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Axis of rotation

The divergent shape of the beam provides facilities for magnification in the distances of the source to detector and of the sources to the axis of rotation, which used in conjunction with a microfocus x-ray source opens the way to high resolution. [Pg.217]

The obvious way to form a similarity between the Wigner rotation matrix and the adiabatic-to-diabatic transformation mabix defined in Eqs. (28) is to consider the (unbreakable) multidegeneracy case that is based, just like Wigner rotation matrix, on a single axis of rotation. For this sake, we consider the particular set of T matrices as defined in Eq. (51) and derive the relevant adiabatic-to-diabatic transfonnation matrices. In what follows, the degree of similarity between the two types of matrices will be presented for three special cases, namely, the two-state case which in Wigner s notation is the case, j =, the tri-state case (i.e.,7 = 1) and the tetra-state case (i.e.,7 = ). [Pg.686]

For a body that consists of n masses mj, each separated by a distance rj from the axis of rotation of the array, the radius of gyration is defined... [Pg.52]

There exists some radial distance from the axis of rotation at which all of the mass could be concentrated to produce the same moment of inertia that the actual distribution of mass possesses. This distance is defined to be the radius of gyration. According to this definition,... [Pg.53]

The ellipsoid of revolution is swept out by rotating an ellipse along its major or minor axis. When the major axis is the axis of rotation, the resulting rodlike figure is said to be prolate when the minor axis is the axis of rotation, the disklike figure is said to be oblate. [Pg.595]

We designate the length of the ellipsoid along the axis of rotation as 2a and the equatorial diameter as 2b to define the axial ratio a/b which characterizes the ellipticity of the particle. By this definition, a/b > 1 corresponds to prolate ellipsoids, and a/b < 1 to oblate ellipsoids. [Pg.595]

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]

In most rotational viscometers the rate of shear varies with the distance from a wall or the axis of rotation. However, in a cone—plate viscometer the rate of shear across the conical gap is essentially constant because the linear velocity and the gap between the cone and the plate both increase with increasing distance from the axis. No tedious correction calculations are required for non-Newtonian fluids. The relevant equations for viscosity, shear stress, and shear rate at small angles a of Newtonian fluids are equations 29, 30, and 31, respectively, where M is the torque, R the radius of the cone, v the linear velocity, and rthe distance from the axis. [Pg.186]

The Bottle Centrifuge. Analysis of the performance of a botde centrifuge is based on the model shown in Figure 1. A soHd or Hquid particle is considered in an initial position, X, at a radius, r, from the axis of rotation. If equation 2 is appHed to this specific particle, assuming that = dr/dt then... [Pg.396]

When experimental data are not available, methods of estimation based on statistical mechanics are employed (7,19). Classical kinetic theory suggests a contribution to CP of S R for each translational degree of freedom in the molecule, a contribution of S R for each axis of rotation, and of R for each vibrational degree of freedom. A cmde estimate of CP for small molecules can be obtained which neglects vibrational degrees of freedom ... [Pg.235]

Effect of Fluid Viscosity and Inertia The dynamic effect of viscosity on a rotating liquid slurry as found in a sedimenting centrifuge is confined in veiy thin fluid layers, known as Ekman layers. These layers are adjacent to rotating surfaces which are perpendicular to the axis of rotation, such as bowl heads, flanges, and conveyor blades, etc. The thickness of the Ekman layer 6 is of the order... [Pg.1725]

The bowl is suspended from an upper bearing and drive (electric or turbine motor) assembly through a flexible-drive spindle with a loose guide in a controlled damping assembly at the bottom. The unit finds its axis of rotation if it becomes slightly unbalanced due to process load. [Pg.1730]

L. Vibrational conveyance. This is referred as the vibratory centrifuge. A relatively bign frequency force is superimposed on the rotating assembly. This can be either in-line with the axis of rotation or torsional, around the drivesbaft. In either case, the cake under inertial force from the vibration is partly fluidized and propelled down the screen under a somewhat steady pace toward the large end, where it is discharged. [Pg.1738]

If supported by journal bearings, the shaft may describe an orbit so that the axis of rotation itself rotates about the geometric center of the bearings. [Pg.192]

Wake-mixing loss. This loss is from the impeller blades, and it causes a wake in the vaneless space behind the rotor. It is minimized in a diffuser, which is symmetric around the axis of rotation. [Pg.253]

Figure 11.3 illustrates the classification of the MOs of butadiene and cyclobutene. There are two elements of symmetry that are common to both s-cw-butadiene and cyclobutene. These are a plane of symmetry and a twofold axis of rotation. The plane of symmetry is maintained during a disrotatory transformation of butadiene to cyclobutene. In the conrotatory transformation, the axis of rotation is maintained throughout the process. Therefore, to analyze the disrotatory process, the orbitals must be classified with respect to the plane of symmetry, and to analyze the conrotatory process, they must be classified with respect to the axis of rotation. [Pg.610]


See other pages where Axis of rotation is mentioned: [Pg.215]    [Pg.188]    [Pg.1829]    [Pg.2040]    [Pg.685]    [Pg.635]    [Pg.113]    [Pg.257]    [Pg.413]    [Pg.399]    [Pg.407]    [Pg.407]    [Pg.409]    [Pg.91]    [Pg.474]    [Pg.902]    [Pg.1554]    [Pg.1724]    [Pg.1724]    [Pg.1729]    [Pg.1735]    [Pg.1736]    [Pg.1737]    [Pg.1738]    [Pg.1781]    [Pg.223]    [Pg.587]    [Pg.598]    [Pg.10]    [Pg.195]    [Pg.430]    [Pg.430]    [Pg.431]    [Pg.433]    [Pg.465]   
See also in sourсe #XX -- [ Pg.46 ]

See also in sourсe #XX -- [ Pg.3 , Pg.6 , Pg.50 ]

See also in sourсe #XX -- [ Pg.692 ]

See also in sourсe #XX -- [ Pg.45 ]




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Axis of rotation-reflection

Axis of symmetry rotational

Axis of symmetry, rotation about

C2 axis of rotation

C3 axis of rotation

Fold rotation-reflection axis of symmetry

Improper axis of rotation

Instantaneous axis of rotation

Principal axis of rotation

Rotation about an -fold axis of symmetry

Rotation axis

Rotation-reflection axis of symmetry

S , axis of rotation

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