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Gravitation particles

These ideas have been applied to gravitational particle creation at the end of inflation by Chung, Kolb Riotto (1998) and Kuzmin Tkachev (1998). Particles with masses M of the order of the Hubble parameter at the end of inflation, Hi 10-6Mpi 1013 GeV, may have been created with a density... [Pg.299]

Figure 3 Schematic filter characteristic of the human respiratory tract for aerosol particles. Three domains can be recognized the domain of deposition decreasing with particle size is solely due to diffusional particle transport, the domain of minimum deposition is due to simultaneous diffusional and gravitational particle transport, and the domain of deposition increasing with particle size due to gravitational and inertial particle transport. Figure 3 Schematic filter characteristic of the human respiratory tract for aerosol particles. Three domains can be recognized the domain of deposition decreasing with particle size is solely due to diffusional particle transport, the domain of minimum deposition is due to simultaneous diffusional and gravitational particle transport, and the domain of deposition increasing with particle size due to gravitational and inertial particle transport.
Very often inertial deposition in impactors is used to characterize the aerodynamic behavior of aerosol particles. However, much larger inertial forces are applied for particle deposition in impactors than are available for particle deposition in the human respiratory tract. The particle size obtained by this technique is the inertial diameter. This diameter is defined in the same way as the aerodynamic diameter but based on inertial rather than gravitational particle transport. When a particle is not only inertially but also gravitationally transported its inertial diameter is identical with its aerodynamic diameter. [Pg.32]

Table 1. Exact and Hartree energies for the system of N equivalent gravitating particles for D = 1 and D oo, and the dimensionally interpolated estimates at D = 3. Table 1. Exact and Hartree energies for the system of N equivalent gravitating particles for D = 1 and D oo, and the dimensionally interpolated estimates at D = 3.
This is the passage about the gravitating particles of nitrous air are thrice the distance from each other that the ultimate particles of dephlogisticated are , quoted on p. 739. [Pg.383]

The charges of repellent matter, by which attractive and gravitating particles form elastic fluids, are distinct atmospheres of fiery matter, in which the densities are reciprocally as the distances from the central particles, in a duplicate or higher ratio. ... [Pg.805]

The decomposition of nitrous air, by the light inflammable air of the hepatic gas [HaS], is equally extraordinary, considering. . . the inflammable air is not in a condensed state and, therefore, combined with its natural portion of fire. Do atmospheres of equal density favour the union of their respective gravitating particles Or, do a... [Pg.807]

Settling velocities for particles of different sizes are given in Table 1. Gravitational particle displacement becomes more effective than diffusional displacement for spheres larger than 0.5 pm. [Pg.238]

Settling and sedimentation. In settling processes, particles are separated from a fluid by gravitational forces acting on the particles. The particles can be solid particles or liquid drops. The fluid can be a liquid or a gas. [Pg.68]

The final and less commonly dealt-with member of the family of electrokinetic phenomena is the sedimentation potential. If charged particles are caused to move relative to the medium as a result, say, of a gravitational or centrifugal field, there again will be an induced potential E. The formula relating to f and other parameters is [72, 77]... [Pg.188]

In the usual situation illustrated in Fig. XIII-6 the particle is supported at a liquid-air interface against gravitational attraction. As was seen, the restoring force... [Pg.473]

Several groups have previously reported parallel implementations of multipole based algorithms for evaluating the electrostatic n-body problem and the related gravitational n-body problem [1, 2]. These methods permit the evaluation of the mutual interaction between n particles in serial time proportional to n logn or even n under certain conditions, with further reductions in computation time from parallel processing. [Pg.459]

CE uses holonomic constraints. In a constrained system the coordinates of the particles 5t independent and the equations of motion in each of the coordinate directions are cted. A second difficulty is that the magnitude of the constraint forces is unknown, in the case of the box on the slope, the gravitational force acting on the box is in the ction whereas the motion is down the slope. The motion is thus not in the same direc-s the gravitational force. As such, the total force on the box can be considered to arise wo sources one due to gravity and the other a constraint force that is perpendicular to otion of the box (Figure 7.8). As there is no motion perpendicular to the surface of the the constraint force does no work. [Pg.386]

An interesting historical application of the Boltzmann equation involves examination of the number density of very small spherical globules of latex suspended in water. The particles are dishibuted in the potential gradient of the gravitational field. If an arbitrary point in the suspension is selected, the number of particles N at height h pm (1 pm= 10 m) above the reference point can be counted with a magnifying lens. In one series of measurements, the number of particles per unit volume of the suspension as a function of h was as shown in Table 3-3. [Pg.74]

Besides particles, the forces of nature play also a key role. In the past century four fundamental forces were recognized the gravitational, electromagnetic, weak, and strong forces. Of these the weak and strong forces are less familiar, because they are nuclear forces and their strength rapidly diminishes over all but subatomic scales. [Pg.9]

With a typical ablated particle size of about 1 -pm diameter, the efficiency of transport of the ablated material is normally about 50% most of the lost material is deposited on contact with cold surfaces or by gravitational deposition. From a practical viewpoint, this deposition may require frequent cleaning of the ablation cell, transfer lines, and plasma torch. [Pg.112]

Since the radial acceleration functions simply as an amplified gravitational acceleration, the particles settle toward the bottom -that is, toward the circumference of the rotor-if the particle density is greater than that of the supporting medium. A distance r from the axis of rotation, the radial acceleration is given by co r, where co is the angular velocity in radians per second. The midpoint of an ultracentrifuge cell is typically about 6.5 cm from the axis of rotation, so at 10,000, 20,000, and 40,000 rpm, respectively, the accelerations are 7.13 X 10, 2.85 X 10 , and 1.14 X 10 m sec" or 7.27 X 10, 2.91 X 10, and 1.16 X 10 times the acceleration of gravity (g s). [Pg.635]

Newton s law of gravitation states that if two particles are a distance r apart, the mutual attraction force between them can be expressed as follows... [Pg.330]

Transport Disengaging Height. When the drag and buoyancy forces exerted by the gas on a particle exceed the gravitational and interparticle forces at the surface of the bed, particles ate thrown into the freeboard. The ejected particles can be coarser and more numerous than the saturation carrying capacity of the gas, and some coarse particles and clusters of fines particles fall back into the bed. Some particles also coUect near the wall and fall back into the fluidized bed. [Pg.79]

Sedimentation (qv) techniques, whether based on gravitational forces or centrifugation, derive the particle size from the measured travel rates of particles in a Hquid. Before the particle analysis is carried out, the sample is usually dispersed in a medium to break down granules, agglomerates, and aggregates. The dispersion process might involve a simple stirring of the powder into a Hquid, but the use of an ultrasonic dispersion is preferred. [Pg.4]


See other pages where Gravitation particles is mentioned: [Pg.42]    [Pg.404]    [Pg.23]    [Pg.23]    [Pg.807]    [Pg.813]    [Pg.739]    [Pg.751]    [Pg.42]    [Pg.404]    [Pg.23]    [Pg.23]    [Pg.807]    [Pg.813]    [Pg.739]    [Pg.751]    [Pg.71]    [Pg.196]    [Pg.354]    [Pg.2673]    [Pg.386]    [Pg.126]    [Pg.120]    [Pg.101]    [Pg.35]    [Pg.4]    [Pg.400]    [Pg.411]    [Pg.412]    [Pg.517]    [Pg.396]    [Pg.396]    [Pg.396]    [Pg.131]    [Pg.131]   
See also in sourсe #XX -- [ Pg.8 ]




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ACCELERATING MOTION OF A PARTICLE IN THE GRAVITATIONAL FIELD

Gravitation

Gravitation settling of particles

Gravitational

Gravitational Settling of an Aerosol Particle

Gravitational field, particle migration

Gravitational particle transport

Gravitational sedimentation, particle sizing

Particle gravitational sedimentation

Particle growth and gravitational sedimentation

Particle size measurement gravitational sedimentation

Particles from gravitational force

Particles gravitational settling

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