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Gravitational radius

Since we have modeled that the gravitational source is a spherical black-hole-like object, see details in [7, 9], it follows that angular momentum is a constant of motion and postulating the limit velocity c at the limiting distance given by the gravitational radius //, one obtains... [Pg.80]

Hence one concludes, identifying /( with the gravitational radius and / with the gravitational constant, i.e. [Pg.127]

Above we have postulated the limit velocity c at the limiting distance given by the gravitational radius jU. Eq. 1.75 serves as a boundary condition for the operator matrix model. With the replacement vjc= K(r), our complex symmetric representation, reads (given that if(r) < j, see below)... [Pg.24]

There are a number of relatively simple experiments with soap films that illustrate beautifully some of the implications of the Young-Laplace equation. Two of these have already been mentioned. Neglecting gravitational effects, a film stretched across a frame as in Fig. II-1 will be planar because the pressure is the same as both sides of the film. The experiment depicted in Fig. II-2 illustrates the relation between the pressure inside a spherical soap bubble and its radius of curvature by attaching a manometer, AP could be measured directly. [Pg.8]

Figure 9.5a shows a portion of a cylindrical capillary of radius R and length 1. We measure the general distance from the center axis of the liquid in the capillary in terms of the variable r and consider specifically the cylindrical shell of thickness dr designated by the broken line in Fig. 9.5a. In general, gravitational, pressure, and viscous forces act on such a volume element, with the viscous forces depending on the velocity gradient in the liquid. Our first task, then, is to examine how the velocity of flow in a cylindrical shell such as this varies with the radius of the shell. Figure 9.5a shows a portion of a cylindrical capillary of radius R and length 1. We measure the general distance from the center axis of the liquid in the capillary in terms of the variable r and consider specifically the cylindrical shell of thickness dr designated by the broken line in Fig. 9.5a. In general, gravitational, pressure, and viscous forces act on such a volume element, with the viscous forces depending on the velocity gradient in the liquid. Our first task, then, is to examine how the velocity of flow in a cylindrical shell such as this varies with the radius of the shell.
Falling ball viscometers are based on Stokes law, which relates the viscosity of a Newtonian fluid to the velocity of the falling sphere. If a sphere is allowed to fall freely through a fluid, it accelerates until the viscous force is exactly the same as the gravitational force. The Stokes equation relating viscosity to the fall of a soHd body through a Hquid may be written as equation 34, where ris the radius of the sphere and d are the density of the sphere and the hquid, respectively g is the gravitational force and p is the velocity of the sphere. [Pg.190]

Since the gravitational constant is extremely small, it is natural to expect that the force of interaction is also very small too. For illustration, consider two spheres with radius Im and mass 31.4x10 kg made from galena, with the distance between their centers 10 m. Then, the force of interaction, Equation (1.1), is... [Pg.3]

By definition, the angle between the z-axis and the radius vector R is equal to 6. At the same time, the gravitational field can be represented as a sum of the attraction force and centrifugal one, and it is almost opposite to the radius vector. Therefore, the radial component of the field is... [Pg.105]

Increasing the radius of the suspended particles, Brownian motion becomes less important and sedimentation becomes more dominant. These larger particles therefore settle gradually under gravitational forces. The basic equation describing the sedimentation of spherical, monodisperse particles in a suspension is Stokes law. It states that the velocity of sedimentation, v, can be calculated as follows ... [Pg.261]

The terms in Eq. (6) include the gravitational constant, g, the tube radius, R, the fluid viscosity, p, the solute concentration in the donor phase, C0, and the penetration depth, The density difference between the solution and solvent (ps - p0) is critical to the calculation of a. Thus, this method is dependent upon accurate measurement of density values and close temperature control, particularly when C0 represents a dilute solution. This method has been shown to be sensitive to different diffusion coefficients for various ionic species of citrate and phosphate [5], The variability of this method in terms of the coefficient of variation ranged from 19% for glycine to 2.9% for ortho-aminobenzoic acid. [Pg.107]

A gravitationally massive object (allegedly) from which fight cannot escape. The Schwarzschild radius is the radius of the black hole that defines the event horizon the distance at which fight cannot escape... [Pg.110]


See other pages where Gravitational radius is mentioned: [Pg.15]    [Pg.79]    [Pg.127]    [Pg.128]    [Pg.130]    [Pg.276]    [Pg.178]    [Pg.77]    [Pg.78]    [Pg.9]    [Pg.9]    [Pg.38]    [Pg.23]    [Pg.15]    [Pg.79]    [Pg.127]    [Pg.128]    [Pg.130]    [Pg.276]    [Pg.178]    [Pg.77]    [Pg.78]    [Pg.9]    [Pg.9]    [Pg.38]    [Pg.23]    [Pg.4]    [Pg.261]    [Pg.131]    [Pg.35]    [Pg.138]    [Pg.638]    [Pg.1728]    [Pg.1729]    [Pg.1826]    [Pg.161]    [Pg.448]    [Pg.531]    [Pg.1481]    [Pg.655]    [Pg.313]    [Pg.20]    [Pg.276]    [Pg.65]    [Pg.163]    [Pg.169]    [Pg.153]    [Pg.446]    [Pg.107]    [Pg.273]    [Pg.107]   
See also in sourсe #XX -- [ Pg.127 , Pg.130 ]

See also in sourсe #XX -- [ Pg.9 , Pg.38 ]




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Gravitation

Gravitational

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