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Soft circle

Figure 8.38. Structural parameters of an ensemble of needle-shaped soft domains in a poly(ether ester) as a function of elongation . D (open circles) is the average needle diameter, a/D (filled circles) is the relative standard deviation of the needle-diameter distribution. Square symbols demonstrate the lateral compressibility of the soft needles during elongation... [Pg.184]

Figure 16.1 The chemical hardness of an atom, molecule, or ion is defined to be half. The value of the energy gap between the bonding orbitals (HOMO—highest orbitals occupied by electrons), and the anti-bonding orbitals (LUMO—lowest orbitals unoccupied by electrons). The zero level is the vacumn level, so I is the ionization energy, and A is the electron affinity, (a) For hard molecules the gap is large (b) it is small for soft molecules. The solid circles represent valence electrons. Adapted from Atkins (1991). Figure 16.1 The chemical hardness of an atom, molecule, or ion is defined to be half. The value of the energy gap between the bonding orbitals (HOMO—highest orbitals occupied by electrons), and the anti-bonding orbitals (LUMO—lowest orbitals unoccupied by electrons). The zero level is the vacumn level, so I is the ionization energy, and A is the electron affinity, (a) For hard molecules the gap is large (b) it is small for soft molecules. The solid circles represent valence electrons. Adapted from Atkins (1991).
Matrixes Three types of paper filters (i). Filtrak, Germany, the filter Number 388 [(0.025) - soft, wide pores] filters No. 90 (0.15) and No. 90 (0.25) - dense, narrow pores) (ii). chromatographic papers FN-5, FN-11 (Germany) the kapron membrane (pore size 0.2 microns) and (iii). the membrane Vladipor MFA-MA No. 6 (Kazan industrial associations Tasma )] were applied to matrixes for biotests. The circles (6 -10 mm dia) are cut out from the matrixes materials by special instrument. The most stable results are received with use of matrixes of chromatographic papers FN-5, FN-11. [Pg.150]

Figure 3.4. Breakdown of device performance at Tg The luminance for a constant current density of 25 mA/cm2 is plotted for two light emitting diodes that were made with hole transport materials of different Tg. Triangles 75-nm TPD/65 nm Alq3 Circles 75-nm Spiro-TAD/65 nm Alq3. The dotted lines mark the respective Tg values TPD 63°C, Spiro-TAD 133°C. At these temperatures, the materials become soft, which results in a steep decrease in the efficiency. Figure 3.4. Breakdown of device performance at Tg The luminance for a constant current density of 25 mA/cm2 is plotted for two light emitting diodes that were made with hole transport materials of different Tg. Triangles 75-nm TPD/65 nm Alq3 Circles 75-nm Spiro-TAD/65 nm Alq3. The dotted lines mark the respective Tg values TPD 63°C, Spiro-TAD 133°C. At these temperatures, the materials become soft, which results in a steep decrease in the efficiency.
Symptoms A very common fungal problem that produces soft, brown patches on fruit Concentric circles of white fluffy growth also develop on these areas while fruit is on the tree or in storage. Fruit may turn black. Some fruit on the tree will shrivel, become mummified, and remain attached throughout the winter. [Pg.323]

Figure 14 shows the result of a Brillouin scattering experiment in the vicinity of Tc [11]. Closed circles and open circles below Tc indicate the modes split from the doubly degenerated ferroelectric soft mode. The closed circles above Tc denote the frequency of the doubly degenerated soft u mode in the paraelectric phase. The results clearly show a softening of the soft mode toward zero frequency at Tc following the Curie-Weiss law. The soft mode remains underdamped even at Tc. Generally, a soft mode is heavily damped in the vicinity of Tc, e.g., as for PbTiOs, which are typical displacive-type... [Pg.105]

Fig. 14 Temperature dependence of modes observed in ST018. The soft u mode closed circles above Tc) in the tetragonal Dih phase is divided into two modes presented by open circles (below T ) and closed circles (at Td. Closed squares and open squares denote the modes split from the doubly degenerated Eg mode. Closed triangles above Tc indicate the Raman-inactive Aiu mode observed by local symmetry breakdown [11]... Fig. 14 Temperature dependence of modes observed in ST018. The soft u mode closed circles above Tc) in the tetragonal Dih phase is divided into two modes presented by open circles (below T ) and closed circles (at Td. Closed squares and open squares denote the modes split from the doubly degenerated Eg mode. Closed triangles above Tc indicate the Raman-inactive Aiu mode observed by local symmetry breakdown [11]...
Fig. 17 Temperature dependencies of the mode observed in ST016 closed circles), STO 18-23 closed squares), and STO 18-32 closed triangles) observed in the scattering geometry x yy)-x. Crosses indicate the results for STO 16 obtained by the hyper-Raman scattering experiment. The corresponding open symbols denotes the half-width at half maximum of the soft u mode spectrum of each specimen [27]... Fig. 17 Temperature dependencies of the mode observed in ST016 closed circles), STO 18-23 closed squares), and STO 18-32 closed triangles) observed in the scattering geometry x yy)-x. Crosses indicate the results for STO 16 obtained by the hyper-Raman scattering experiment. The corresponding open symbols denotes the half-width at half maximum of the soft u mode spectrum of each specimen [27]...
Fig. 25. Guinier plot of the soft sphere model. The numbers denote the number of branching shells the filled and open circles are lightscattering results from polyvinyl acetate (PVAc) microgels in methanol at 20 °C at A0 = 546 nm and 436 nm, respectively. The dot-dash line corresponds to the Rayleigh-Gans behavior of hard spheres, i.e. no Mie scattering93)... Fig. 25. Guinier plot of the soft sphere model. The numbers denote the number of branching shells the filled and open circles are lightscattering results from polyvinyl acetate (PVAc) microgels in methanol at 20 °C at A0 = 546 nm and 436 nm, respectively. The dot-dash line corresponds to the Rayleigh-Gans behavior of hard spheres, i.e. no Mie scattering93)...
FIGURE 2.5 Hypoglycemic effect of insulin administered orally to normal rats by means of coated soft capsules containing an absorption-enhancing formulation (8 IU porcine insulin, 4 mg sodium laurate (Ci2) and 16 mg cetyl alcohol) two capsules RSI (open stars) 2 capsules RS2 (open circles) 2 capsules RS2 + 1 capsule surfactant post-insulin administration (open square) insulin i.p. 4 IU (close circles) 2 placebo capsules (no insulin) (close stars). Each point is the mean SD of five animals for insulin administration and of four animals for controls. RSI and RS2 are capsules coated with various mixtures of Eudragits RS, S, and L. (From Touitou, E. and Rubinstein, A., Int. J. Pharm., 30, 95, 1986. With permission from Elsevier.)... [Pg.47]

Figure 1. Saturation magnetization and initial permeability of various soft magnetic materials. The open squares and circles denote FINEMET [1, 6] and NANOPERM [8, 25], respectively. Figure 1. Saturation magnetization and initial permeability of various soft magnetic materials. The open squares and circles denote FINEMET [1, 6] and NANOPERM [8, 25], respectively.
Figure 4.8-18 Soft modes of Pb vGe.iTe. Reflectivity, experimentally determined (full line) and calculated (circles), for x = 0.0056 (a) and square TO frequency vs. temperature for two different carrier concentrations p = 5.2-10 and 6.8- lO cm respectively, as indicated in (b), according to Jantsch, 1983. Figure 4.8-18 Soft modes of Pb vGe.iTe. Reflectivity, experimentally determined (full line) and calculated (circles), for x = 0.0056 (a) and square TO frequency vs. temperature for two different carrier concentrations p = 5.2-10 and 6.8- lO cm respectively, as indicated in (b), according to Jantsch, 1983.
When my discomfort subsided, I poked my head out and oriented myself. I rose and moved away from the circle to an area I had spotted before the session. There I knelt on a soft sandy bed, bordered by tall lush plants. Next to me, the creek narrowed into a strong flow of water that descended to a gentle waterfall. The plants were luminescent, glowing with an inner light that spilled out into the ether around them. I sensed the presence of faeries in this natural garden. I could hear them speak in sweet singsong tones. [Pg.237]

A technological overview of soft drinks can be visualised as a soft drink circle , as shown in Fig. 5.30. This overview shows the broad variability of raw materials used in soft drinks. [Pg.466]

The soft drink circle should be read from inner to outer circle. First of all, the world of soft drinks can be categorised into clear and cloudy products, as further described in 5.2.1.1 and 5.2.1.2. In these chapters, more information can be found on important raw materials, like juices, extracts and emulsions. Within these main categories of soft drinks, it is also important to differentiate between juice specialities, flavours, source of extracts and the principal bases of emulsions. [Pg.467]

The three outer closed circles characterise the raw materials that will be used in all types of soft drinks. More information on colours, the important area of health and nutrition and sweeteners can be found in 5.2.1.3. All remarks on single ingredients are focused on their importance in soft drinks. [Pg.467]

Fig. 21. The histograms show the distributions of total scattering angle a for the reflected atoms, (a) Ar+, 50 eV, 85°, bare Si and (b) C1+, 50 eV, 85°, 2.3-MI. Si -Cl. Filled circles represent the average reflected energy fraction corresponding to the reflection angle. Single-scatter (SS) soft-soft branch and double half-scatter (DHS) soft-soft branch model predictions for (a) jjL = 1.43 and (b) jjL = 1.0 also shown for comparison with data from simulation. Fig. 21. The histograms show the distributions of total scattering angle a for the reflected atoms, (a) Ar+, 50 eV, 85°, bare Si and (b) C1+, 50 eV, 85°, 2.3-MI. Si -Cl. Filled circles represent the average reflected energy fraction corresponding to the reflection angle. Single-scatter (SS) soft-soft branch and double half-scatter (DHS) soft-soft branch model predictions for (a) jjL = 1.43 and (b) jjL = 1.0 also shown for comparison with data from simulation.
The major difference between soft shaped pulses and DANTE methods is the occurrence of strong sideband excitation windows either side of the principal window with DANTE. These occur at offsets from the transmitter at multiples of the hard-pulse frequency, 1/x. They arise from magnetisation vectors that are far from resonance and which process full circle during the x period. Since this behaviour is precisely equivalent to no precession, they are excited as if on-resonance. Further sidebands at 2/x, 3/x and so on also occur by virtue of trajectories completing multiple full circles during x. Such multisite excitation can at times be desirable [50,51] but if only a single excitation window is required, the hard pulse repetition frequency must be adjusted by varying x to ensure the sideband excitations do not coincide with other resonances. [Pg.355]

Soft C (sounds like s) central circle cymbal circus cirrus cent... [Pg.45]

Fig. 12. Values of the reduced diffusion coefficient for the soft-sphere model as a function of the reduced volume from molecular dynamics simulations circles, from Cape and Woodcock squares, from Hiwatari et al. triangles, from Ross and Schofield. The scale at the right shows the equivalent diffusivities for argon-like soft-spheres. Fig. 12. Values of the reduced diffusion coefficient for the soft-sphere model as a function of the reduced volume from molecular dynamics simulations circles, from Cape and Woodcock squares, from Hiwatari et al. triangles, from Ross and Schofield. The scale at the right shows the equivalent diffusivities for argon-like soft-spheres.
What s the matter, baby " Jezzibella asked quietly. Soft arms circled around him. [Pg.358]


See other pages where Soft circle is mentioned: [Pg.240]    [Pg.208]    [Pg.19]    [Pg.313]    [Pg.327]    [Pg.18]    [Pg.477]    [Pg.46]    [Pg.169]    [Pg.247]    [Pg.14]    [Pg.399]    [Pg.105]    [Pg.442]    [Pg.790]    [Pg.56]    [Pg.244]    [Pg.467]    [Pg.4]    [Pg.343]    [Pg.20]    [Pg.232]    [Pg.162]    [Pg.443]    [Pg.336]    [Pg.235]    [Pg.197]   
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