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Moment of inertia, equations

The only tenn in this expression that we have not already seen is a, the vibration-rotation coupling constant. It accounts for the fact that as the molecule vibrates, its bond length changes which in turn changes the moment of inertia. Equation B1.2.2 can be simplified by combming the vibration-rotation constant with the rotational constant, yielding a vibrational-level-dependent rotational constant. [Pg.1153]

It should be stressed here also that all the moment of inertia equations above deal with a collection of point masses with fixed positions. They also specify properties of a vibrating molecule (a collection of point mass atoms) at some instant in time, or at some point (perh s fictitious) in 3N-6 (or 5) dimensional space at which the atoms are motionless, such as the equilibrium position. [Pg.9]

To first order, the 7 moments are equal to the equilibrium moments of inertia 7 . The above procedure is repeated for another parent species. Once a sufficient number of 7 for different parent isotopic species have been determined, the moment-of-inertia equations may be solved to give the structure. The structure for SO2 is given in Table XVIII. This measure of the molecular structure has limited applicability because of the large amount of precise isotopic moment-of-inertia data required and because the first-order approximation 7 = 7 is not sufficient especially for light atoms. Thus, hydrogen bond lengths cannot be determined by this method. [Pg.320]

Equation XVI-21 provides for the general case of a molecule having n independent ways of rotation and a moment of inertia 7 that, for an asymmetric molecule, is the (geometric) mean of the principal moments. The quantity a is the symmetry number, or the number of indistinguishable positions into which the molecule can be turned by rotations. The rotational energy and entropy are [66,67]... [Pg.583]

Their moment of inertia is kept low to restrict their times of acceleration and deceleration (equation (2.. t)) to facilitate frequent starts and stops,... [Pg.176]

Component reliability will vary as a function of the power of a dimensional variable in a stress function. Powers of dimensional variables greater than unity magnify the effect. For example, the equation for the polar moment of area for a circular shaft varies as the fourth power of the diameter. Other similar cases liable to dimensional variation effects include the radius of gyration, cross-sectional area and moment of inertia properties. Such variations affect stability, deflection, strains and angular twists as well as stresses levels (Haugen, 1980). It can be seen that variations in tolerance may be of importance for critical components which need to be designed to a high reliability (Bury, 1974). [Pg.163]

In equation (2.17) / is the moment of inertia about the rotational axis. [Pg.17]

A flywheel of moment of inertia / sits in bearings that produee a frietional moment of C times the angular veloeity uj t) of the shaft as shown in Figure 2.7. Find the differential equation relating the applied torque T t) and the angular veloeity uj t). [Pg.19]

Figure 2.8 shows a reduetion gearbox being driven by a motor that develops a torque T tn(t). It has a gear reduetion ratio of and the moments of inertia on the motor and output shafts are and /q, and the respeetive damping eoeffieients Cm and Cq. Find the differential equation relating the motor torque CmfO and the output angular position 6a t). [Pg.19]

The laser-guided missile shown in Figure 2.19 has a piteh moment of inertia of 90kgm. The eontrol fins produee a moment about the piteh mass eentre of 360 Nm per radian of fin angle (3 t). The fin positional eontrol system is deseribed by the differential equation... [Pg.32]

However, four different moments of inertia for each of the four different materials (hence different moduli of elasticity) are obtained from Equation (7.2). Moreover, knowing the moment of inertia of a column does not teli us the shape or dimensions of a column We usually select a column... [Pg.374]

The left-hand side of the second equation of (6-186) is the pendulum equation (J being the moment of inertia, D, the coefficient of damping and C, the coefficient of the restoring moment). [Pg.382]

For diatomic molecules, B0 is the rotational constant to use with equation (10.125), while Be applies to equation (10.124). They are related by Bq = Be 2 - The moment of inertia 70(kg-m2) is related to 50(cm ) through the relationship /0 = h/ 8 x 10 27r22 oc), with h and c expressed in SI units. For polyatomic molecules, /a, /b, and Iq are the moments of inertia to use with Table 10.4 where the rigid rotator approximation is assumed. For diatomic molecules, /0 is used with Table 10.4 to calculate values to which we add the anharmonicity and nonrigid rotator corrections. [Pg.503]

In terms of principal moments of inertia A, B and G, and the molecular mass M, the entropy term is then given by equation (14) (cf. also Leffek and Matheson, 1971). [Pg.10]

US denote by A and C the moments of inertia with respect to the axis, lying in the plane of an equator and the polar axis, respectively. The ratio... [Pg.158]

This is an equation of rotation of an elementary mass around the y-axis. Here r can be treated as the moment of inertia of the unit mass and dco/dt is the angular acceleration. The product gx characterizes the torque with respect to the point 0. Multiplying Equation (3.49) by dm and performing integration over the pendulum mass, we obtain... [Pg.176]

The integral at the left hand side of Equation (3.50) represents the moment of inertia of the pendulum ... [Pg.177]

The integral on the right hand side represents the moment of inertia of the pendulum with respect to the axis passing through the center of gravity, and Equation (3.55) describes the well-known theorem of mechanics. Bearing in mind that, we already introduced the reduced length /, (Equation (3.54)), let us assume... [Pg.178]

Here I — ma is moment of inertia, a angular acceleration, and z the resultant moment. Note that we have neglected attenuation but in reality, of course, it is always present. This equation characterizes a motion for any angle a, but we consider only the vicinity of points of equilibrium. For this reason, the resultant moment in the linear approximation can be represented as... [Pg.203]


See other pages where Moment of inertia, equations is mentioned: [Pg.205]    [Pg.6107]    [Pg.6106]    [Pg.205]    [Pg.6107]    [Pg.6106]    [Pg.2077]    [Pg.502]    [Pg.511]    [Pg.21]    [Pg.106]    [Pg.132]    [Pg.140]    [Pg.123]    [Pg.33]    [Pg.374]    [Pg.375]    [Pg.427]    [Pg.163]    [Pg.142]    [Pg.142]    [Pg.167]    [Pg.177]    [Pg.536]    [Pg.783]    [Pg.783]    [Pg.789]    [Pg.10]    [Pg.55]    [Pg.113]    [Pg.177]    [Pg.214]   
See also in sourсe #XX -- [ Pg.223 , Pg.229 ]




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Moment equations

Moment of inertia

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