Thermal model of the spindle drive structure
Journal of Machine Engineering, Vol. 10, No. 4, 2010
machine tool, spindle unit
temperature, thermal deformations, model
Zdzisław WINIARSKI1
Zbigniew KOWAL1
Wojciech KWAŚNY1
Jae-Yong HA2
THERMAL MODEL OF THE SPINDLE DRIVE STRUCTURE
A computation system dedicated for machine tool spindle drives is presented which integrates a FDM model
with a FEM model. Modelling of heat exchange through coolers are discussed, as well as modelling of heat
exchange between cooling-lubricating oil and gear transmissions, shafts and headstock walls. In modelling
of heat exchange inside headstock, the use of additional elements - type "Fluid" and "Air" - is proposed. Sample
modelling results are presented concerning a headstock from a drilling-milling machine tool for machining with
high loads and are compared with experimental data.
1. INTRODUCTION
Main drives of turning, milling and grinding machine tools, as well as machining
centres are usually equipped in synchronous or asynchronous electric motors. Types
of drive transmission from a motor to a machine tool spindle can be various. The
introduction of a gear box between the motor and spindle allows, in a broad range, adjusting
rotational speed and torque on the spindle for the needs of the technological process. While
selecting drive parameters it is important to achieve required rotational speed quickly which
requires high acceleration and at the same time suitable motor power surplus. In such
solutions there is a possibility of the appearance of large radial forces, increased vibrations,
noise and other unfavourable phenomena. At required high torques between the motor and
the spindle, gear transmissions are applied. At lower torques such transmission is adequately
shortened all the way to a direct integration of the motor with the spindle (electrospindle).
There are also solutions of main drives with high-torque motors or motors coupled in
series in order to increase torque on the spindle. Such solutions are however much more
expensive from these described before. The selection of one of ways for transmitting drive
will always be a compromise between the required torque value and rotational speed,
precision and cost.
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1
2
Institute of Production Engineering and Automation, Wroclaw University of Technology, Wroclaw, Poland
DOOSAN Infracore Corporation, Korea
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Zdzisław WINIARSKI, Zbigniew KOWAL, Wojciech KWAŚNY, Jae-Yong HA
Difficulties in modelling main drives rise together with the complexity of their
kinematic structure and the need of applying motor, bearing and transmission cooling
systems. It also causes the rise of the amount and diversity of generated heat sources, which
require proper computation models, as well as the rise of the complexity of modelling
forced cooling of particular drive components.
The possibility of using commercial FEM programs, such as: Nastran, Ansys,
ABAQUS or Simdesigner for CATIA to simulate the behaviour of machine tool structures
is limited, because they do not have many required boundary conditions, which enable
taking into account significant interactions between the efficiency of internal heat sources
and temperatures and deformations of the entire structure. This especially applies to bearing
assemblies, gear transmissions, couplings, etc. placed in closed spaces, in which power
losses are a relation of temperature with thermal and elastic dimension changes. In such
situations, the best results are yielded by dedicated systems. In this paper, a dedicated
system, called SATO[6], will be described, which has been elaborated and is still developed
at the Wroclaw University of Technology, as well as thermal and elastic phenomena models
used in it, enabling the analysis of complex kinematic structures of spindle drives in varying
operational conditions and in transient thermal states.
2. DEDICATED SYSTEM SATO FOR THERMO-ELASTIC ANALYSES
This system is designated to simulate thermal and static behaviour of machine tools.
During its development, various methods were used, such as a Finite Element Method
(FEM), Finite Difference Method (FDM), as well as a series of procedures supporting
modelling of boundary conditions [5]. This system integrates computations of temperature
and displacement distributions with determining power losses in kinematic links of drive
systems (Fig. 1.).
Such integration ensures high precision of simulations. It is especially important for
the spindle assembly, where interactions take place between power losses, temperature and
thermal dimensional changes. These can significantly change values of power losses in
relation to these defined by simplified mathematical models without such conjugations.
Boundary conditions included in the system ensure modelling of thermal and elastic
phenomena taking place in the structure, as well as on stationary and mobile links between
machine tool units and components. These include: radiation, natural convection and
convection forced by the movement of elements, carrying of heat by means of coolant flow,
contact conductivity and contact stiffness. Boundary conditions included in the system
enable modelling of heat exchange with the environment, as well as in closed spaces inside
housings, as it takes place e.g. inside headstock bodies.
Internal procedures for computing power losses in subassemblies and kinematic pairs
of a machine tool require preparation of input data in the initial (cold) state with help
of external procedures. The most complex ones include procedures for ball bearings in the
assembled state. Fig. 2 shows an algorithm for determining such input data concerning
spindle angular contact bearings taking into consideration contact angle changes in
a bearing according to ball bearing theory [2].
Thermal Model of the Spindle Drive Structure
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Fig. 1. Dedicated SATO system general structure
The result of the operation of such algorithm are: after-assembly load of a bearing set
Fap or negative after-assembly clearance Lp, after-assembly contact angles αp, as well as
resulting interferences or clearances between a bearing and housing W1p and between
a bearing and spindle W2p. Fit W1p, W2p take into account not only dimensional
deviations of a hole in a housing and spindle pin, but also surface quality expressed as
roughness height Rz.
Angular contact ball bearings are assembled in sets of two or more bearings, arranged
in “X”, “O” arrangements or their combinations. Each of bearings in such set can have
different assembly conditions, due to e.g. varying dimensions of a hole in the spindle or
dimensions of the external diameter of a housing (Fig. 3).
Thermal changes of bearings set node dimensions during operation disrupt the elastic
force equilibrium on both sides of a set, taking place in an assembled bearing set, and lead
to the establishment of a new equilibrium of axial forces, but on a different level. In special
cases it can lead to partial or full unload of bearings. The consequence of such phenome (...truncated)