Abstract

Modelling of propeller shaft dynamics at pulse load The article discusses a method of modelling of propeller shaft dynamics at the presence of virtually introduced underwater detonation effects. The propeller shaft model has four degrees of freedom, which provides opportunities for introducing shaft displacements and rotations similar to those observed in a real object. The equations of motion, taking into account the action of external agents, were implemented to the Matlab SIMULINK environment. The obtained time-histories and their spectra were compared with the experimental results of the tests performed on the marine testing ground. The performed model identification confirmed its sensitivity to changing parameters of motion and external actions.

Highlights

  • The article discusses a method of modelling of propeller shaft dynamics at the presence of virtually introduced underwater detonation effects

  • The following actions were introduced to the proposed dynamic model [2]: main engine driving torque screw propeller anti-torque axial thrust force the action resulting from changes in relative positions of load-carrying bearings and thrust bearings in the shaft line the action of the hydrodynamic pressure generated by an underwater detonation

  • The propeller shaft model was an object of simulation tests to check its sensitivity to the action of external agents and compliance with the behaviour of the object in the conditions of the simulated environmental action [5]

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Summary

Analysed degree of freedom

The propeller shaft model was an object of simulation tests to check its sensitivity to the action of external agents and compliance with the behaviour of the object in the conditions of the simulated environmental action [5]. The proposed model is nonlinear, and an attempt to describe it by linearisation of actions is unacceptable as it may lead to incorrect conclusions resulting from possible superposition of the effects observed in linear systems [3]. Since in the equations of motion the time is represented explicitly, this system is non-autonomous. The kinetic energy of the presented system was written as:

DYNAMIC MODEL OF THE SHAFT LINE
IDENTIFYING THE PROPELLER SHAFT MODEL
CONCLUSIONS

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