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Tire triangle

Figure C2.6.9. Phase diagram of charged colloidal particles. The solid lines are predictions by Robbins et al [85]. Fluid phase (open circles), fee crystal (solid circles) and bee crystal (triangles). is tire interaction energy at tire... Figure C2.6.9. Phase diagram of charged colloidal particles. The solid lines are predictions by Robbins et al [85]. Fluid phase (open circles), fee crystal (solid circles) and bee crystal (triangles). is tire interaction energy at tire...
At equilibrium, in order to achieve equality of chemical potentials, not only tire colloid but also tire polymer concentrations in tire different phases are different. We focus here on a theory tliat allows for tliis polymer partitioning [99]. Predictions for two polymer/colloid size ratios are shown in figure C2.6.10. A liquid phase is predicted to occur only when tire range of attractions is not too small compared to tire particle size, 5/a > 0.3. Under tliese conditions a phase behaviour is obtained tliat is similar to tliat of simple liquids, such as argon. Because of tire polymer partitioning, however, tliere is a tliree-phase triangle (ratlier tlian a triple point). For smaller polymer (narrower attractions), tire gas-liquid transition becomes metastable witli respect to tire fluid-crystal transition. These predictions were confinned experimentally [100]. The phase boundaries were predicted semi-quantitatively. [Pg.2688]

Fig. 5.5 The first few steps of the simplex algorithm with the function + 2i/. The initial simplex corresponds to the triangle 123. Point 2 has the largest value of the function and the next simplex is the triangle 134. The simplex for tire third step is 145. Fig. 5.5 The first few steps of the simplex algorithm with the function + 2i/. The initial simplex corresponds to the triangle 123. Point 2 has the largest value of the function and the next simplex is the triangle 134. The simplex for tire third step is 145.
Figure 13-6. The vullage dependence ol the cuinenl densities in the dark (open triangles), under illumination (open circles) and their difference (filled squares) for an fTO/MEH-PPV/Mg OLED. The inset shows the same data plotted as tire logarithm of the current (difference)- Reproduced with permission front [97J. Figure 13-6. The vullage dependence ol the cuinenl densities in the dark (open triangles), under illumination (open circles) and their difference (filled squares) for an fTO/MEH-PPV/Mg OLED. The inset shows the same data plotted as tire logarithm of the current (difference)- Reproduced with permission front [97J.
For vacuum fractional distillation of liquids having close boiling points, which necessitates the use of a total condensation variable take-off head, the receiver adapter modification noted in Fig. 2,106 is employed. Its operation is similar to that of the Perkin triangle the column is operated under total reflux while the receivers tire being changed. [Pg.185]

A good way to visualise the data is via contours in a mixture triangle, allowing three components to vary and constraining the fourth to be constant. Using a step size of 0.05, calculate tire estimated responses from tire model in question 2 when... [Pg.114]

Tire case of cyclopropane has been discussed in detail by Robin Quantum chemical calculations show that the frontier orbital is 3e a, a sigma orbital composed of 2p atomic orbitals of the carbon atoms oriented tangentially to the inter-nuclear triangle, and having maximum overlap symmetrically in-plane, outside each edge . The lowest energy photoelectron band which corresponds to ionization from this orbital exhibits a large split (about 8000 cm ) due to the Jahn-Teller effect. [Pg.112]

The steady-state nucleation rate J is measured during the nucleation stage, when the number of precipitates is varying quite linearly with time. Slowdown of precipitation kinetics with triangle and tetrahedron order corrections can be seen on the steady-state nucleation rate (Fig. 7) without these corrections is about two times higher than when these corrections tire included. [Pg.233]


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