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Shape stability

For purposes of illustration, suppose that the only the velocity fields Vn considered are those corresponding to the cross-sectional shape of the cavity remaining elliptical, but with changing aspect ratio. This can be accomplished by adopting the equation f x,y,t) = 0 as the equation of the ellipse, as in (8.33), with the additional feature that a and b are now viewed as functions of time t. The equation in (8.33) is then satisfied identically in time. For any time dependent plane curve described by such a function /, the normal velocity is given in terms of partial derivatives of that function with respect to its arguments as [Pg.621]

If the resulting expression is written in terms of the elliptic coordinate ry, [Pg.621]

Similarly, the increment of arclength Sji per unit increment in r/ is given by [Pg.621]

To simplify the calculation further, suppose that Vn is also restricted by the condition that the volume of the cavity remains unchanged. This is assured if the area Tvab of the elliptic hole is held fixed or, equivalently, if o6 + o6 = 0 is satisfied identically in time. [Pg.621]

With this additional constraint, the integral in (8.38) takes the form [Pg.621]


What this adds up to is simply the fact that your study of organic chemistry must integrate the general with the specific. You must not only learn general patterns but also how to apply them to specific molecules, and you must also learn the behavior of specific molecules in order to see where patterns come from. These skills can be learned in a variety of ways, but one of the most effective learning techniques is to study models of molecules that duplicate their size, shape, stability, and other chemically important properties. That is where this workbook comes in. [Pg.1]

Lina, K. Zhang, Y. Xua, X. Dia, H. Yang, R. Qina, P., 2005, Experimental study of underfloor electric heating system with shape-stabilized PCM plates, Energy and Buildings 37 215-220. [Pg.150]

In Fig. 1.1, the parameter space for transient and stable cavitation bubbles is shown in R0 (ambient bubble radius) - pa (acoustic amplitude) plane [15]. The ambient bubble radius is defined as the bubble radius when an acoustic wave (ultrasound) is absent. The acoustic amplitude is defined as the pressure amplitude of an acoustic wave (ultrasound). Here, transient and stable cavitation bubbles are defined by their shape stability. This is the result of numerical simulations of bubble pulsations. Above the thickest line, bubbles are those of transient cavitation. Below the thickest line, bubbles are those of stable cavitation. Near the left upper side, there is a region for bubbles of high-energy stable cavitation designated by Stable (strong nf0) . In the brackets, the type of acoustic cavitation noise is indicated. The acoustic cavitation noise is defined as acoustic emissions from... [Pg.3]

Fig. 1.1 The regions for transient cavitation bubbles and stable cavitation bubbles when they are defined by the shape stability of bubbles in the parameter space of ambient bubble radius (R0) and the acoustic amplitude (p ). The ultrasonic frequency is 515 kHz. The thickest line is the border between the region for stable cavitation bubbles and that for transient ones. The type of bubble pulsation has been indicated by the frequency spectrum of acoustic cavitation noise such as nf0 (periodic pulsation with the acoustic period), nfo/2 (doubled acoustic period), nf0/4 (quadrupled acoustic period), and chaotic (non-periodic pulsation). Any transient cavitation bubbles result in the broad-band noise due to the temporal fluctuation in the number of bubbles. Reprinted from Ultrasonics Sonochemistry, vol. 17, K.Yasui, T.Tuziuti, J. Lee, T.Kozuka, A.Towata, and Y. Iida, Numerical simulations of acoustic cavitation noise with the temporal fluctuation in the number of bubbles, pp. 460-472, Copyright (2010), with permission from Elsevier... Fig. 1.1 The regions for transient cavitation bubbles and stable cavitation bubbles when they are defined by the shape stability of bubbles in the parameter space of ambient bubble radius (R0) and the acoustic amplitude (p ). The ultrasonic frequency is 515 kHz. The thickest line is the border between the region for stable cavitation bubbles and that for transient ones. The type of bubble pulsation has been indicated by the frequency spectrum of acoustic cavitation noise such as nf0 (periodic pulsation with the acoustic period), nfo/2 (doubled acoustic period), nf0/4 (quadrupled acoustic period), and chaotic (non-periodic pulsation). Any transient cavitation bubbles result in the broad-band noise due to the temporal fluctuation in the number of bubbles. Reprinted from Ultrasonics Sonochemistry, vol. 17, K.Yasui, T.Tuziuti, J. Lee, T.Kozuka, A.Towata, and Y. Iida, Numerical simulations of acoustic cavitation noise with the temporal fluctuation in the number of bubbles, pp. 460-472, Copyright (2010), with permission from Elsevier...
Calvisi ML, Lindau O, Blake JR, Szeri AJ (2007) Shape stability and violent collapse of microbubbles in acoustic traveling waves. Phys Fluids 19 047101 (15 pages)... [Pg.26]

Chemical hardness is an energy parameter that measures the stabilities of molecules—atoms (Pearson, 1997).This is fine for measuring molecular stability, but energy alone is inadequate for solids because they have two types of stability size and shape. The elastic bulk modulus measures the size stability, while the elastic shear modulus measures the shape stability. The less symmetric solids require the full set of elastic tensor coefficients to describe their stabilities. Therefore, solid structures of high symmetry require at least two parameters to describe their stability. [Pg.189]

Conducting reactions in nanospace where the dimensions of the reaction vessel are comparable to those of the reactants provides a new tool that can be used to control the selectivity of chemical transformations.1 This dimensional aspect of nano-vessels has been referred to as shape selectivity.2 The effect of spatial confinement can potentially be exerted at all points on the reaction surface but its influence on three stationary points along the reaction coordinate (reactants, transition states, and products) deserve special attention.3,4 (1) Molecular sieving of the reactants, excluding substrates of the incorrect dimension from the reaction site can occur (reactant selectivity). (2) Enzyme-like size selection or shape stabilization of transition states can dramatically influence reaction pathways (transition state selectivity). (3) Finally, products can be selectively retained that are too large to be removed via the nano-vessel openings/pores (product selectivity). [Pg.225]

Recently, the size and shape of a liquid droplet at the molten tip of an arc electrode have been studied,12151 and an iterative method for the shape of static drops has been proposed. 216 Shapes, stabilities and oscillations of pendant droplets in an electric field have also been addressed in some investigations. 217 218 The pendant drop process has found applications in determining surface tensions of molten substances. 152 However, the liquid dripping process is not an effective means for those practical applications that necessitate high liquid flow rates and fine droplets (typically 1-300 pm). For such fine droplets, gravitational forces become negligible in the droplet formation mechanism. [Pg.126]

Sulphur is essential in the usual processing technology of rubbers it brings about the formation of cross-links , which provide the necessary shape stability. Pentane is a blowing agent, applied in a.o. PS, to form foam. [Pg.3]

The high coefficient of expansion can cause problems with shape stability and dimension tolerances in precision products. Moreover the high expansion causes more shrinkage upon cooling after a shaping process (see e.g. MT 10.3.2). [Pg.39]

An example of such a catalyst system is racemic isopropylene bis(l-indenyl) zirconium dichloride in combination with an alumi-noxane (21). The reaction is carried out in hydrocarbon solvents, e.g., toluene. A solution of norbornene in toluene with the catalyst is degassed and then pressurized with ethene. The polymerization is carried out while stirring at 70°C under constant ethylene pressure at 18 bar. After completion, the polymer is precipitated in acetone and filtered (21). The cycloolefin copolymers obtained in this way have a high thermal shape stability and it is possible to use the polymers as thermoplastic molding compositions. [Pg.47]

Semenov (S7) simplified the wavy flow equations by omitting the inertia terms, which is permissible in the case of very thin films. Expressions are obtained for the wavelength, wave velocity, surface shape, stability, etc., with an adjoining gas stream the treatment refers mainly to the case of upward cocurrent flow of the gas and wavy film in a vertical tube. [Pg.175]

The elongation of a stretched liber is best described as a combination of instantaneous extension and a time-dependent exicusion or creep. This viscoelastic behavior is common to many textile libers, including acetate. Conversely, recovery of viscoelastic libers is typically described as a combination of immediate clastic recovery, delayed recovery, and permanent set or secondary creep. The permanent set is the residual extension that is not recoverable. These three components of recovery lor acetate arc given in Table I. The elastic recovery of acetate fibers alone and in blends has also been reported In textile processing strains of mure than 10% are avoided in order to produce a fabric of acceptable dimensional or shape stability. [Pg.629]

Thermomechanical Analysis (TMA). Thermomechanical analysis (TMA) measures shape stability of a material at elevated temperatures by physically penetrating it with a metal rod. A schematic diagram of TMA equipment is shown in Fig. 2.23. In TMA, the test specimen s temperature is raised at a constant rate, the sample is placed inside the measuring device, and a rod with a specified weight is placed on top of it. To allow for measurements at low temperatures, the sample, oven, and rod can be cooled with liquid nitrogen. [Pg.56]

In contrast to natural structures the morphological features of structures in fabricated foods are in principle within our control. The source of the many structures of foods, even those made from a single raw material (e.g., wheat flour), lies in the ingredient mix and the fact that thermodynamic equilibrium is practically never required or achieved during processing. These metastable structures can be attained because they are favored kinetically, that is, the approach to equilibrium is slow. At any point during the development of a particular structure a process of shape stabilization sets in, usually by vitrification, partial crystallization, phase separation and/or formation of a network (Figure 12.5). [Pg.236]

The functional requirements of the ablative heatsliield must be well understood before selection of die proper material can occur. Ablative heatshield materials not only protect a vehicle from excessive heating, they also act as an aerodynamic body and sometimes as a structural component (2,3). Intensity and duration of heating, thermo structural requirements and shape stability (4,5), potential for particle erosion (6), weight limitations (7—10), and reusability (11) are some of the factors which must be considered in selection of an ablative material. [Pg.1]

Pulse shape stability <0.1 ns/h Long time evolution (0.02 ns/h)... [Pg.108]

Kas, J. and Sackmann, E. (1991) Shape transitions and shape stability of giant phospholipid-vesicles in pure water induced by area-to-volume changes. Biophysical Journal, 60 (4), 825-844. [Pg.360]

Parts with an open coherent porosity of >20% are used in vacuum tubes and aeronautics because of refractoriness, shape stability, and chemical resistance. Examples are porous cathodes impregnated with alkaline earth oxides as electron-emitting sources in special tubes, thermoionic converters heated by nuclear energy, and ionic propulsion units with porous tungsten plates as ionic sources for Cs vapor of high temperature. Those emitter plates are made of globular tungsten powder (7 pm) density 75-85%, pore size 2-30 pm, and pore number 1.4 x 10 -8 x 10 cm . ... [Pg.246]

Figure 1.6. Logarithmic dependence of small-angle meridional measurements of PCA-fibres initial of laboratory (2) and factory (1) shaping, stabilized XLY of laboratory (3) and factory (4) shaping. Figure 1.6. Logarithmic dependence of small-angle meridional measurements of PCA-fibres initial of laboratory (2) and factory (1) shaping, stabilized XLY of laboratory (3) and factory (4) shaping.
In the rest of this book we will be examining in more detail ligands, metal-ligand assembly and the consequences. These include molecular shape, stability, properties and how we can measure and interpret these. Further, we will look at metal complexes in place -in nature and in commerce, and speculate on the future. Overall, the intent is to give as broad and deep an overview as is both reasonable and proper in an introductory text. Pray continue. [Pg.14]

Tertiary structure the way in which the polypeptide chains of a protein fold into a characteristic three-dimensional shape, stabilized by bonds between amino acids far apart in the sequence. These bonds may be strong covalent interactions such as disulfide bridges or weaker interactions involving hydrogen bonds or salt bridges. [Pg.111]


See other pages where Shape stability is mentioned: [Pg.48]    [Pg.3]    [Pg.5]    [Pg.25]    [Pg.97]    [Pg.16]    [Pg.673]    [Pg.100]    [Pg.95]    [Pg.104]    [Pg.9]    [Pg.449]    [Pg.289]    [Pg.178]    [Pg.592]    [Pg.215]    [Pg.215]    [Pg.168]    [Pg.508]    [Pg.511]    [Pg.177]    [Pg.337]    [Pg.135]    [Pg.95]    [Pg.554]    [Pg.508]   
See also in sourсe #XX -- [ Pg.222 ]




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Shape stabilization

Shape stabilization

Shape thermodynamic/kinetic stability

Shape-memory stability

Stability bubble shape

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