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Mass rotation

To achieve a vibration level off) micron in a rotating mass is practically impossible. It will possess some runout, however precisely and accurately it has been balanced. While rotating, therefore, the shaft on which the other masses rotate, will deflect to the side which is heavier and the opacity around the centre of the shaft wiii become uneven. The masses wiii rotate in smail cireies about their own geometrical axis rather than the axis of the shaft. [Pg.157]

Next we consider systems in which a mass rotates, and start from the simplest case. [Pg.200]

Microwave spectra Calculation of reduced mass, rotational constant, bond... [Pg.83]

The volumetric rotational flow term (Q ) depends on the several geometric parameters and rotation speed. Since most extruder rates are measured in mass per unit time, the term is defined as the mass rotational flow ... [Pg.13]

Dimension of mass Rotational speed Pressure, pressure difference Power... [Pg.53]

If adequate spectral resolution is available, infrared spectra of molecules in the gas phase can be highly structured. The varying molecular complexity and symmetry makes it necessary to employ different models for spectrum interpretation. These models may be characterized by considering the molecular moments of inertia. Generally, the moment of inertia la of a rigid body with n point masses rotating about the axis ri is defined as... [Pg.258]

There is, however, a number of instabilities that induce vortices, and these can delay the onset of the mass rotation condition. The next section will discuss the cause of these instabilities. [Pg.2886]

Enhancement of annular gap instabilities. The instability of the previous section will be suppressed by higher viscosities, again reverting to mass rotation. There are different methods used to overcome this with varying degrees of success ... [Pg.2888]

For a complete treatment of a laser-driven molecule, one must solve the many-body, multidimensional time-dependent Schrodinger equation (TDSE). This represents a tremendous task and direct wavepacket simulations of nuclear and electronic motions under an intense laser pulse is presently restricted to a few bodies (at most three or four) and/or to a model of low dimensionality [27]. For a more general treatment, an approximate separation of variables between electrons (fast subsystem) and nuclei (slow subsystem) is customarily made, in the spirit of the BO approximation. To lay out the ideas underlying this approximation as adapted to field-driven molecular dynamics, we will consider from now on a molecule consisting of Nn nuclei (labeled a, p,...) and Ne electrons (labeled /, j,...), with position vectors Ro, and r respectively, defined in the center of mass (rotating) body-fixed coordinate system, in a classical field E(f) of the form Eof t) cos cot). The full semiclassical length gauge Hamiltonian is written, for a system of electrons and nuclei, as [4]... [Pg.55]

Intensified mass Rotation, vibration. Many processes 3... [Pg.45]

We have seen that the two-particle system of an electron and a nucleus rotating about a center of mass (COM) can be transformed to the one-particle system of a reduced mass rotating about a fixed point. However, this transformation can be made for any two-mass system, and so it applies also to the case of the nuclei of a rotating diatomic molecule. As we now show, the mathematical outcome for the rotating diatomic molecule is strikingly similar to that for the hydrogenlike ion. [Pg.117]

All three may be coupled if the molecules are not centrosymmetric, a rotation of their orientation will in most cases be accompanied by a shift of their center of mass and if the center of mass rotates, tilting is favored. [Pg.360]

Fig. 1.11. Wavefunctions and probability functions for a small mass rotating in a circle on a hypothetical guide wire. ... Fig. 1.11. Wavefunctions and probability functions for a small mass rotating in a circle on a hypothetical guide wire. ...
When further analysing the results, it was assumed that a change in the feed mass, rotations fiiequency and mass of the balls were the only process variables which had been estimated. TTie analysis was carried out for steel and corundum balls separately. [Pg.678]


See other pages where Mass rotation is mentioned: [Pg.106]    [Pg.342]    [Pg.14]    [Pg.155]    [Pg.202]    [Pg.203]    [Pg.22]    [Pg.322]    [Pg.280]    [Pg.485]    [Pg.745]    [Pg.2886]    [Pg.300]    [Pg.110]    [Pg.110]    [Pg.745]    [Pg.271]    [Pg.355]    [Pg.116]    [Pg.136]    [Pg.28]    [Pg.36]   
See also in sourсe #XX -- [ Pg.5 , Pg.479 ]




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Equation of mass rotation

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Mass transfer rotating cylinder

Mass transfer rotating disk

Non-Adiabatic Rotational and Vibrational Reduced Masses

Rotating disc electrode mass transfer control

Rotating disk electrode mass transfer

Rotating disk electrode steady-state mass transfer

Rotating mass transport

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