Abstract

Dynamic model of the ball in space for ball screw mechanism is established under different angular accelerations of the screw, and non-linear equations of the ball acceleration motion model were solved in accordance with ball movement characteristics during acceleration process of the ball screw mechanism. Forces and motion on the ball were analyzed taking into consideration acceleration state and the characteristics of the ball. Using the existing structural parameters of the ball screw mechanism and accelerating operating conditions of the ball, motion parameters of the ball were theoretically analyzed using simulations at different angular accelerations of the screw, along with motion parameters of the ball, which included contact angle, helix angle, the ball center locus helix path radius, normal force at contact points of the ball, the tangential velocity of ball center, relative sliding velocity of ball, and drag torque of the ball screw mechanism. A ball screw comprehensive test bench was used to experimentally measure drag torque of the ball screw mechanism under different angular accelerations of the screw. Changing regularity was found to be consistent between measured data with simulation results. As a result, acceleration dynamic model of the ball in space was demonstrated to be accurate and feasible.

Highlights

  • As a key component of numerical control machine tool, performance of the ball screw mechanism (BSM) has significant impact on processing quality of the workplaces

  • A larger angular acceleration of the screw resulted in greater friction torque of in speed results in the centrifugal force affecting the contact angle at the nut to decrease in magnitude

  • According to the dynamic model, angular acceleration was adjusted; drag torque of simulation can be compared with measured value

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Summary

Introduction

As a key component of numerical control machine tool, performance of the ball screw mechanism (BSM) has significant impact on processing quality of the workplaces. Between the ball and nut raceway is zero, the following equation can be obtained abn cos bB + abb sin bB = 0 (4)), relative acceleration of point A in the ball, relative to screw raceway in tangential direction t can be expressed as aASt = aÃbt + abnrb sin bA À abbrb cos bA, and acceleration in the raceway section peripheral direction is aASc = abtrb.

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