2003
DOI: 10.1016/s0022-460x(02)01137-9
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Transient vibration phenomena in deep mine hoisting cables. Part 1: Mathematical model

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Cited by 120 publications
(82 citation statements)
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“…And according to literature [7]: the frictional force brought by the press of the hoisting rope on the groove of head sheave was greater than the effect of the moment of head sheave, and if the shaft liner and shaft of head sheave was lubricated fully, it is impossible that slip happened between the hoisting rope and oriented pulley. The hypothesis of the same linear velocity of winding on the head sheave was also used by literatures [12,13] to investigate the vibration of hoisting rope. The effect of the oriented pulley and head sheave was similar, i.e., the linear speed of hoisting rope and the oriented pulley is assumed same and the torsional movement of hoisting rope on the groove of oriented pulley is restricted.…”
Section: A Extensional-torsional Coupledmentioning
confidence: 99%
“…And according to literature [7]: the frictional force brought by the press of the hoisting rope on the groove of head sheave was greater than the effect of the moment of head sheave, and if the shaft liner and shaft of head sheave was lubricated fully, it is impossible that slip happened between the hoisting rope and oriented pulley. The hypothesis of the same linear velocity of winding on the head sheave was also used by literatures [12,13] to investigate the vibration of hoisting rope. The effect of the oriented pulley and head sheave was similar, i.e., the linear speed of hoisting rope and the oriented pulley is assumed same and the torsional movement of hoisting rope on the groove of oriented pulley is restricted.…”
Section: A Extensional-torsional Coupledmentioning
confidence: 99%
“…The shape function is assumed to be related to the fundamental mode of the high-rise building and is approximated by a cubic polynomial representing the lateral displacements of the structure corresponding to the top of the structure and to the position of the car and counterweight estimated by Eqs. (5) - (9) .…”
Section: Description Of the Mathematical Modelmentioning
confidence: 99%
“…A model of an inclined rope's lateral oscillations is established on the following assumptions [5,6]: (i) The linear density of the inclined rope is constant; (ii) No rope slip on the friction pulley or across the head sheave; (iii) The effect of torsional coupling on the dynamic response is not significant and thereby can be neglected; (iv) Assume the spatial derivatives of longitudinal displacement to be small, and hence to be ignored; (v) No bending during deformation; and (vi) Without regard to air drags and the viscoelastic damping for their effects on the transverse vibrations are negligible. In the present model, in order to investigate how the axial fluctuations of head sheaves influence the transverse vibrations of the inclined ropes, only one inclined rope is adopted as the study object.…”
Section: Governing Equationmentioning
confidence: 99%