Complete balancing of a disk mounted on a vertical cantilever shaft using a two ball automatic balancer

2006 ◽  
Vol 290 (1-2) ◽  
pp. 169-191 ◽  
Author(s):  
C. Rajalingham ◽  
R.B. Bhat
Keyword(s):  
1992 ◽  
Vol 114 (3) ◽  
pp. 326-329 ◽  
Author(s):  
Lien-Wen Chen ◽  
Der-Ming Ku

The dynamic stability behavior of a cantilever shaft-disk system subjected to axial periodic forces varying with time is studied by the finite element method. The equations of motion for such a system are formulated using deformation shape functions developed from Timoshenko beam theory. The effects of translational and rotatory inertia, gyroscopic moment, bending and shear deformation are included in the mathematical model. Numerical results show that the effect of the gyroscopic term is to shift the boundaries of the regions of dynamic instability outwardly and, therefore, the sizes of these regions are enlarged as the rotational speed increases.


2017 ◽  
Vol 4 (2) ◽  
pp. 1366-1374 ◽  
Author(s):  
Dinesh Satpute ◽  
Prasad Baviskar ◽  
Pritesh Gandhi ◽  
Mayur Chavanke ◽  
Tejas Aher

1966 ◽  
Vol 17 (2) ◽  
pp. 127-140 ◽  
Author(s):  
A. V. Krishna Murty

SummaryA rational method of lumping inertia forces by considering the equilibrium of the vibrating element has been developed. This method requires the selection of a suitable displacement distribution function over each element. The closer it is to the true mode shape, the better the result.Considering a linear displacement distribution function over each element, the natural frequencies and mode shapes are obtained for transverse vibrations of a stretched string, torsional vibrations of a cantilever shaft (fixed at one end and free at the other) and transverse vibrations of a uniform cantilever beam. It is found that, even with a few elements, a reasonable accuracy can be obtained in the natural frequency, while the mode shapes are exact in the first two cases and almost exact in the third at the points considered.In Appendix A, it is shown that, for the torsional vibration of a uniform cantilever shaft and with a linear displacement function over each element, this method gives exact mode shapes at the points considered, while the natural frequency is always an upper bound and the error follows an inverse square law when the number of elements considered is large.In Appendix B, it is shown that a combination of this method with the conventional lumped mass method reduces the error in the natural frequency. The error follows an inverse fourth-power law when the number of elements considered is large and the mode shapes are exact at the points considered.This method can incorporate better displacement distribution functions, to obtain better results and convergence, and can easily be adapted to the buckling of columns, the vibration of beam columns and forced vibrations, as well as more complicated problems such as the vibration or buckling of plates and shells.


2000 ◽  
Author(s):  
Hong-Cheng Sheu ◽  
Lien-Wen Chen

Abstract A semi-analytic model is proposed to study the critical speeds and critical loads of the cantilever shaft-disk systems subjected to longitudinal loads. In the present work, both the exact and approximate stiffness influence coefficients of the longitudinally loaded cantilever shafts are derived. In order to obtain deeper insight into the dynamic behavior of such a shaft-disk system, the present shaft mathematical model has taken account of shear deformation effect. Because the exact stiffness influence coefficients of the shaft are transcendental and difficult to get their characteristics on longitudinal load intuitively, each stiffness influence coefficient is expanded in a Taylor’s series about the longitudinal load. Based on the present approximate stiffness influence coefficients, the critical speeds and critical loads of the cantilever shaft-disk systems can be easily and quickly obtained. Numerical simulations show that the present results are seen to be quite in agreement with the exact solutions.


2014 ◽  
Vol 24 (7) ◽  
pp. 1047-1069
Author(s):  
Jajneswar Nanda ◽  
LD Das ◽  
Sandeep Das ◽  
Harish Chandra Das

2013 ◽  
Vol 436 ◽  
pp. 180-187
Author(s):  
Luminita Bibire ◽  
Adrian Stelian Ghenadi ◽  
Liliana Topliceanu

Loading shaft of the mixing device is complex. Because the operating regime is characterized by a random variation of the regime parameters, it is difficult to determine an exact theoretical approach, from the point of view of calculation of the shaft. The stress shaft of a mixing device takes into account only partally of the real state of loading. At present, there is no unitary methodology for calculating of shaft for mixing devices. Although the effect of the mixer weight on the own frequency, has been partially taken into account when the shaft-mixer system rotates in the air, it must be reconsidered if the shaft-mixer system rotates in a liquid. The calculation presented in this paper will take into account "hydrodynamic mass" mam of liquid, corresponding to the mixer that actually vibrates with it. This contributes to an increase of its inertia, and to reducing of the own frequency (respectively of the critical speed). In this paper, the influence of the working environment on the deflection of vertical cantilever shaft will be considered, and calculation relations for own pulsation of the shaft equipped with a mixer will be set, with consideration of mixer hydrodynamic mass. For this purpose, it is calculated hydrodynamic mass mh attached to the mixer, and the reduction factor of pulsation due to hydrodynamic mass.


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