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Moment-of-momentum

Angular Momentum (Moment of Momentum). Angular momentum is linear momentum (kg-m/s) times moment arm (m). Its SI unit is kg-m /s. For a rotating body the total angular momentum is equal to the moment of inertia I (kg-m ) times the angular velocity CO (rad/s or 1/s). [Pg.310]

Macroscopic and Microscopic Balances Three postulates, regarded as laws of physics, are fundamental in fluid mechanics. These are conservation of mass, conservation of momentum, and con-servation of energy. In addition, two other postulates, conservation of moment of momentum (angular momentum) and the entropy inequality (second law of thermodynamics) have occasional use. The conservation principles may be applied either to material systems or to control volumes in space. Most often, control volumes are used. The control volumes may be either of finite or differential size, resulting in either algebraic or differential consei vation equations, respectively. These are often called macroscopic and microscopic balance equations. [Pg.632]

Balance equations for angular momentum, or moment of momentum, may also be written. They are used less frequently than the lin-... [Pg.632]

Since the momentum density is related to the reciprocal form factor or internally folded density by a Fourier transform, Eq. (5.29), there are sum rules that connect moments of momentum with the spherical average of B f) defined by... [Pg.318]

Other moments of momentum can also be obtained directly from the Compton profile without first going through the numerical differentiation of Eq. (5.64), which is prone to roundoff and truncation errors. In particular, several groups [9,188-191] independently reported one or more of the sum rules... [Pg.320]

Balance equations for angular momentum, or moment of momentum, may also be written. They are used less frequently than the linear momentum equations. See Whitaker (Introduction to Fluid Mechanics, Prentice-Hall, Englewood Cliffs, N.J., 1968, Krieger, Huntington, N.Y., 1981) or Shames (Mechanics of Fluids, 3d ed., McGraw-Hill, New York, 1992). [Pg.7]

Therefore this work concerns the formulation of a proposal for the thermochemistry of an immiscible mixture of reacting materials with microstructure in presence of diffusion a new form of the integral balance of moment of momentum appears in the theory, in which the presence of the microstructure is taken into account. Moreover, the density fields can no longer be regarded as determined by the deformation fields because chemical reactions are present,... [Pg.183]

If one performs the vector operation x x (equations of motion), the balance of rotational momentum or moment of momentum about an axis of rotation is obtained. It is this equation that forms the basis of design of rotating machinery such as centrifugal pumps and turbomachinery. [Pg.255]

Suspended spherical particles, each containing a permanently embedded dipole (e.g., magnetic), are unable to freely rotate (Brenner, 1984 Sellers and Brenner, 1989) in response to the shear and/or vorticity field that they are subjected to whenever a complementary external (e.g., magnetic) field acts on them. This hindered rotation results from the tendency of the dipole to align itself parallel to the external field because of the creation of a couple arising from any orientational misalignment between the directions of the dipole and external field. In accordance with Cauchy s moment-of-momentum equation for continua, these couples in turn give rise to an antisymmetric state of stress in the dipolar suspension, representable as the pseudovector Tx = — e Ta of the antisymmetric portion Ja — (T — Tf) of the deviatoric stress T = P + Ip. [Pg.66]

In passing, we note that Eq. (7) involves the evaluation of a moment of momentum, defined in general as... [Pg.88]

Of special importance is the formula for the angular momentum (or, in other words, the moment of momentum) of the electron about the nucleus from the two preceding formulae it follows that... [Pg.99]

The relation thus formulated is capable of immediate generalization. Consider in the first place, as an example with one degree of freedom, the case already treated above (p. 100), that of the rotator. Here the co-ordinate is the azimuth q== (f>y to which belongs, as canonically conjugated quantity, the angular momentum (or, in other words, the moment of momentum) p. In the free rotation p is constant, i.e. independent of the angle turned through. Thus... [Pg.103]

Angular Momentum (Moment of Momentum) in Wave Mechanics. [Pg.127]

Moreover the balance laws of moment of momentum are, by applying the conservation law of rotational momentum. [Pg.538]

If we denote by T, Cauchy s stress tensor of our material and by b, the density of body forces, then by Truesdell s third principle the balances of linear momentum and of moment of momentum for the whole mixture in local form turn out to be... [Pg.538]

There is one important question why are tectonic stresses changing relatively slowly as we can see in the field Definitely, there is a special mechanism of their redistribution typical for a wave energy transfer in a cataclastic medium. Its elements (blocks) can rotate. This adds the balance of the moment of momentum to the conventional impulse balance equations as well as spin (surplus) velocity of an individual block. The constitutive laws were suggested (Nikolaevskiy, 1996), that led to the Sin-Goidon equation with its soliton solution. [Pg.729]

This equation, often referred to as the moment-of-momentum equation is one of the basic tools in the analysis of rotating fluid machines, turbines, pumps, and other devices [5]. In the steady-state flow dLldt) is zero and equals m p.so we have... [Pg.271]

Axiality of w is automatically achieved by the usual transformation ((c) in Rem. 4) of tensor W. Therefore the skew-symmetric tensors instead of axial vectors and outer product (see Rem. 16) may be used and we do it this way at the moment of momentum balances in the Sects. 3.3,4.3, cf. [7, 8, 14, 27]. Generalization of this Lemma to third-order tensors, made by M. Silhav, is published in Appendix of [28]. [Pg.79]

Balances of Mass, Momentum, tind Moment of Momentum... [Pg.91]

To formulate another main principle—the balance of moment of momentum—we introduce for some part of body (or body itself) with material volume V in actual configuration of the considered frame the moment of momentum or angular moment related to the point y as follows ... [Pg.91]

To obtain a simple form of the balance of moment of momentum, we confine its formulation to inertial frame with angular moment (3.88) having point y fixed here (although we use here the inertial frame fixed with distant stars, resulting formulations are valid in any inertial frame as will be shown at the end of this section). Again, the main reason for that is the nonobjectivity of x, y, v in (3.88), cf. (3.25), (3.38) generalization of this balance in the arbitrary frame will be discussed below but we note that the main local result—symmetry of stress tensor (3.93) below—is valid in the arbitrary frame. [Pg.92]


See other pages where Moment-of-momentum is mentioned: [Pg.107]    [Pg.127]    [Pg.171]    [Pg.330]    [Pg.337]    [Pg.337]    [Pg.43]    [Pg.67]    [Pg.3]    [Pg.99]    [Pg.80]    [Pg.538]    [Pg.636]    [Pg.1]    [Pg.86]    [Pg.87]    [Pg.89]   
See also in sourсe #XX -- [ Pg.43 ]




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