Patent Document

CROSS-REFERENCES TO RELATED APPLICATIONS 
   This application claims the priority of German Patent Application, Ser. No. 102 20 937.5, filed May 10, 2002, pursuant to 35 U.S.C. 119(a)-(d), the disclosure of which is incorporated herein by reference. 
   BACKGROUND OF THE INVENTION 
   The present invention relates to a method for damping chatter oscillations in a processing machine, in particular a cutting machine, and to a device for carrying out the method. 
   Chatter oscillations in a workpiece or in a tool can occur when materials, particularly metals, are cut with a machine tool. Chatter can produce unusable surfaces and waste. Frequently, chatter occurs when the machine structure mechanically yields under the applied cutting forces. Periodic excursions are observed in particular when the cutting forces are excited at a frequency close to one of the characteristic resonance frequencies of the machine. These periodic excursions due to chatter can cause periodic discontinuities in the cutting force which under certain phase relationships with the machine resonances can sustain and/or even amplify chatter. The presence of chatter oscillations limits machine productivity, in particular when materials that require a high cutting force or a large cutting depth are cut. Chatter may only be reliably eliminated by reducing the cutting depth below a certain value. 
   If the desired cutting depth is to be maintained while eliminating chatter, the machine structure has to be either stiffened or better damped. Frequently, the available installation space and/or the weight or the costs of the machine make it difficult to implement a stiffer construction. Damping is difficult to improve by employing only mechanical means. The materials used in the construction of the machine have only very small and unpredictable intrinsic damping, in the order of a few percent. 
   The publication “Hochgenaue Regelung von Linearmotoren durch optimierte Strommessung” ( High Precision Control Of Linear Motors Through Optimized Current Measurements ) published in the German technical journal “antriebstechnik”, Vol. 38 (1999), No. 9, pp 90-93, discloses a feed system with a permanent-excited synchronous linear motor and a field control with a high-resolution PWM transistor converter and a synchronized, high precision current measurement. A conventionally controlled linear motor with low friction guides exhibits under controlled operating conditions a parasitic motion which is superimposed on the feed motion. This parasitic motion is also observed when the motor is stopped. An adequate motion quality can be achieved by measuring the current with a secondary current controller while controlling the position. With a closed loop control, noise produces a corresponding feed force in the linear motor, which then causes a parasitic motion of the feed carriage. Only the parasitic components of the current along the q-axis (quadrature or out-of-phase axis), where the force is produced, cause a parasitic force and hence a parasitic motion. The parasitic components of the current along the d-axis (direct or in-phase axis), where the field is formed, do not affect the parasitic motion. Due to the high inertia of the carriage, high parasitic frequencies have only a small effect on the position of the carriage. The parasitic frequency curve has a maximum at intermediate frequencies, depending on the control bandwidth of the velocity and position control. This is the frequency range where disturbances in the current measurement have the greatest impact on the position of the carriage. A precise feed motion can be realized with a single drive system, which includes a synchronous linear motor, by synchronously measuring the currents, for example, by using an oversampling method with an effective resolution of 12 bits. This high-precision current measurement in conjunction with a field control improves the parasitic motion by a factor of 20, using the same control dynamics. 
   Unlike rotary servo motors, linear motors used for driving feed axes have a flat air gap. Linear motors have a (feed) direction along which the feed force is generated, and another (force) direction along which the attractive magnetic force is produced. The feed direction is parallel to the plane of the air gap, whereas the force direction is oriented normal to the plane of the air gap. Because the attractive force is perpendicular to the drive force, this force is also referred to as transverse force. In principle, the linear motor can produce controllable forces both in the feed direction and also in the transverse direction. For controlling the feed force, the q-component (quadrature or out-of-phase component) of the three-phase current is used, whereas the d-component (direct or in-phase component) is responsible for the attractive force. The two components are perpendicular in a three-phase system. Controlling the drive force via the q-component of the motor current does not affect the attractive force and vice versa. The two force directions are hence decoupled from each other. In conventional machine tools, only the direction of the feed force, i.e., the q-component is operational, because the machine carriage moves in the direction of the feed force. The attractive force is not controlled in conventional machine tools, so that the current of the d-component is always set to zero. 
   It would therefore be desirable and advantageous to provide an improved method and device for damping chatter oscillations in a machine tool, which obviates prior art shortcomings and is able to specifically operate with a linear motor controlled with a single field controller. 
   SUMMARY OF THE INVENTION 
   It has been observed that chatter oscillations that occur at a position of the linear motor produce an excursion in the direction of the attractive force. Such excursions can be damped with forces that are applied in the opposite direction of the attractive force. The forces in the direction of the attractive force are controlled by the so-called d-component of the motor current. 
   According to one aspect of the invention, a method for attenuating a chatter oscillation in a processing machine with at least one feed system which includes a linear motor controlled by a field controller, includes the steps of generating an actual signal that is proportional to the chatter oscillation; comparing the actual signal with a predetermined desired value for a chatter oscillation for determining a control variable; and applying the control variable as a desired current value of a secondary current control of the field controller for controlling a current of the linear motor. 
   Accordingly, a setpoint (also referred to as desired value) is generated for the d-component of the motor current as a function of the chatter oscillation. The occurring chatter oscillation is initially measured. This actual signal is regulated to a predetermined desired value for an occurring chatter oscillation, producing a control variable which is applied as a current setpoint for the d-component of the motor current to a secondary current controller for the d-axis of a field control of the linear motor. The linear motor thereby produces a transverse force which corresponds the excursion caused by the chatter oscillation and opposes the chatter oscillation. 
   According to another aspect of the invention, a device for attenuating a chatter oscillation in a processing machine with at least one feed system driven by a linear motor includes an acquisition system for generating an actual signal which is proportional to the chatter oscillation, a control circuit having a first input connected to an output of the acquisition system, and a second input receiving a predetermined desired value for the chatter oscillation, wherein the control circuit produces at an output of the control circuit a signal representing a d-component of a magnetic field in the linear motor; and a current control circuit connected to the output of the control circuit. The current control circuit produces, in response to the d-component, a field current in the linear motor that attenuates the chatter oscillation. 
   According to an advantageous feature of the invention, an acceleration value of the chatter oscillation can be measured and integrated to produce an actual velocity signal representing the chatter oscillation. Alternatively, a velocity of the chatter oscillation can be measured directly. Optimal results can be obtained when the predetermined desired value for a chatter oscillation is set to zero. 
   According to another advantageous feature of the invention, the controlled current applied to the stationary (movable) section has a phase relative to the magnetic field of the movable (stationary) section so as to produce an attractive force between a movable section and a stationary section of the feed system. The desired phase relationship can be easily implemented by supplying current to the linear motor via a converter. 
   Since the chatter oscillation is a mechanical oscillation, it can be measured either by measuring the velocity or the acceleration in the direction of the attractive force of the linear motor. According to an advantageous feature of the invention, an actual signal which is proportional to the chatter oscillation is generated by an acquisition system which can include a seismic acceleration sensor and an integrating circuit receiving a signal from the seismic acceleration sensor. A seismic sensor can be attached directly at the location where the chatter oscillation occurs and does not require a reference point. Alternatively or in addition, the acquisition system may include an optical sensor and an integrating circuit receiving a signal from the optical sensor. Other sensors capable of measuring a velocity or an acceleration can also be used. 
   The control circuit can include a comparator which compares the signals received from the acquisition system with a predetermined desired value for the chatter oscillation, a regulator connected to an output of the comparator, and a limiter connected to an output of the regulator, wherein the limiter produces the signal representing the d-component of the magnetic field in the linear motor. 
   With the process of the invention, any occurring chatter oscillation can be easily damped in a processing machine that has a feed system with a field-operated converter-fed linear motor. 
   The control circuit for controlling chatter oscillations can be integrated in the field control for the d-axis, for example as a software module that can be switched in and out. Accordingly, an acquisition system with at least one sensor has to be attached only at the location where the chatter oscillations are generated. 

   
     BRIEF DESCRIPTION OF THE DRAWING 
     Other features and advantages of the present invention will be more readily apparent upon reading the following description of currently preferred exemplified embodiments of the invention with reference to the accompanying drawing, in which: 
       FIG. 1  shows a control structure of the conventional field control of a permanent-excited synchronous motor; 
       FIG. 2  shows a linear motor of a processing machine (not shown) with a magnetic field distribution and a primary field in the feed direction, 
       FIG. 3  shows a linear motor with a magnetic field distribution and a primary field in the direction of the attractive force, 
       FIG. 4  shows a first embodiment of a device for carrying out the method of the invention, and 
       FIG. 5  shows a second embodiment of the device for carrying out the method of the invention. 
   

   DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS 
   Throughout all the Figures, same or corresponding elements are generally indicated by same reference numerals. These depicted embodiments are to be understood as illustrative of the invention and not as limiting in any way. 
   Turning now to the drawing, and in particular to  FIG. 1 , there is shown a permanent-excited synchronous motor  2 , with a rotor position sensor  4 , a brake  6 , a converter  8 , in particular an intermediate voltage converter, and a conventional field control  10 . The stator of the permanent-excited synchronous motor is powered by the converter  8 . The conventional field control  10  includes a rotation speed control circuit  12 , two current control circuits  14 ,  16  as well as two conversion circuits  18  and  20 . The field control  10  also includes a differentiating circuit  22  and a conversion device  24 . 
   The rotation speed control circuit  12  includes a rotation speed controller  26 , a comparator  28  and a limiter  30 . A predetermined rotation speed setpoint n* is applied to the non-inverting input of the comparator  28 , whereas a measured actual rotation speed value n is applied to the inverting input. The actual rotation speed value n is generated by the differentiating circuit  22  from the position signal R generated by the rotor position sensor  4 . The output of the comparator  28  is connected to an input of the rotation speed controller  26 , with the output of the rotation speed controller  26  being connected to the limiter  30 . The output of the limiter  30  produces the setpoint signal i* q  of the secondary current control circuit  14 . 
   The current control circuit  14  includes a comparator  34  and a current controller  32  connected to an output of the comparator  34 . A second current control circuit  16  also includes a comparator  38  and current controller  36  connected to an output of the comparator  38 . The outputs of the two current control circuits  14  and  16  are connected to corresponding inputs of a conversion circuit  20  which converts the two orthogonal setpoints U* q  and U* d  of the field voltage into three voltage setpoints U* r , U* s  and U* t  for the stator. The voltages U* r , U* s  and U* t  represent the voltage setpoints of the permanent-excited synchronous motor. 
   The stator currents i r  and i s  of the permanent-excited synchronous motor  2  are measured, and an input-side conversion circuit  18  converts the stator currents i r  and i s  into two orthogonal field current components i q  and i d  of a stator current space vector of the synchronous motor  2 . The current components i q  and i d  are supplied to corresponding inverting inputs of the comparators  34  and  36  of the two current control circuits  14  and  16 , as described above. The current component i q , which is also referred to as a torque-forming current, is applied to the inverting input of the comparator  34 . A setpoint of the current component i d , which is also referred to as a flux-forming current component and has a value of zero, is applied to the non-inverting input of the comparator  38 . Each of the two conversion circuits  18  and  20  requires information about the rotor position angle φ, which is generated by the conversion device  24  from the rotor position signal R of the rotor position sensor  4 . 
     FIG. 2  shows a linear motor  40  of a feed system of a processing machine (not shown in detail). The motor  40  includes a primary section  42  and a secondary section  44 . The secondary section  44  of the linear motor  40  is adapted to hold a tool  46 , for example a cutting tool. The secondary section  44  of the linear motor  40  includes a plurality of permanent magnets  48  which are arranged side-by-side along the secondary section  44 . The depicted magnetic field distribution  50  depends on the particular arrangement of the permanent magnets  48 . A primary field with a q-component  52  and a d-component  54  (see  FIG. 3 ) is produced in the primary section  42  of the linear motor  40 . 
     FIG. 2  shows the q-component  52  of the primary field of the linear motor  40 . The q-component  52  of the primary field is shifted by 90° elec. with respect to the magnetic field distribution of the permanent magnets  48  of the secondary section  44  of the linear motor  40 . The d-component  54  of the primary field of the linear motor  40  is shown in more detail in FIG.  3 . The d-component  54  of the primary field is in phase with the magnetic field distribution  50  of the permanent magnets  48 . The q-component  52  of the primary field is produced when the linear motor  40  is energized in the feed direction. Conversely, the d-component  54  of the primary field is produced when the linear motor  40  is energized in the direction of the attractive force. The q- and d-components can be linearly combined and applied simultaneously. In conventional servo drives, only the q-component is used to move a secondary section relative to a primary section in a linear motor. 
     FIG. 2  also shows a workpiece  56  to be machined by an exemplary cutting tool  46 . The workpiece is omitted from  FIG. 3  for sake of clarity. A workpiece can be machined eccentrically by moving the secondary section  44  of the linear motor  40  back and forth in the feed direction. This motion is indicated by the double arrow  58 . Machining the workpiece  56  in this way can generate chatter oscillations, as indicated by the arrows  60  and  62 . Chatter can render the surfaces of the workpiece  56  unusable. Chatter is frequently caused when the machine structure mechanically yields to the cutting forces. Periodic excursions occur in particular, when the cutting force oscillations have a frequency in the range of a characteristic resonant frequency of the machine. The periodic machine excursions due to chatter can also produce periodic discontinuities in the cutting force which can have a phase relationship to the machine resonances that sustain and/or even amplify chatter. In particular, with materials requiring a large cutting force or a large cutting depth, the onset of chatter oscillations can reduce or limit the machine productivity. The cutting depth may therefore have to be reduced so as to reliably eliminate chatter. 
     FIG. 4  depicts a linear motor  40  of a feed system of a processing machine (not shown in detail) according to  FIG. 2  coupled to a device for carrying out the method of the invention. The device includes an acquisition system  64  that generates an actual signal S RS  which is proportional to the chatter oscillation, and a control circuit  66 . The control circuit  66  is electrically connected to an output of the acquisition system  64 . In its simplest embodiment, the control circuit  66  includes a comparator  68 , a controller  70 , in particular a PI-controller, and a limiter  72 . A setpoint signal S* RS  for the chatter oscillation is applied to the non-inverting input of the comparator  68 . The measured actual signal S RS  of an occurring chatter oscillation is applied to the input of the acquisition system  64 , with the output of the acquisition system  64  being connected to the inverting input of the comparator  68  of the control circuit  66 . The output of the comparator  68  is connected to the input of the controller  70 , and the limiter  72  is connected to the output of the controller  70 . The output of the limiter  72  produces a control variable S RSY  which is supplied as a setpoint signal i* d  to the current control circuit  16  for the d-component of the field control  10  depicted in FIG.  1 . The control variable S RSY  is indicative of a correction that has to be applied to the actual signal S RS  of an occurring chatter oscillation, such that the setpoint signal S* RS  for the chatter oscillation has a predetermined value. The value for the setpoint signal S* RS  is set to zero, since any chatter oscillation present can render surfaces of the workpiece  56  unusable. 
   In the embodiment illustrated in  FIG. 4 , the acquisition system  64  that generates an actual signal S RS  proportional to the occurring chatter oscillation includes a seismic acceleration sensor  74  and an integrating circuit  76 . The exemplary seismic acceleration sensor  74  is a piezo sensor which does not require a reference point. As a result, the seismic acceleration sensor  74  can be placed directly on the tool  46 . The output signal S RSa  of the seismic acceleration sensor  74  is the acceleration a of an occurring chatter oscillation in the direction of the attractive force of the linear motor  40 . The integrating circuit  76  generates from the determined output signal S RSa  a corresponding velocity signal which is supplied as the actual signal S RS  to the inverting input of the comparator  68  of the control circuit  66 . 
   The actual velocity signal S RS  and a predetermined velocity signal setpoint S* RS  can be used to generate a setpoint S RSY , which is supplied as a current setpoint i* d  to the secondary current control circuit  16  for the d-component of the motor current of the field controller  10 . The secondary current control circuit  16  for the d-component regulates the attractive force in the linear motor  40  so as to counteract the velocity of the occurring chatter oscillation. In this way, the velocity of the chatter oscillation is controlled to the predetermined value of the setpoint signal S* RS . 
     FIG. 5  shows a second embodiment of the device for carrying out the method for damping an occurring chatter oscillation in a processing machine with at least one feed system. This embodiment is different from the embodiment of  FIG. 4  in that the acquisition system  60  includes an optical sensor  78  and a signal processor  80 . The optical sensor  78  is used to measure the velocity of the occurring chatter oscillation in the direction of the attractive force of the motor. The output signal of the optical sensor  78  is supplied to the signal processor  80  which generates an actual signal S RS  which is proportional to the chatter oscillation. 
   The method of the invention can be used when chatter oscillations that have a component in the direction of the attractive force extend into the air gap space of the linear motor  40 . The method of the invention does not depend on the particulars by which a chatter oscillation is detected or measured. The method of the invention advantageously uses the previously unused d-component of the field controller  10  to dampen chatter oscillations. The method of the invention can advantageously be implemented with a single acquisition system  64  and a single control circuit  66 . The control circuit  66  can subsequently be integrated with other field controllers, for example, as a software module. The software module can also be activated on demand, so that the method of the invention operates only in the presence of chatter oscillations. The acquisition system  64  depicted in  FIG. 4  operates with a piezo sensor which does not require a reference point and can therefore determine the velocity of an occurring chatter oscillation. Moreover, the seismic acceleration sensor  74  is small enough to be placed in close proximity to a location where a chatter oscillation is generated. 
   While the invention has been illustrated and described in connection with currently preferred embodiments shown and described in detail, it is not intended to be limited to the details shown since various modifications and structural changes may be made without departing in any way from the spirit of the present invention. The embodiments were chosen and described in order to best explain the principles of the invention and practical application to thereby enable a person skilled in the art to best utilize the invention and various embodiments with various modifications as are suited to the particular use contemplated.

Technology Category: 4