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19-07-2021 | Machine Tool | Issue 6/2021 Open Access

Production Engineering 6/2021

Acceleration-based disturbance compensation for elastic rack-and-pinion drives

Production Engineering > Issue 6/2021
Felix Brenner, Armin Lechler, Alexander Verl

1 Introduction

The achievable productivity and machining accuracy of modern machine tools and manufacturing systems is essentially determined by the dynamic properties of the feed drive systems used. These determine the achievable drive force and acceleration and the positioning accuracy as well as the static and dynamic stiffness characteristics of the individual machine axes [ 3]. Consequently, position-controlled feed drive systems are a key component of the modern manufacturing industry. Nowadays, the motion of the individual machine axes is generated by the use of linear direct drives and electromechanical feed drives [ 2]. In the latter case, the rotary motion of the highly dynamic motors is converted into a linear motion of the machine table, with ball screw drives or rack-and-pinion drives (RPD) usually being used as mechanical transmission elements. Due to the excellent cost-performance ratio, the high positioning accuracy as well as a low assembly and maintenance requirements, ball screw drives are still the main drive solution in the machine tool industry. However, from a feed length of about 4–5 m, the gradually increasing spindle diameter leads to a large inertia increase, which is accompanied by a reduction in the drive dynamics [ 9]. Since ball screw drives can no longer be operated efficiently above such feed lengths, RPDs are used in particular for large machine tools [ 29].

1.1 Rack-and-pinion drive control

Today, position-controlled feed drive systems are almost exclusively operated through a cascade structure with subordinate proportional-integral (PI) current and speed control as well as proportional (P) position control [ 25]. The controlled values of the individual cascades are fed back separately, whereby the dynamics of the individual control loops decrease from the inside to the outside. Essential for the achievable accuracy and stiffness is the type of measuring system used within the position control loop, see Fig.  1. While direct positioning measurement systems on the table side are widely used for compact and high-precision machine tools, indirect position signals are often used as controlled value for large machine tools with rack-and-pinion drives. In this case, the table position \(x_T\) is determined indirectly based on the motor encoder \(x_M\) and the known transmission ratios [ 32]. By omitting the additional direct measuring system, great cost advantages can be achieved. Here, not only the acquisition costs themselves, but also the integration costs, which arise due to the increasingly complex alignment with long feed distances, must be included in the overall economic calculation. In addition, there is a probability of 15 \({\,\%}\) that machine failures are due to measuring system errors [ 20], making indirect position control loops still widespread despite the falling costs of the linear scales themselves. However, a central problem of indirect position control loops is the unavailability of table-sided state informations. This means that the system can only react inadequately to disturbance variables that are outside the control loop, resulting in an overall reduction in positioning accuracy and disturbance stiffness. In addition to process-related load forces, friction forces typically occur as disturbance variables within the machine axes, which are usually characterized by a pronounced nonlinearity.

1.2 Disturbance compensation in drive systems

Considering the constantly increasing accuracy requirements for modern machine tools, additional actions have to be taken to improve the dynamic tracking and disturbance behavior of indirectly controlled rack-and-pinion drives. In particular, compensating control loops, which extend the conventional cascade control, provide considerable potential for dynamic improvement [ 21, 23]. For the realization of such structures, acceleration sensors mounted on the table side are particularly suitable. These can be used to detect the vibration state of the feed axis on the output side even without a direct position measuring system. However, the currently existing approaches of acceleration-based compensators mainly focus on ball screws and linear direct drives with additional direct measurement of the table position [ 7, 13, 17].
For ball screws drives, an additional speed control loop for the mechanics with a Ferraris sensor has been researched, which increases the bandwidth within the postion control loop [ 22]. In addition, compensation modules have already been developed for directly controlled ball screws drives [ 4, 14] and linear direct drives [ 28], which provide compensating reference values on the position and velocity level. On top of that, there are control loops on the force or current level [ 16, 18], which can be used to compensate disturbances in a highly dynamic manner.
In contrast, there are only a few approaches for indirectly controlled rack-and-pinion drives. In the method presented in [ 19], the table acceleration is fed back into the velocity control loop on the motor side via a complex filter structure, thus, the compensation does not take place directly at the current or force level. Furthermore, there are two approaches [ 15] and [ 5] where the compensation is applied directly on the current level, but the elasticity of the oscillatory mechanics is neglected. This results in a relatively small useful frequency range of the methods.
This paper is intended to fill the gap of the already existing approaches by developing a highly dynamic compensation method on the current respectively force level, which will simultaneously capture the influence of the dynamic-limiting mechanics. After a theoretical derivation of the method on the basis of a generally valid drive model (Sect. 2), the mode of action is confirmed by numerous experimental investigations. Particular attention will be paid to the dynamic disturbance behavior, which will be evaluated on the one hand by investigating compliance frequency responses and on the other hand by applying milling forces (Sect. 3). In addition, a standardized parameterization scheme is presented and the robustness of the method is finally evaluated.

2 Disturbance compensation design

The dynamic transfer behavior of rack-and-pinion drives results from the interaction of the individual subcomponents of the drive train. Due to today’s modern servo and inverter technology, very high current control bandwidths are usually achieved, so that the mechanical transfer behavior is the limiting factor compared to the electrical subsystem. The coupled mechanical transmission behavior can basically be described by multi-mass oscillator systems with a large number of degrees of freedom (DOF). Typically, the lowest natural frequency occurring in the drive train has the dominant influence and limits the achievable bandwidth of the position control [ 12]. The starting point for the design of the acceleration-based disturbance compensation is thererfore a simplified two-mass oscillator model [ 24], which is used to abstract the dynamic transfer behavior in a model-based manner by capturing the first natural frequency [ 8], see Fig.  2.
The feed drive system is composed of a rotational equivalent mass \(m_M\) (motor, gearbox, pinion) and a translational moving mass \(m_T\), whereby the elasticity is captured via the stiffness and damping constants c and d. The addtional gearbox is often installed between the motor and the pinion shaft in order to generate high torques for the movement of the mostly large inertias. The conversion of all rotatory parameters into their translatory equivalence is carried out taking into account the transmission ratio of the the pinion radius r and gearbox i. The driving force F acting on the system results from the proportional relationship between torque constant \(K_M\) and the torque-generating current \(i_q\). The torque-generating current is available as a measurable signal in the frequency inverter due to the transformations performed on the electrical currents and the subordinate current control that is present anyway. Of central importance for the development of a compensating control loop is the dynamic transfer behavior of the driving force to the resulting table force \(F_T\)
$$\begin{aligned} G_E(s)=\frac{F_T(s)}{F(s)}=\frac{1+s\frac{d}{c}}{1+s\frac{d}{c}+s^2\frac{m_Mm_T}{(m_M+m_T)c}}. \end{aligned}$$
The transfer behavior is composed of a second-order low-pass filter with an additional zero. The latter can be neglected due to the often very low mechanical damping values [ 31], since the behavior in the relevant frequency range is dominated by the conjugate complex pole pair of the denominator
$$\begin{aligned} G_E(s)\approx \frac{1}{1+s\frac{d}{c}+s^2\frac{m_Mm_T}{(m_M+m_T)c}}. \end{aligned}$$
In addition to the existing friction forces, process-related load forces \(F_{S,M}/F_{S,T}\) typically occur as disturbance variables in the drive train, which act on the drive motor as a feedback disturbance force. Since the drive immediately reacts to the introduced disturbance by applying an additional compensation torque, the input of the current control loop is the innermost and thus most dynamic point of intervention within the cascade control in order to implement a disturbance compensator. For this purpose, the acceleration \(\hat{a}_T\) expected at the machine table is firstly estimated using the relationship established in eq. ( 2). In addition, the actual acceleration \(a_T\) is measured via an accelerometer attached to the machine table. The difference between the measured and estimated acceleration can be used to obtain a synthesized current \(i_{q,c}\), which is fed into the control cascade as an additional command value, see Fig.  3. The mode of operation of the compensation term is limited by an additional low-pass filter \(G_{LP}\) with the filter cut-off frequency \(f_g\) in the feedback path in order to attenuate the high-frequency noise effects occurring in the measured current and acceleration signal.

3 Experimental results

The disturbance compensation method developed in the previous section is implemented and evaluated for experimental studies on a rack-and-pinion test bench. Figure  4 shows the test bench, which can be used either in classic pre-loaded dual-motor mode or in single-motor mode [ 30]. In the present application, however, the second drive train is completely dismounted and the approach is initially evaluated for the case with only one drive. However, it should be noted that the method can in principle also be used for pre-loaded rack-and-pinion drives with a master-slave position control structure [ 11]. In addition to extensive measuring systems, an additional linear direct drive is integrated on the machine slide, which can be used to introduce table-side disturbance forces into the axis structure. The dimensioning and component selection of the test bench was based on common requirements in the machine tool area, see Table  1. The entire conventional cascaded drive control is implemented on the control unit (CU) of the servo control system, whereby the position control loop is operated at 1 kHz and the speed, respectively, current control loop at \({8\,\mathrm {kHz}}\). The individual control cascades were parameterized according to the usual setting rules in machine tool industry. For this purpose, the speed control loop was implemented using the symmetrical optimum and the position control loop was designed with regard to overshoot-free positioning (aperiodic case).
The disturbance compensation is implemented on a separate real-time system and is operated in the same cycle as the current control loop, see Fig.  5. The torque-generating motor current and the externally connected acceleration sensor are processed analog via an FPGA board and are available on the real-time system with a sampling rate of \({8\,\mathrm {kHz}}\). As an acceleration sensor, a compact and low-cost MEMS (micro electro mechanical system) sensor is used, which is rigidly attached to the machine table. Through an additional ProfiBUS module, all measured and controlled variables available on the CU can be accessed and monitored on the control PC. An overview of the components installed on the test bench is shown in Table  2.
Table 1
Parameters of the test bench
Gear ratio
Pinion radius
Torque constant
Drive mass
Table mass
Nominal motor speed
Nominal motor torque
Position control gain
Speed control gain
Speed control reset time
Table 2
Components of the test bench
Factory number
Synchronous motor siemens
1FT7086-5AH70-1CA0 (Drive Cliq)
Planetary Gear Wittenstein RP040S
Wittenstein RMT400
Linear direct drive
Siemens 1FN3300
Acceleration sensor
Capacitive MEMS Accelerometer
Kistler 8315A010D0AC10
Absolute Encoder Siemens AM24DQI
Direct position measuring system
Schneeberger SSI AMSABS3

3.1 Parameterization of the disturbance compensation

The application of the developed concept for disturbance compensation requires the parameterization of the two filter structures \(G_E\) and \(G_{LP}\). All remaining parameters such as the pinion radius, the gear ratio, the motor constant and the inertias in the drive train can be taken from the corresponding data sheets of the components. The parameters for stiffness and damping ( c,   d) in the feed direction contained in the elastic transfer function \(G_E\) can either be estimated approximately on the basis of the mechanical properties of the rack-and-pinion drive or obtained via a frequency response analysis. For the second case, the mechanical frequency response can be used, which characterizes the dynamic transfer behavior from the motor speed \(v_M\) to the table speed \(v_T\) and can be measured as standard in many drive units. If the mechanical frequency response for the already described two-mass oscillator model is set up
$$\begin{aligned} G_M(s)=\frac{v_T(s)}{v_M(s)}=\frac{1+s\frac{d}{c}}{1+s\frac{d}{c}+s^2 \frac{m_T}{c}} \end{aligned}$$
and the occurring zero is equally neglected due to the low mechanical damping
$$\begin{aligned} G_M(s)\approx \frac{1}{1+s\frac{d}{c}+s^2 \frac{m_T}{c}}, \end{aligned}$$
it can be seen that the mechanical transmission behavior can be approximated as a second-order delay element with conjugate complex pole pairs
$$\begin{aligned} G(s)=\frac{\omega _0^2}{s^2+2D\omega _0s+\omega _0^2}. \end{aligned}$$
Using a corresponding coefficient comparison, the mechanical stiffness and damping can be determined from the damping ratio D and the characteristic frequency \(\omega _0\), see Table  3.
Figure  6 compares the real mechanics frequency response to the described model-based approximation. If the normalized root-mean-square deviation (NRSME)
$$\begin{aligned} \xi = 1-\frac{\left| y-\hat{y} \right| }{\left| y-\mathrm {mean}\left( y\right) \right| } \end{aligned}$$
is used as a performance criterion for the degree of model accuracy, the model shows an overall fit of \({76.2\,\mathrm {\%}}\) in the frequency range up to about \({100\,\mathrm {Hz}}\). The performance value results from an error comparison, normalized to the mean value, between the actual output y and the estimated output \(\hat{y}\). Only in the higher frequency range up to \({250\,\mathrm {Hz}}\) the model shows a deviating behavior due to the existing resonance-absorber phenomenon. This can be seen as the feedback effect of an additional vibration element on the table mass and is accompanied by a temporary phase increase in the phase response. To capture such effects, the introduced two-mass model would have to be extended by additional degrees of freedom.
Table 3
Identified mechanical parameters of the test bench
Damping ratio
Characteristic frequency
\(\omega _0\)
Stiffness constant
Damping constant
Since the bandwidth of the method is limited anyway by the low-pass behavior in the forward path for estimating \(\hat{a}_T\) with the transfer function \(G_E\), the bandwidth of the synthesized current \(i_{q,c}\) is limited to the same frequency range. As a practical parameter, the -3dB cutoff frequency \(f_{\mathrm {-3dB}}\) of the transfer function is used and equated with the cutoff frequency of the lowpass filter, see Fig.  7. This results in a filter cutoff frequency of \({f_g=99.6\,\mathrm {Hz}}\). For the present application, low-order infinite impulse response (IIR) filters have proved particularly useful. Compared to the otherwise widespread FIR filters (finite impulse response), this is due to the relatively low time delay of the filter response, which makes it possible to generate a drive torque in counterphase to the disturbance variable. The IIR filter type used is a Bessel filter [ 27] with a low filter order of \(n=2\). The Bessel filter used is characterized by a low phase shift in the relatively small effective frequency range and by a smooth frequency response in the passband. Finally, it should be noted that in principle also other (IIR) filter types can be used.

3.2 Compliance behavior

Due to the acceleration measurement of the machine table, the developed disturbance compensation is primarily used to specifically suppress disturbance forces occurring on the drive side. For the evaluation of the disturbance behavior, the dynamic compliance
$$\begin{aligned} {G_c(s)=\frac{x_s-x_T}{F_{S,T}}} \end{aligned}$$
is to be considered. It is the complex coefficient of a displacement and the dynamic force \(F_{S,T}\) [ 32]. Consequently, the dynamic compliance describes the frequency-dependent reciprocal value of the stiffness of a controlled electromechanical system. For the measurement-based frequency response analysis, a sine sweep of constant force amplitude and increasing frequency is applied to the linear direct drive and the resulting difference between the reference position \(x_s\) and the table position is determined
$$\begin{aligned} e(t)=x_s(t)-x_T(t). \end{aligned}$$
Figure  8 shows the compliance frequency responses of the RPD with and without disturbance compensation. Due to the closed position control loop on the motor side, the rack-and-pinion drive has only a low overall static stiffness ( \({f=0\,\mathrm {Hz}}\)) compared to systems with a direct position measuring system. Regarding the latter case, the static stiffness depends mainly on the linear measurement system used [ 8]. On the other hand, there is a visible maximum in the range of the first natural frequency. From this, it can be concluded that disturbance forces with a high spectral proportion in the range of the first natural frequency lead to a strong excitation of the drive system. Since the developed disturbance compensation generates a drive torque that is in counterphase to the disturbance force and thus compensates it significantly faster than conventional control, this leads to a considerable increase in damping. Due to the limited operating range of the disturbance compensation, the two compliance frequency responses match above the cutoff frequency of the low-pass filter. The compliance frequency responses shown in the figure were averaged over 18 frequency responses at different axis positions to remove measuring uncertainties. In contrast to the assumption of a position-independent behavior of rack-and-pinion drives which is often found in the literature [ 6, 29], the experimental results show that the local contact conditions of the engaged rack-and-pinion pair cause a certain spread of the results. Figure  9 illustrates the maximum dynamic compliance \(N_{\mathrm {max}}\) in relation to the axis position. Despite the existing spread, the additional disturbance compensation reduces the maximum compliance occurring in the drive train at all positions in comparison to the conventional system.

3.3 Milling forces

In order to verify the practical usability of the developed compensation method in an industrial environment, the behavior during the application of milling forces will be investigated. For this purpose, a standard 2-DOF milling force model [ 1] is implemented on the real-time system with configurable process parameters, which is used to control the linear direct drive. Since significantly higher disturbance forces are caused in peripheral milling compared to face milling due to the same direction of all force vectors, the critical case of peripheral milling in the feed direction will be addressed below. The process force of a single cutting edge of the milling cutter
$$\begin{aligned} F_P(\varphi ,a_p)=f(\varphi )\left( -F_t(\varphi ,a_p)\mathrm {cos}(\varphi )-F_r(\varphi ,a_p)\mathrm {sin}(\varphi ) \right) \end{aligned}$$
is composed of a cutting force
$$\begin{aligned} F_t(\varphi ,a_p)=a_pk_ch_z(\varphi )^{1-m_c} \end{aligned}$$
and a radial force
$$\begin{aligned} F_r(\varphi ,a_p)=a_pk_nh_z(\varphi )^{1-m_n}, \end{aligned}$$
whereby the infeed depth is captured via the parameter \(a_p\). The Heaviside function f, which depends on the cutter geometry, indicates whether the cutting edge is in engagement
$$\begin{aligned} f (\varphi ) = \left\{ \begin{array}{ll} 1 ~~ &{} \text {if intervention,} \\ 0 ~~ &{} \text {otherwise.} \\ \end{array}\right. \end{aligned}$$
The chip thickness
$$\begin{aligned} h_z(\varphi )=f_z\mathrm {sin}(\varphi ) \end{aligned}$$
contained in the partial forces depends on the current rotational angle of the cutter \(\varphi\) and the feed per tooth \(f_z\). The remaining parameters for the specific cutting force \(k_c\)/ \(k_n\) and the material constants \(m_c\)/ \(m_n\) in eqs. ( 10) and ( 11) are material-dependent cutting parameters and can be taken from tables, thus they will not be discussed further [ 10, 26]. Taking into account the number of cutting edges n of the cutter and the corresponding angular offset between the individual cutting edges \(\Delta \phi\), the total force acting in the feed direction can finally be calculated as
$$\begin{aligned} F_s(\varphi ,\Delta \phi ,a_p)=\sum _{k=0}^{n-1}F_P(\varphi +k\Delta \phi ,a_p). \end{aligned}$$
As an application scenario, a \(2\,\mathrm {m}\) long, \(3\,\mathrm {mm}\) deep and \(30\,\mathrm {mm}\) wide material removal is to be considered, with a cutting speed of \(150\,\mathrm {m/min}\) at a feed rate of \(390\,\mathrm {mm/min}\). All parameters used for the milling force model are presented in Table  4. The choice of the mentioned parameters is based on reference values from table books [ 10] (low strength steels, milling with carbide). The process force resulting from the milling force model for the application described is shown in Fig.  10. The generated milling force leads to a broadband excitation of the drive system, which can be recognized, by the additionally shown one-sided spectrum of the milling force.
Table 4
Process parameters of the generated milling force
Groove length
Cutting speed
Width of engagement
Cutting edge number
Feed rate
Specific cutting force
\({{{\rm N/mm}}^2}\)
\({{{\rm N/mm}}^2}\)
Material constant
Furthermore, the error curve on the output side according to eq.  ( 8), as well as the resulting quadratic error summation
$$\begin{aligned} J_s = \int _{0}^{t_f}e(t)^2\mathrm {d}t \end{aligned}$$
over the duration of the milling process \(t_f\) is shown. As shown in the figure, the use of an additional acceleration-based disturbance compensator contributes to a significant reduction of the output side positioning error.
In addition to the objective of increasing accuracy, the efficiency of drive systems is becoming equally important. For this reason, the electrical energy consumption
$$\begin{aligned} E=\int _{0}^{t_f}P(t)\mathrm {d}t \end{aligned}$$
via the integral of the absorbed power P of the electric motor as well as the mechanical load [ 8]
$$\begin{aligned} B=\int _{0}^{t_f}|M(t)|^3|\dot{\phi }(t)|\mathrm {d}t \end{aligned}$$
should also be taken into account. The latter is related to the wear and thus the durability of the feed drive system and is calculated via the motor torque M acting on the drive system as well as the angular velocity oft the motor \(\dot{\phi }\). As shown in Table  5 with the listed performance indicators, the use of the disturbance compensator contributes to a significant increase in efficiency. The electrical power consumption of the motor is reduced by the counterphase compensation, since the cascaded drive controller has to operate less against the disturbance variables that occur. Additionally, the mechanical load to the drive system is reduced due to the damping effect, which leads to a reduction in the acceleration peaks.
Table 5
Performance characteristics during milling forces
Disturb. comp.
Sq. error \(J_s {({\rm mm}^{2{\rm s}})}\)
0.195 ( \(-61.8\,\mathrm {\%}\))
El. Energy \(E {\rm (Wh)}\)
2.638 ( \(-45.8\,\mathrm {\%}\))
Load \(B {({\rm Nm}^{3{\rm rad/s}})}\)
1040.32 ( \(-69.8\,\mathrm {\%}\))

3.4 Robustness analysis

The key problem of many control concepts for increasing the dynamics of electromechanical feed drive systems is that they have insufficient robustness properties. Consequently, the robustness of the method will finally be evaluated. For this purpose, a practical scenario is to be used in which the mass of the machine table is being varied. This occurs, for example, when machining a large-volume component, which can cause significant mass changes. The mass change of the workpiece clamped on the machine table with the associated variation of the system dynamics is defined as a varying operating condition in the following.
This is accomplished by adding an additional mass of approximately \(+130\,\mathrm {kg}\) to the existing test bench, so that the total table mass corresponds to \(\tilde{m}_T=550\,\mathrm {kg}\). Subsequently, the cascade control is parameterized according to the usual setting rules and the distrubance compensation control loop is adjusted according to the guidelines presented in Sect. 3. Using the test brench configured in this way, the milling tests as well as the compliance evaluation are repeated and the results with and without the compensator are compared. Next, the table mass is loaded ( \(+24\,\mathrm {\%}\)) or reduced ( \(-24\,\mathrm {\%}\)) by a further \(\pm 130\,\mathrm {kg}\). The same series of measurements are then performed for both configurations, with both the control and compensator settings remaining unchanged. The results obtained from the described measurement methodology are shown for all three mass configurations in Fig.  11. In addition, Table  6 shows the performance characteristics for the tracking behavior and efficiency resulting from the milling scenario.
Table 6
Performance characteristics during milling forces and varrying table mass
Disturb. comp.
\(-130\,{\rm kg}\)
Sq. error \(J_s {({\rm mm}^{2{\rm s}})}\)
0.183 ( \(-60.0\, {\%}\))
El. Energy \(E~{\rm (Wh)}\)
2.732 ( \(-39.39\,{\%}\))
Load \(B{({\rm Nm}^{3{\rm rad}/{\rm s}})}\)
1186.86 ( \(-60.4\,{\%}\))
Sq. error \(J_s {({\rm mm}^{2{\rm s}})}\)
0.187 ( \(-49.7\, {\%}\))
El. Energy \(E {\rm (Wh)}\)
2.488 ( \(-38.8\,{\%}\))
Load \(B {({\rm Nm}^{3{\rm rad}/{\rm s}})}\)
1350.10 ( \(-54.1\,{\%}\))
\(+130\,\mathrm {kg}\)
Sq. error \(J_s {({\rm mm}^{2{\rm s}})}\)
0.141 ( \(-50.4\,{\%}\))
El. Energy \(E~{\rm (Wh)}\)
2.494 ( \(-36.2\,\mathrm {\%}\))
Load \(B {({\rm Nm}^{3{\rm rad}/{\rm s}})}\)
1359.33 ( \(-52.2\,{\%}\))
Based on the compliance frequency responses and the control errors, it can first be concluded that the increasing table mass in the drive train has a generally positive effect on the disturbance behavior. The gradually increasing damping effect can be seen both from the progressively reduced compliance and also in the reduction of the squared error norms. With respect to the disturbance compensation, it is shown that despite the incorrectly adjusted compensator, a significant improvement can be achieved for both a positive and a negative variation of the table mass. Depending on the table mass, the compensator achieves a reduction of the squared error norm from 49.7 \({\,\%}\) to 60.0 \({\,\%}\) compared to the nominal system. Equally, the compensator continues to improve the efficiency parameters at all operating points in terms of electrical energy consumption and mechanical load. In summary, it can be concluded that the method has promising robustness properties and contributes to a holistic improvement of the disturbance behavior even in different operating conditions with varying mass parameters.

4 Conclusion

In this paper, a highly dynamic disturbance compensation for indirectly controlled rack-and-pinion drives was developed and its performance was experimentally validated. The presented method bridges the gap to the already existing approaches, since both the elasticity of the drive system is considered as well as the compensation is simultaneously performed on the current level. The results show that considerable improvement of the dynamic disturbance behavior can be achieved. This is shown on the one hand in the reduction of the maximum compliance occurring in the drive train and on the other hand in the reduction of the position error on the output side while applying milling forces. At the same time, the method has a positive effect on the efficiency of the feed drive system, as both the mechanical load and the electrical energy consumed are reduced. Furthermore, the method shows robust behavior in different operating conditions.
The implementation of the method requires the presence of an acceleration sensor mounted to the machine table. In addition, the torque-generating current of the drive is required, which, however, is available as a sensor signal on the inverter for the underlying current control. For a robust performance with counterphase disturbance suppression, the compensation must be operated in the highly dynamic current control cycle, thus the requirements for the computing and signal processing hardware must be considered demanding. In contrast to this, however, there is the relatively low complexity of the compensation algorithm itself, which can be realized via a relatively small number of elementary operations with two additional filter structures. The parameterization of the compensation method follows a standardized procedure based on a frequency response analysis and the data sheet values of the components that are available anyway.
In a further step, the improvement potential of the method will be evaluated in real milling applications. At the same time, the model for estimating the table acceleration will be extended by including higher-frequency effects such as absorber resonance phenomena. On top of that, further robustness investigations will be carried out for varying model parameters.


This work was funded by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation), Project No. 271104968. The authors gratefully acknowledge the support by DFG.


Conflict of interest

The authors declare that they have no conflict of interest.
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