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Dilation velocity

Lowenfeld12 identified the components of the fight reflex that were controlled by parasympathetic and sympathetic innervation of the smooth muscles controlling pupil diameter. They concluded that the parasympathetic nervous system must be intact to observe the light reflex the sympathetic nervous system influences the shape of the reflex. For example, in the absence of sympathetic innervation, the constriction velocity is increased and the dilation velocity is decreased. Conversely, in situations of increased sympathetic tone, the constriction is sluggish and incomplete, and the pupil slowly returns to its baseline size. The effects of abused drugs on these and other components of the light reflex were studied in the experiment described below. [Pg.130]

Drug Dose Pupil Diameter Constriction Amplitude Constriction Velocity Dilation Velocity... [Pg.133]

The physics and modeling of turbulent flows are affected by combustion through the production of density variations, buoyancy effects, dilation due to heat release, molecular transport, and instabiUty (1,2,3,5,8). Consequently, the conservation equations need to be modified to take these effects into account. This modification is achieved by the use of statistical quantities in the conservation equations. For example, because of the variations and fluctuations in the density that occur in turbulent combustion flows, density weighted mean values, or Favre mean values, are used for velocity components, mass fractions, enthalpy, and temperature. The turbulent diffusion flame can also be treated in terms of a probabiUty distribution function (pdf), the shape of which is assumed to be known a priori (1). [Pg.520]

Now we consider the possibility that the target is moving relative to the radar. The scattered waveform is modified by the Doppler effect. If this is done correctly it results in a time dilation of the return signal, so that, if the target has a radial velocity v, the return signal su(t) becomes... [Pg.271]

Figure 3.10 The dilation of the flow field around a spherical particle. The shear field has a vorticity equal to y/2 and the particle rotates with this constant angular velocity... Figure 3.10 The dilation of the flow field around a spherical particle. The shear field has a vorticity equal to y/2 and the particle rotates with this constant angular velocity...
Boussinesq (B4) proposed that the lack of internal circulation in bubbles and drops is due to an interfacial monolayer which acts as a viscous membrane. A constitutive equation involving two parameters, surface shear viscosity and surface dilational viscosity, in addition to surface tension, was proposed for the interface. This model, commonly called the Newtonian surface fluid model (W2), has been extended by Scriven (S3). Boussinesq obtained an exact solution to the creeping flow equations, analogous to the Hadamard-Rybczinski result but with surface viscosity included. The resulting terminal velocity is... [Pg.36]

The first equation is scalar, and has a wave solution with velocity Vi = -J c /p). This is the longitudinal wave of eqn (6.7). It is sometimes called an irrotational wave, because V x u = 0 and there is no rotation of the medium. The second equation is vector, and has two degenerate orthogonal solutions with velocity v = s/(cu/p)- These are the transverse or shear waves of eqn (6.6) the degenerate solutions correspond to perpendicular polarization. They are sometimes called divergence-free waves, because V u = 0 and there is no dilation of the medium. Waves in fluids may be considered as a special case with C44 = 0, so that the transverse solutions vanish, and C = B, the adiabatic bulk modulus. [Pg.82]

The preceding is a result of special relativity precise to one part in 1023 [49]. Its explanation in standard special relativity is as follows. Let the tangential velocity of the disk be vi and the velocity of the particle be V2 in the laboratory frame [52]. When the particle and disk are moving in the same direction, the velocity of the particle is v2 v i = V3 relative to an observer on the periphery of the disk. Vice-versa, the relative velocity is v2 + v = V4. The special theory of relativity states that time for the two particles will be dilated to different... [Pg.118]

Stress and Strain Rate The stress and strain-rate state of a fluid at a point are represented by tensors T and E. These tensors are composed of nine (six independent) quantities that depend on the velocity field. The strain rate describes how a fluid element deforms (i.e., dilates and shears) as a function of the local velocity field. The stress and strain-rate tensors are usually represented in some coordinate system, although the stress and strain-rate states are invariant to the coordinate-system representation. [Pg.17]

The radial velocity itself varies over the length of the differential element that is to say, the velocity at one edge of the element is different than that at the other end. For this reason the element will stretch or shrink, meaning dilate. The extent of the dilatation, over a differential unit of time, is (dvfdr)drdt. Thus it follows easily that... [Pg.30]

Note that even for pure radial flow, w = 0, there is still a circumferential dilatation, Fee 7 0. This is because the radial velocity spreads the flow as seen by the dashed differential element in Fig. 2.7. [Pg.32]

The relative volumetric expansion is seen to be the sum of the normal strain rates, which is the divergence of the vector velocity field. The sum of the normal strain rates is also an invariant of the strain-rate tensor, Eq. 2.95. Therefore, as might be anticipated, the relative volumetric dilatation and V V are invariant to the orientation of the coordinate system. [Pg.39]

Using the spreadsheet representation of the CVD flow field (Fig. 2.23), form the divergence of the velocity field (V V). Where are the regions of very small divergence In these regions, what can be said about the volumetric dilatation and defacto incompressibility ... [Pg.64]

Figure 7.1 Pupil diameter before (A) and after a light stimulus (S). Constriction (B) and dilation (D) velocities are determined from a least square fit of the slope. Amplitude of constriction (C) represents the maximal difference in diameter before and after the flash. Figure 7.1 Pupil diameter before (A) and after a light stimulus (S). Constriction (B) and dilation (D) velocities are determined from a least square fit of the slope. Amplitude of constriction (C) represents the maximal difference in diameter before and after the flash.
As summarized in Table 7.1, only the high dose of marijuana significantly changed (reduced) the velocity of dilation of the pupil during the recovery phase of the light reflex. [Pg.133]

One way to understand special relativity is to see how time dilation and Lorentz contraction of objects parallel to motion can be used to explain the null results of the Michelson-Morley [1] experiment, which was performed to measure the velocity of earth in relation to an assumed ether. The result was that the expected influence of such an ether on the velocity of light was not found. Let us now study this double-pass example, where one arm of a Michelson interferometer was perpendicular to the velocity of the earth s surface, while the other... [Pg.268]

Thus the Doppler shift is the difference between the Doppler-shifted wavelength (k) and the original wavelength (A0) divided by Aq- The numerator is the classical Doppler redshift from a moving light source, while the denominator represents the red-shift caused by the relativistic time dilation resulting from the total velocity, which is independent of the direction of motion. [Pg.280]


See other pages where Dilation velocity is mentioned: [Pg.130]    [Pg.131]    [Pg.133]    [Pg.135]    [Pg.136]    [Pg.139]    [Pg.140]    [Pg.130]    [Pg.131]    [Pg.133]    [Pg.135]    [Pg.136]    [Pg.139]    [Pg.140]    [Pg.120]    [Pg.96]    [Pg.2099]    [Pg.1160]    [Pg.146]    [Pg.353]    [Pg.184]    [Pg.132]    [Pg.2]    [Pg.91]    [Pg.175]    [Pg.691]    [Pg.182]    [Pg.250]    [Pg.12]    [Pg.11]    [Pg.30]    [Pg.34]    [Pg.51]    [Pg.133]    [Pg.256]    [Pg.270]    [Pg.270]    [Pg.287]   
See also in sourсe #XX -- [ Pg.133 , Pg.133 ]




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