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Motion of water

Lateral density fluctuations are mostly confined to the adsorbed water layer. The lateral density distributions are conveniently characterized by scatter plots of oxygen coordinates in the surface plane. Fig. 6 shows such scatter plots of water molecules in the first (left) and second layer (right) near the Hg(l 11) surface. Here, a dot is plotted at the oxygen atom position at intervals of 0.1 ps. In the first layer, the oxygen distribution clearly shows the structure of the substrate lattice. In the second layer, the distribution is almost isotropic. In the first layer, the oxygen motion is predominantly oscillatory rather than diffusive. The self-diffusion coefficient in the adsorbate layer is strongly reduced compared to the second or third layer [127]. The data in Fig. 6 are qualitatively similar to those obtained in the group of Berkowitz and coworkers [62,128-130]. These authors compared the structure near Pt(lOO) and Pt(lll) in detail and also noted that the motion of water in the first layer is oscillatory about equilibrium positions and thus characteristic of a solid phase, while the motion in the second layer has more... [Pg.361]

Reynolds, O. Papers on Mechanical and Physical Subjects 2 (1881-1901) 51. An experimental investigation of the circumstances which determine whether the motion of water shall be direct or sinuous and the law of resistance in parallel channels. 535. On the dynamical theory of incompressible viscous fluids and the determination of the criterion. [Pg.139]

The net direction of motion of water is not always the same as the wind, because other... [Pg.235]

TOWARDS THE HYDRODYNAMIC LIMIT STRUCTURE FACTORS AND SOUND DISPERSION. The collective motions of water molecules give rise to many hydrodynamical phenomena observable in the laboratories. They are most conveniently studied in terms of the spatial Fourier ( ) components of the density, particle currents, stress, and energy fluxes. The time correlation function of those Fourier components detail the decay of density, current, and fluctuation on the length scale of the Ijk. [Pg.246]

Kutateladze, S. S, and L. L. Schneiderman, 1953, Experimental Study of Influence of Temperature of Liquid on the Change in the Rate of Boiling, USAEC Rep. tr-3405, 95-100, Washington, DC. (2) Labuntsov, D. A., 1961, Critical Thermal Loads in Forced Motion of Water Which is Heated to a Temperature below the Saturation Temperature, Sov. J. Atomic Energy (English transl.) 70 516-518.(5)... [Pg.542]

Whatever its previous history before disposal and deposition at a site, the alteration of bone buried or exposed to the elements is determined, mainly, by the combined effect of the physical, chemical, and biological conditions at the site where it is deposited these include the seasonal characteristics, average temperature, relative humidity, amount and flow motion of water, pH value, extent of aeration, and the nature of the microorganism population (Millard 2001 White and Hannus 1983). [Pg.410]

Hair cells are the sensory cells of the auditory and vestibular systems. Hair cells are the sensory cells of the internal ear, essential for the senses of sound and balance. The hair cell s transduction apparatus, the molecular machinery that converts forces and displacements into electrical responses, can respond to mechanical stimuli of less than 1 nm in amplitude, and of tens or even hundreds of kilohertz in frequency. Indeed, our hearing is ultimately limited by Brownian motion of water molecules impinging on the transduction apparatus. [Pg.835]

Rotational motion is spinning of the entire molecule around an axis in three-dimensional space. Figure 10 illustrates the rotational motion of a water molecule. Rotational motion occurs in liquid and gas phases of water and, to a limited extent, through defects in the solid phase (ice). Rotational motion of water molecules can be measured using NMR and dielectric spectroscopy (Belton, 1994). [Pg.16]

Despite the care taken to depict the three types of water motion in Figures 9 through 11, it is difficult to illustrate the dynamic three-dimensional motion of water in a static figure. A basic, but very well-done narrated... [Pg.17]

In addition to Ti and T2, which reflect the rotational motion of water, NMR can also be used to measure the translational motion of water. If an additional, relatively small (compared to B0), steady magnetic field gradient is incorporated into a pulsed NMR experimental setup, a translational diffusion coefficient (D, m2/s) can be measured (called pulsed field gradient NMR). [Pg.45]

Rose and Benjamin studied the water dipole and the water H-H vector reorientation dynamics at the water/Pt( 100) interface and the results are reproduced in Fig. 4. As in the case of the translational diffusion, the effect of the surface is to significantly slow down the adsorbed water layer. We note that the effect is very short range, and that the rotational motion of water molecules in the second layer is already very close to the one in bulk water. [Pg.137]

Water motion in the ocean is the result of two general phenomena, advection and turbulence. Advection causes water to experience large-scale net displacement (directed transport), whereas turbulent mixing involves the random motion of water molecules... [Pg.82]

A negative change in entropy associated with the decreased freedom of motion of water molecules in the vicinity of a nonpolar group. As pointed out by Jencks one should not be too literal when interpreting this behavior, because the system is dynamic, and not frozen. The term flickering cluster implies some reduction in libration and rotation without complete loss. [Pg.359]

FIGURE 3.1 (a) Internal vibrations of the bonds in the water molecule, (b) rotational motion of water, and (c) translation of the water molecule. [Pg.44]

This illustration from four dimensions, suggesting other illustrations derivable from mathematics, may serve a double purpose in our present investigation. On the one hand it may lead us to vaster views of possible circumstances and existence on the other hand it may teach us that the conception of such possibilities cannot, hy any ditect path, bring us closer to God. Mathematics may help us to measure and weigh the planets, to discover the materials of which they are composed, to extract light and warmth from the motion of water and to dominate the material universe but even if by these means we could mount up to Mars or hold converse with the inhabitants of Jupiter or Saturn, we should be no nearer to the divine throne, except so far as these new experiences might develop in our modesty, respect for facts, a deeper reverence for order and harmony, and a mind more open to new observations and to fresh inferences from old truths. [Pg.167]

Figure 5 shows the change of T2 values for XH of water with the inverse absolute temperature. A sudden decrease in T2 values is seen at almost the same temperatures at which the minimum in Ti is observed. The T2 values give an average representation of the motion of water molecules in the system. Therefore, if we consider the molecular motion of water in the water-NaLS system having a certain Wc, the T2 values at higher temperatures are characteristic of more mobile water, while the T2 values at lower temperatures are characteristic of more restricted water. [Pg.282]

Ultrafast motion of water molecules near ions... [Pg.149]


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Translational motion of water inside a CNT

Water motion

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