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عدد المساهمات : 18996 التقييم : 35494 تاريخ التسجيل : 01/07/2009 الدولة : مصر العمل : مدير منتدى هندسة الإنتاج والتصميم الميكانيكى
| موضوع: بحث بعنوان Gearbox Dynamic Modelling الخميس 22 يوليو 2021, 1:33 am | |
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أخوانى فى الله أحضرت لكم بحث بعنوان Gearbox Dynamic Modelling Walter Bartelmus Machinery Systems Division, Wrocław University of Technology
و المحتوى كما يلي :
The paper reports on current developments in gearbox dynamic modelling. It refers to M¨uller’s one-mass two-parameter (stiffness and damping) gearbox model with rectilinear vibration. The paper shows that there is a need to develop a new model, which would incorporate torsional vibration. The paper refers to the previous papers on gearbox dynamic modelling published by the author in journals and conference proceedings. In the present paper, the influence of the clutch damping coefficient and one random parameter value from the three-parameter error mode, and that of the interaction between error parameters on the vibration generated by a gearbox system, is analyzed. Key words: gearbox model, mathematical modelling, computer simulation. Introduction The modelling of gearbox dynamic behaviour belongs to the fundamental problems of mechanical system modelling. The problem has been the subject of many papers in Poland and abroad: Wang (1974), Mark (1978), Velex and Maatar (1996), Smith (1998). The model presented by M¨uller in 1979 has received a lot of attention in Poland. It was discussed, for example, by Ryś (1977), Wilk (1981), and Dąbrowski (1992). The model is a two-parameter (stiffness and damping) model in which the inertia of two wheels has been reduced to one mass equivalent to a one-stage gearbox. The author of the present paper has found that more sophisticated models are needed to describe the gearbox dynamics properly; Bartelmus (1994, 2000). Mathematical modelling and computer simulation can be applied to990 W. Bartelmus gearbox dynamics to support diagnostic signal evaluation for diagnostic inference. This is the main aim of the present research. The computer simulation is based on a mathematical model developed by Bartelmus (1994, 2000). General information on gearing needed for the computer simulation of gearbox behaviour was given by Bartelmus (2000). Some results of computer simulations supporting diagnostic inference were presented by Bartelmus (1996-1999). The papers show that mathematical modelling and computer simulation enable the detailed investigation of the dynamic properties of a gearing system. All the basic factors such as: design, technology, operation and change of the gearing system conditions which have a bearing on the vibration generated by a gearing can be investigated. The causes of vibration in gearboxes are mainly the tooth errors and vibration is an indication of them. The computer simulation results are referred to the laboratory investigation results presented by Rettig (1977) and to the field measurements reported by Penter (1991), Bartelmus (1992), and Tuma et al. (1994). As mentioned above, the vibration of a gearbox indicates that there are tooth errors in it. The errors appear at the production stage. The nature of the gear-wheel interaction is such that non-linear phenomena occur caused by friction, intertooth backlash, impact-like intertooth forces and periodic changes in tooth stiffness. As a result, the intertooth forces may exceed the force values, which follow from the gearbox system’s rated moment. Mathematical description enabling to include these phenomena in the equation of motion is given by Bartelmus (2000). The intertooth forces increase dramatically under unstable conditions. A one-stage gear system operates under resonance conditions and is unstable when the gearbox system’s mesh frequency is equal to its natural frequency. In such conditions, the intertooth forces are two times greater than the rated forces. The phenomenon of resonance has not been investigated fully for gearbox systems. Computer simulations reveal that conditions similar to the ones occurring at resonance may result as errors (pitting, scuffing of teeth flanks and failure of bearings) increase during the service of a gearbox system. In the present paper, current developments in gearbox modelling are presented with reference to the previous papers by the present author. It is shown that a flexible clutch and an error mode random parameter have an influence on the gearbox stability (teeth separation). An error mode is described by several parameters, i.e. maximum error value, shape of error plot and random error fluctuation depth. Conclusions The paper has shown a detailed analysis of a mutual influence of the error mode parameters and influence of a clutch damping on a dynamic factor Kd, which reveals the gearing condition. The error mode is described by three parameters: a – shape parameter, e – maximum value of the error, r – scope998 W. Bartelmus of the error random change. The analysis proves that, in general conditions of a gearing change (change of e and r), the linear increase of Kd does not hold, as it is stated in Bartelmus (1992) (experiment on a real object) and 1996 (computer simulation experiment). In the experiment on a real object and in the computer simulation experiment, only the value of e was taken into consideration.
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