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Inertia constant

The inertia constant H for four pole machines varies from about 1.2 MW seconds/MVA for a 1 MVA generator to about 2.5 for a 40 MVA generator. [Pg.79]

Represent all the low voltage motors on a typical motor control centre by one, two or perhaps three equivalent motors to cover the kilowatt range. A typical selection would be 20 kW and 100 kW. The equivalent motor would have the electrical parameters, inertia constant and pump characteristic of the typical machine, but would have the rating of the total of all the motors in the group. [Pg.307]

It does not seem possible to provide a figure of merit for a fluid that possesses these sundry needs, but (see Sect. 6.6) the linear traverse mechanism will demonstrably test total capability in that respect [115]. In this device, two contra-rotating, high-inertia, constant-velocity rotors provide motion somces with HT (high tension) and earth busbars , the excitation being controlled via switches. [Pg.178]

Nonlinear Dynamic Seismic Anaiysis, Tabie 1 Material properties, geometric, inertia constants, and shear deformation coefficients of the rectangular cross section of application section Free Vibrations of Hinged Beam of Rectangular Cross Section ... [Pg.1605]

In this application the free vibrations of Timoshenko beams with very flexible boundary conditions is examined, since in this case the natural frequencies and the corresponding modeshapes are highly sensitive to the effects of shear deformation and rotary inertia (Aristizabal-Ochoa 2004). Thus, the linear free vibration analysis of piimed-free beams of length L = 5.0 m of various cross sections is examined (p = 2.40 tn/m, E = 25.42 GPa, G = 11.05 GPa). In Table 3 the geometric and inertia constants as well as the shear correction factors of the examined cross sections are presented (re = 1/a). The differential equations for the linear free vibrations of this special case can be obtained by Eq. 14 for zero axial stress resultant and external force as... [Pg.1605]

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]

The effective moment of inertia / and the friction coefficient / could easily be estimated. The force constant k associated with the relative motion of the lobes was determined from an empirical energy function. To do so, the molecule was opened in a step-wise fashion by manipulating the hinge region and each resulting structure was energy minimized. Then, the interaction energy between the two domains was measured, and plotted versus 0. [Pg.72]

A number of properties can be computed from various chemical descriptors. These include physical properties, such as surface area, volume, molecular weight, ovality, and moments of inertia. Chemical properties available include boiling point, melting point, critical variables, Henry s law constant, heat capacity, log P, refractivity, and solubility. [Pg.325]

As in diatomic molecules the structure of greatest importance is the equilibrium structure, but one rotational constant can give, at most, only one structural parameter. In a non-linear but planar molecule the out-of-plane principal moment of inertia 4 is related to the other two by... [Pg.132]

The attenuation of ultrasound (acoustic spectroscopy) or high frequency electrical current (dielectric spectroscopy) as it passes through a suspension is different for weU-dispersed individual particles than for floes of those particles because the floes adsorb energy by breakup and reformation as pressure or electrical waves josde them. The degree of attenuation varies with frequency in a manner related to floe breakup and reformation rate constants, which depend on the strength of the interparticle attraction, size, and density (inertia) of the particles, and viscosity of the Hquid. [Pg.549]

Constant in rotational partition function of gases Constant relating wave number and moment of inertia Z = constant relating wave number and energy per mole... [Pg.42]

For conditions approaching constant flow through the orifice, a relationship derivea by equating the buoyant force to the inertia force of the liquid [Davidson et al., Tran.s. In.stn. Chem. Engr.s., 38, 335 (I960)] (dimensionally consistent),... [Pg.1417]

Power to drive a belt conveyor is made up of five components power to drive the empty belt, to move the load against fric tion of the rotating parts, to raise or lower the load, to overcome inertia in putting material into motion, and to operate a belt-driven tripper if required. As with most other conveyor problems, if is advisable to work with formulas and constants from a specific manufacturer in making these calculations. For estimating purposes, typical data are given in Table 21-7. [Pg.1917]

Moment of inertia or stored energy constant, applicable to motors of frame sizes above 315 10% of the guaranteed value... [Pg.269]

Another popular approach to the isothennal (canonical) MD method was shown by Nose [25]. This method for treating the dynamics of a system in contact with a thennal reservoir is to include a degree of freedom that represents that reservoir, so that one can perform deterministic MD at constant temperature by refonnulating the Lagrangian equations of motion for this extended system. We can describe the Nose approach as an illustration of an extended Lagrangian method. Energy is allowed to flow dynamically from the reservoir to the system and back the reservoir has a certain thermal inertia associated with it. However, it is now more common to use the Nose scheme in the implementation of Hoover [26]. [Pg.59]

The purpose of the deceleration mode is to decelerate the unloaded system inertia to near zero rpm in a specified time period. As the e-stop relay switches to the deceleration mode, the brake coil is excited from the battery source at a lower, constant value voltage, which will produce sufficient torque to achieve the rated brake continuous thermal load. The system will then decelerate under a constant torque load. [Pg.269]

AT = average accelerating torque over the speed interval (difference between motor and load torque) g = gravitational constant WR -- torsional moment of inertia... [Pg.274]

Fig. 4.41 Angular positional control system. = Error detector gain (V/rad) K2 = Amplifier gain (A/V) Kj = Motor constant (Nm/A) n = Gear ratio Hi = Tachogenerator constant (Vs/rad) H = Load moment of inertia (kg m ) Q = Load damping coefficient (Nms/rad). Fig. 4.41 Angular positional control system. = Error detector gain (V/rad) K2 = Amplifier gain (A/V) Kj = Motor constant (Nm/A) n = Gear ratio Hi = Tachogenerator constant (Vs/rad) H = Load moment of inertia (kg m ) Q = Load damping coefficient (Nms/rad).
The turbulent regime for Cq is characterized by the section of line almost parallel to the x-axis (at the Re" > 500). In this case, the exponent a is equal to zero. Consequently, viscosity vanishes from equation 46. This indicates that the friction forces are negligible in comparison to inertia forces. Recall that the resistance coefficient is nearly constant at a value of 0.44. Substituting for the critical Reynolds number, Re > 500, into equations 65 and 68, the second critical values of the sedimentation numbers are obtained ... [Pg.298]

Usually this type of anemometer does not provide information on the flow direction. Vice versa, the. sensors are made as independent of the flow direction as possible—omnidirectional. This is an advantage for free-space ventilation measurements, as the flow direction varies constantly and a direction-sensitive anemometer would be difficult to use. Naturally, no sensor is fully omnidirectional, but satisfactory constructions are available. Due to the high sensor thermal inertia, this type of anemometer is unsuitable for high-frequency flow fluctuation measurement. They can be used to monitor low-frequency turbulence up to a given cut-off frequency, which depends on the dynamic properties of the instrument. [Pg.1154]

An even more difficult problem occurs if the bar is not prismatic, i.e., if the moment of inertia is not constant along the length. We must then solve for l(x) where x is the axial coordinate of the bar. This optimization of cross-section distribution has been addressed only for problems with fixed E and L, not the general column design problem. [Pg.375]


See other pages where Inertia constant is mentioned: [Pg.1245]    [Pg.548]    [Pg.56]    [Pg.57]    [Pg.306]    [Pg.362]    [Pg.194]    [Pg.202]    [Pg.124]    [Pg.1605]    [Pg.61]    [Pg.1245]    [Pg.548]    [Pg.56]    [Pg.57]    [Pg.306]    [Pg.362]    [Pg.194]    [Pg.202]    [Pg.124]    [Pg.1605]    [Pg.61]    [Pg.119]    [Pg.1153]    [Pg.2441]    [Pg.2441]    [Pg.511]    [Pg.132]    [Pg.292]    [Pg.67]    [Pg.403]    [Pg.761]    [Pg.781]    [Pg.883]    [Pg.1337]    [Pg.1417]    [Pg.2481]    [Pg.102]    [Pg.84]   
See also in sourсe #XX -- [ Pg.54 , Pg.78 , Pg.306 ]




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