly, it does not appear that other metals or metal oxides in conjunction with Ni significantly change the sulfur tolerance defined in terms of steady-state activity of Ni. These materials can, however, influence the rate at which the... 

A corresponding states plot of the self-diffusivity /J>AA., which is the interdiffusion of labeled molecules of A at the low-pressure limit, is shown in Figure 2.7. The reduced self-diffusivity that is cDAA> at pressure P and T divided by cDAfi. at the critical point is plotted as a function of the reduced pressure and reduced temperature. Figure 2.7 shows that c+>AA. increases sharply with increasing temperature, especially for liquids. The values of c/J>AA. decrease toward a low-pressure limit at each temperature. 

This relation is valid for every wavelength channel. The measuring time which is available for each channel is the total time t, divided by the time ta needed to measure one channel. The time which is necessary to record the entire spectrum with M channels is... 

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