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Damping bands

As previously mentioned, auxiliary bearings are used to proteet eleetromeehanieal parts in ease of bearing overload or eleetronie failure. These auxiliary bearings are used for both radial and axial motion and are mounted on damping bands. The maximum air gap between the shaft and the auxiliary bearings is 0.25 mm (.010 in.) radial and 0.30 mm (.012 in.) axial, ineluding band defleetion of 0.07 mm (.003 in.). [Pg.459]

Figure 14.13 Typical broad band floor response spectra showing the floor acceleration at different damping levels... Figure 14.13 Typical broad band floor response spectra showing the floor acceleration at different damping levels...
Another area of concern is the Q of the filter at self-resonance. If the Q is too high, or in other words, the damping factor is too low, the filter will actually generate noise in the form of narrow-band ringing. This can be dealt with during the design. [Pg.246]

Most of the forcing functions generated by V-belt drives can be attributed to the elastic or mbber band effect of the belt material. This elasticity is needed to provide the traction required transmitting power from the drive sheave (i.e., pulley) to the driven sheave. Elasticity causes belts to act like springs, increasing vibration in the direction of belt wrap, but damping it in the opposite direction. As a result, belt elasticity tends to accelerate wear and the failure rate of both the driver and driven unit. [Pg.705]

We may observe that the two sub-bands of the damped spectral density (110), as well as the two peaks involved by the undamped case, must be of the same intensity in the resonant case (A = 0), which may be verified by looking at the... [Pg.277]

When the direct damping of the fast mode is strong, with that of the bending mode being weak, the lineshape (c) shows a broad shape involving a window that is due to the band splitting. [Pg.283]

Figure 12. Hydrogen bond involving a Fermi resonance damping parameters switching the intensities. The lineshapes were computed within the adiabatic and exchange approximations. Intensities balancing between two sub-bands are observed when modifying the damping parameters (a) with y0 =0.1, and y5 = 0.8 (b) with ya = ys = 0.8 (c) with yB — 0.8 and ys — 0.1. Common parameters oto = 1, A = 150cm, 2g)5 = 2850cm-1, and T = 30 K. Figure 12. Hydrogen bond involving a Fermi resonance damping parameters switching the intensities. The lineshapes were computed within the adiabatic and exchange approximations. Intensities balancing between two sub-bands are observed when modifying the damping parameters (a) with y0 =0.1, and y5 = 0.8 (b) with ya = ys = 0.8 (c) with yB — 0.8 and ys — 0.1. Common parameters oto = 1, A = 150cm, 2g)5 = 2850cm-1, and T = 30 K.
If the experimental lineshapes do not exhibit sub-bands and are asymmetric, or if they involve sub-bands, but with intensity anomalies with respect to the Franck-Condon progression law, then, together with the dephasing mechanism, damping of the slow mode ought to be also considered as occurring in a sensitive competitive way. [Pg.304]

A proportional plus integral controller is used to control the level in the reflux accumulator of a distillation column by regulating the top product flowrate. At time t = 0, the desired value of the flow controller which is controlling the reflux is increased by 3 x 10-4 m3/s. If the integral action time of the level controller is half the value which would give a critically damped response and the proportional band is 50 per cent, obtain an expression for the resulting change in level. [Pg.329]

Finally, it should be mentioned that neither the ideal metal model nor the damped metal model are able to explain why the actual reflectivity of aluminum is lower than the calculated one (iC >= 1) at frequencies lower than cop. Also, these simple models do not reproduce features such as the reflectivity dip observed around 1.5 eV. In order to account for these aspects, and then to have a better understanding of real metals, the band structure must be taken into account. This will be discussed at the end of this chapter, in Section 4.8. [Pg.127]

Sodium (Na) gas shows two well-defined absorption bands that peak at 589 nm and 589.6 nm. Consider this gas as a diluted medium (so that n 1), with a density of ions of N = 1 x 10" cm and a damping rate of F = 628 MHz. (a) Estimate the absorption coefficient at these two peaks, (b) Now estimate the power of a laser beam of 1 mW at 589.0 nm after it passes through a Na cell of thickness 5 cm. [Pg.147]

Active from spring to fall, snails usually hide under shrubs and In cool, damp places during the day. They feed at night especially during damp weather. The garden snail Is the most common pest with a gray-brown shell up to I A In (3 cm) across. Banded snails are not normally a serious pest Their shells have white, yellow, gray, or pink bands with darker stripes, or are sometimes entirely pale yellow. [Pg.338]

By considering the extreme case of a crystal completely covered by a layer of foreign atoms, we have already seen in Sec. III,B that, if chemisorption involves the formation of localized electron pair bonds, some interesting interaction effects are to be expected. In this section, we approach the problem from the other extreme by considering just two atoms chemisorbed on a crystal surface. If the localized level formed by the interaction does not lie too far below the normal crystal band (or any surface band), the wave function for the localized level is damped only slowly in the crystal. Therefore, two chemisorbed atoms will be in interaction at distances when the interaction between the isolated atoms would be entirely negligible. To investigate this effect, we take the simplest model which may be expected to yield useful results 11). The crystal is represented by a straight... [Pg.13]


See other pages where Damping bands is mentioned: [Pg.481]    [Pg.372]    [Pg.428]    [Pg.565]    [Pg.481]    [Pg.372]    [Pg.428]    [Pg.565]    [Pg.2221]    [Pg.449]    [Pg.445]    [Pg.562]    [Pg.71]    [Pg.222]    [Pg.520]    [Pg.113]    [Pg.89]    [Pg.278]    [Pg.281]    [Pg.395]    [Pg.222]    [Pg.283]    [Pg.283]    [Pg.303]    [Pg.304]    [Pg.304]    [Pg.306]    [Pg.491]    [Pg.152]    [Pg.368]    [Pg.11]    [Pg.157]    [Pg.145]    [Pg.26]    [Pg.249]    [Pg.347]    [Pg.75]    [Pg.4]    [Pg.9]    [Pg.719]   
See also in sourсe #XX -- [ Pg.459 ]




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