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Revision as of 06:24, 5 September 2023 by Vettermann (talk | contribs)

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Motivation

Due to the increasing interest in manufacturing accuracy without an additional energy demand for cooling, knowledge about the thermo-elastic behavior of entire machine tools becomes crucial. Methods to correct the thermally induced position error between the tool-center-point (TCP) and the workpiece in real-time are needed. Therefore, reduced-order models that enable a fast simulation of entire machine tools are applied in the design and production process.

Description

Figure 1: Experimental machine tool MAX.
Figure 2: Subassemblies and FE-model of the benchmark MAX.

The MAX benchmark is a linear time-invariant thermal model of the demonstrator machine tool MAX(Fig. 1). Due to its lightweight construction based on aluminium structures, low heat capacities and high thermal coefficients of expansion are to be expected [1]. It is divided into 50 stationary subassemblies (SA), see Fig. 2. The thermal finite element (FE) model was generated in ANSYS and afterwards the model was exported for post-processing as described in [2]. The interaction between the subassemblies is modeled by contact boundary conditions. The evolution of the temperature field is modeled with the heat equation

cpρTt=λΔT, on Ωk, k=1,,50,λTn=f, on ΓckΩk, k=1,,50,λTn=αext(TextT), on ΓextkΩk, k=1,,50,T(0)=T0, at t=0

with

f=κc(TciTck),ik,

and

k - number of the subassembly, k=1,,50
T - temperature
cp - specific heat capacity
ρ - density
λ - heat conductivity
Ωk - domain of the k-th subassembly
Γck - contact boundary of the k-th subassembly (partly time varying, moves with the position of the z-slide (considered as heat flow))
κext - heat transfer coefficient between a subassembly and the ambient air
Text - external temperature
Γextk - contact boundary with the ambience
κc - heat transfer coefficient between two subassemblies
Tck - temperature of the contact area of subassembly k.

The finite element discretization of the heat conduction models leads to the system

ET˙=AT+Bu(t),y(t)=CT,

with

En×n - capacity matrix
An×n - conductivity matrix
Tn - state vector (discrete temperature)
Bn×m - input map
um - input vector
yp - output vector
Cp×n - output map.


Data

Figure 3: Sketch of the two coupling approaches using the example of a model with 2 subassemblies.

The system matrices are available in the .mat file format and can be downloaded under the following link MAX.tar.gz. The model has n=1265497 degrees of freedom and is available for two diffenrent coupling approaches, which are explained in more detail in [2], see also Fig. 3:

  • A so called output-coupled model: In this case, an input-output coupling was used, i.e., the model is block diagonal and thus the subassemly models can be reduced separately for structure preserving MOR. There is a set of matrices for each subassembly with a total number of m=287 inputs and p=224 outputs.
  • A so called FE-coupled model: In this case, the subassemblies are coupled on FE-level, i.e., the conductivity matrix A of the overall system has additional (off-diagonal) coupling blocks. Thus the subassembly models cannot be reduced separately anymore. There is one set of matrices for the overall model with m=69 inputs and p=11 outputs.

Origin

The MAX is used as an experimental machine tool in the CRC/TR 96 Project-ID 174223256 financed by the German Research Foundation DFG.

References

  1. K. Großmann, ed., "Thermo-energetic Design of Machine Tools", Springer International Publishing, Switzerland, pp. 9-10, 2015.
  2. 2.0 2.1 J. Vettermann, S. Sauerzapf, A. Naumann, J. Saak, P. Benner, M. Beitel- schmidt and R. Herzog, "Model order reduction methods for coupled machine tool models", MM Science Journal, Special Issue ICTIMT 2021, 2021.

Contact

User:Saak