PREVENTIVE FUNCTION CONTROL IN AN ELECTROMAGNETIC SPRING PRESSURE BRAKE

Abstract

The invention relates to a method for preventive function control in an electromagnetic spring pressure brake for a simpler and more accurate determination of the critical operating state. The spring pressure brake comprises at least one coil, and an armature disk, a coil carrier having compression springs distributed thereon, a control module, and a monitoring module having at least one semiconductor component, a current measuring device, and a voltage measuring device, wherein the method comprises the following steps: Initially, the spring pressure brake is controlled by the control module by means of a voltage. Next, the state variables current (I) and voltage (U) at the electromagnetic spring pressure brake are measured by the monitoring module. Subsequently, a determination variable (T; F) of the electromagnetic spring pressure brake is determined by the monitoring module. Said determination variable (T; F) is summed over a range (a), which extends from the starting point of the actuation to a point (W), at which the armature disk begins to move. At the point (W), a current value is detected, at which the movement of the armature disk begins. The determination variable (T; F) is additionally summed over a range (b), which extends from the point of actuation, when the current (I) again reaches the value detected above, up to the point, at which a constant current is reached. Subsequently, a ratio (X) is calculated from the sum of the determination variable over the range (a) to the sum of the determination variable over the ranges (a) and (b). Upon reaching or exceeding a predetermined value (Y) by the value of the ratio (X), a state signal relating to the spring pressure brake is output.

Claims

1. Method for preventive function control of at least one electromagnetic spring-loaded brake, which at least: comprises a coil, as well as an armature disk; a coil carrier with compression springs distributed thereon; a control module; and a monitoring module with at least: a semiconductor component, a current measuring device, and a voltage measuring device; wherein the method includes: (i) activating the spring-loaded brake with a voltage by the control module; (ii) measuring state variables current (I) and voltage (U) at the electromagnetic spring-loaded brake by the monitoring module; (iii) determining a parameter (T; F) during the activation of the electromagnetic spring-loaded brake by the control module; (iv) summing the parameter (T; F) over a range (a) which extends from a starting point of the activation (12) to a point (W) at which the armature disk begins to move; (v) detecting a current value at the point (W) at which the armature disk begins to move; (vi) summing of the parameter (T; F) over a range (b) which extends from the starting point of the activation when the current (I) again reaches the value detected in step (v) to a point at which a constant current is achieved; (vii) calculating a ratio (X) from the sum of the parameter (T; F) over the range (a) to the sum of the parameter over the ranges (a) and (b); (viii) outputting a status signal upon the value of the ratio (X) reaching or exceeding a predetermined value (Y).

2. The method according to claim 1, characterized in that the parameter (T) is time.

3. The method according to claim 1, characterized in that the parameter (F) is the linked flux.

4. The method according to claim 1, wherein detecting a current value at the point (W) at which the armature disk begins to move includes: (i) calculating a further state variable from the measured state variables current (I) and voltage (U) and from a resistance value of the coil (Rs) or from a variable derived from the measured state variables current (I) and voltage (U) and from the resistance value of the coil (Rs); (ii) comparing the further state variable with a predefined value/course of this further state variable stored in the monitoring module for movement of the armature disk in the spring-loaded brake; and (iii) determining and outputting the current value at the point (W) at which the movement of the armature disk begins.

5. The method according to claim 4, characterized in that the variable derived from the measured state variables current (I) and voltage (U) is the synchronized moving average or comparable higher-order filter function of the measured state variable current (I) and voltage (U).

6. The method according to claim 4, characterized in that the further state variable is an inductance (L).

7. The method according to claim 4, characterized in that the further state variable is a change in inductance (dL/dt).

8. The method according to claim 4, characterized in that the further state variable is an induced voltage (U.sub.ind).

9. The method according to claim 1, characterized in that the electromagnetic spring-loaded brake is controlled by the control module with a DC voltage.

10. The method according to claim 1, characterized in that the electromagnetic spring-loaded brake is controlled by the control module with a pulsating DC voltage.

11. The method according to claim 1, characterized in that the electromagnetic spring-loaded brake is a damped or undamped electromagnetic spring-loaded brake.

12. The method according to claim 1, characterized in that the value (Y) is 50% to 80%.

13. The method according to claim 1, characterized in that the value (Y) is 80% to 90%.

14. The method according to claim 1, characterized in that the value (Y) is 90% to 99%.

Description

DESCRIPTION OF THE FIGURES

[0018] FIG. 1 shows as a block structure the physical conversion processes that take place during the operation of an electromagnetic spring-loaded brake.

[0019] FIG. 2 shows the measured state variables current (I) and voltage (U) upon switching on (releasing) an electromagnetic spring-loaded brake with a DC voltage.

[0020] FIG. 3 shows the measured state variables current (I) and voltage (U) upon switching on (releasing) an electromagnetic spring-loaded brake with a pulsating DC voltage.

[0021] FIG. 4 shows the curve of the linked flux versus the current drop at the spring loaded brake during a switch-on process of an electromagnetic spring-loaded brake.

[0022] FIG. 5 shows the curve of the current drop across the spring loaded brake versus time during a switch-on process of an electromagnetic spring loaded brake.

[0023] FIG. 6 shows the curve of the inductance during a switch-on process of an electromagnetic spring-pressure brake with a pulsating DC voltage.

[0024] FIG. 7 shows the progress of the change in inductance during a switch-on process of an electromagnetic spring-loaded brake with a pulsating DC voltage.

DETAILED DESCRIPTION

[0025] In FIG. 1, the at least one electromagnetic spring-loaded brake is shown as a block structure (1), wherein the movement of the armature disk in the spring-loaded brake can be described as a sequence of different physical conversion of energy processes (2, 3, 4). The named physical conversion processes (2, 3, 4) are detailed below and are stored in a monitoring module as a model-based description of the armature disk movement in the spring-loaded brake.

[0026] The supplied electrical energy (5) in the form of DC or pulsating DC from an electrical energy source is subjected to several energy conversion processes when the spring-loaded brake is in operation. At the outset, the brake as an electromagnetic actuator can be described as an electro-magnetic energy converter (2). The electrical energy experiences a conversion from electrical energy into magnetic energy (3) and concurrently a conversion from potential energy into kinetic energy (4). The conversion of potential energy into kinetic energy takes effect in the electromagnetic actuator through a movement (release) of the armature disk towards the coil carrier. At the same time as the armature disk is released, further energy conversions take place. When the armature disk moves, the kinetic energy is converted into potential energy, this conversion ending when the armature disk has reached the open position. At the same time, a magneto-mechanical energy conversion takes place (3), so that in the last conversion step the originally electrical energy is stored in the mass spring system of the spring-loaded brake. When the brake is closed, i.e. when the armature disk moves from the open to the closed position, the physical conversion processes described take place. These are not free of retroactive effects and are reflected in the model-based description of the armature disk movement. The model-based description includes predefined values that correspond to the movement of the armature disk in the spring-loaded brake.

[0027] The model-based description contains the values and the progress of state variables such as current (I) or voltage (U) or variables derived from the state variables such as in particular inductance, change in inductance or the induced voltage. The various predefined values from the model-based description of the armature disk movement in a spring-loaded brake are related to the various operating states of an electromagnetic spring-loaded brake.

[0028] Various operating states of a spring-loaded brake are described below. At the beginning of operation or to open an electromagnetic spring-loaded brake, this is switched on, i.e. supplied with a voltage (pulsating DC or DC). As a result of a sufficient voltage supply, the armature disk moves from a closed (applied) position to an open (released) position. The spring-loaded brake is then in an open operating state. At the end of operation or when closing (braking) an electromagnetic spring-loaded brake, the power supply is interrupted, i.e. the spring-loaded brake is not or not sufficiently supplied with a voltage (AC or DC). As a result of a missing or insufficient power supply, the armature disk moves from the open position to the closed position. The spring-loaded brake is then in a closed operating state. Additionally, the spring-loaded brake can include the operating state of partial application, particularly in the case of damped spring-loaded brakes. Here, the armature disk is supplied with a voltage to such an extent that the armature disk slowly moves between the open and closed position within the spring-loaded brake. Depending on the voltage supply, the armature disk moves slowly upwards or downwards.

[0029] The model-based description of the movement of the armature disk in relation to the possible operating states of the spring-loaded brake is stored in a monitoring module. The monitoring module comprises at least one semiconductor component, in particular a microprocessor, and at least one current measuring device and/or a voltage measuring device.

[0030] By means of a control module, which is connected to the at least one spring-loaded brake and the monitoring module, the spring-loaded brake can be given an operating state and supplied with the voltage corresponding to the operating state.

[0031] FIG. 2 shows an exemplary current (6) and voltage (7) curve when an electromagnetic spring-loaded brake is switched on with a DC voltage. In this case, the spring-loaded brake is activated with a voltage via a control module and an operating state to be achieved can be specified, in this case an open operating state. As a result of the application of a suitable DC voltage to the at least one spring-loaded brake, the current builds up according to an exponential function. As soon as the above-described physical conversion processes of the electrical energy have progressed so far that the armature disk moves towards the coil carrier, this movement is also reflected in particular in the state variable current (6). As shown in FIG. 2, the movement of the armature disk causes a characteristic drop in the curve of the state variables current (6). Following this characteristic drop, the current rises again during the movement of the armature disk, following the exponential function of the inductive switch-on process, until it reaches a constant current value after the open operating state has been reached.

[0032] FIG. 3 shows an exemplary current (8) and voltage (9) curve when an electromagnetic spring-pressure brake is switched on with (mains) AC with a bridge rectifier. Here, the voltage curve (9) shows a pulsating DC voltage and the current curve (8) shows a rising curve, this curve being overlaid by a wave structure. In addition, the synchronized moving average value for the measured state variables current (10) and voltage (11) is shown in FIG. 3 as a derived variable. Synchronized moving average in this context means that the length of the moving average of the measured current and voltage values is set and synchronized to an integer multiple of the half period of the mains frequency of the input voltage that is common on site. In particular, the moving average values are synchronized to the common mains frequencies of 50 Hz or 60 Hz. In addition, equivalent higher-order filtering methods can alternatively be used instead of the synchronized moving average.

[0033] In FIG. 4, the curve of the linked flux (13) is plotted against the current applied to the brake, specifically for the control (12) of the spring-loaded brake with a DC voltage, as shown in FIG. 2. In this case, the linked flux increases steadily from the starting point of the activation as the current increases. This steady increase in the linked flux with increasing current (I) is maintained up to a point (W) at which the movement of the armature disk within the spring-loaded brake begins. A current value that is measured by the monitoring module can be assigned to this point (W). Following the start of the movement of the armature disk in the electromagnetic spring-loaded brake, the current drops significantly, with the linked flux continuing to increase. In the further course of the movement of the armature disk, the current increases again as the linked flux continues to increase and again reaches the current value measured at point (W). Following this, the linked flux increases steadily together with the current, up to a constant value of the current. The magnetic flux goes into saturation, which means that despite a further increase in the current, the linked flux remains almost constant. The constant current value to be achieved results from the applied voltage and the resistance (Rs) of the coil. In order to determine the functionality of the spring-loaded brake, the parameter linked flux (F) is now summed in an area (a) and an area (b). For area (a), summation is from the starting point of activation to a point (W) at which the armature disk moves. At point (W), the associated current value at which the armature disk begins to move is recorded by the monitoring module.

[0034] For area (b), the parameter linked flux is summed, namely from the point of control from which the current value again reaches the current value of point (W) after the movement of the armature disk, up to the point at which a constant current is achieved.

[0035] Following the summation of the parameter linked flux over the ranges defined above, a ratio (X) is calculated from the sum of the parameter linked flux in range (a) to the sum of the parameter linked flux over ranges (a) and (b). The ratio (X) provides information about how large the reserve of the linked flux is for operating the brake. Depending on the type of brake used, in particular damped or undamped brake or depending on the brake size, a value (Y) is stored in the monitoring module, with a status signal being issued when this value (Y) is reached or exceeded by the value of the ratio (X). This status signal indicates that the limit value for wear of the brake has been reached or exceeded and/or, if necessary, maintenance or replacement of the spring-loaded brake should be carried out promptly. This method presented here can accordingly also be used for controlling a spring-loaded brake with a pulsating DC voltage.

[0036] In FIG. 5, the curve of the current (14) is plotted against the time when a spring-loaded brake is switched on, specifically for the control of the spring-loaded brake with a DC voltage as shown in FIG. 2. The current (I) increases steadily with increasing time from the starting point of activation. This steady increase in current over time is maintained up to a point (W) at which the armature disk begins to move within the spring-loaded brake. A current value that is measured by the monitoring module can be assigned to this point (W). Following the start of the movement of the armature disk in the electromagnetic spring-loaded brake, the current drops significantly with increasing time. As the armature disk movement continues over time, the current increases again and again reaches the current value determined at point (W). In the further course of time, the current increases steadily, up to a constant current value. The constant current value to be achieved results from the applied voltage and the resistance (Rs) of the coil.

[0037] To determine the functionality of the spring-loaded brake, the parameter time (T) is accordingly summed in an area (a) and an area (b). For area (a), summation is from the starting point of activation (12) to the point (W) at which the armature disk moves. The associated current value is recorded at the point (W) at which the armature disk begins to move. For area (b), parameter time is summed from the point of control from which the current value after the armature disk has returned to the current value of point (W) to the point at which a constant current is achieved.

[0038] Following the summation of the parameter time over the areas (a) and (b) defined above, a ratio (X) is calculated as the sum of the parameter time in area (a) to the sum of the parameter time over the areas (a) and (b). The ratio (X) provides information about the remaining reserve for releasing the spring-loaded brake. Depending on the type of brake used, in particular damped or undamped brake or depending on the brake group, a value (Y) is stored in the monitoring module, with a status signal being issued when this value (Y) is reached or exceeded by the value of the ratio (X). This state signal indicates that the limit value for the critical operating state of the brake has been reached or exceeded and/or that maintenance or replacement of the spring-loaded brake should be carried out promptly, if necessary. This method presented here can accordingly also be used for controlling a spring-applied brake with a pulsating DC voltage.

[0039] In FIG. 6, the curve of the inductance (15) is shown by way of example during a movement of the armature disk during a switch-on process with pulsating DC according to FIG. 3. In a first embodiment, the beginning of the movement of the armature disk can be determined on the basis of the curve of the inductance. The inductance was calculated from the synchronized moving average of current and voltage and from the resistance value (Rs) of the coil.

[0040] Immediately after switching on, the inductance (L) initially increases sharply, after which the inductance almost reaches a plateau. During this plateau, the above-described physical conversion processes of the electrical energy progress so far that the movement of the armature disk from the closed to the open state in the course of the inductance can be recognized from the renewed increase in the inductance (16). Following this renewed increase in the inductance, the inductance (15) decreases in the further course to an almost constant value. Preferably, the linked magnetic flux Ψ=Σ U.sub.IND can be determined to calculate the inductance (L). The brake is to be regarded as a series connection of inductance and ohmic resistance, whereby the voltage U.sub.IND induced by the applied voltage U, is reduced by the voltage value U.sub.RS dropping across the ohmic resistance of the coil, so that the induced voltage is U.sub.IND=U−U.sub.RS. Here, the falling voltage is U.sub.RS=I.Math.R where R.sub.RS is the resistance value (Rs) of the coil. The inductance L then results from the relationship L=Ψ/I. This method presented here can accordingly also be used for controlling a spring-loaded brake with DC. In a further embodiment of the invention, the beginning of the movement of the armature disk can be determined on the basis of the change in inductance (dL/dt).

[0041] FIG. 7 shows the change in inductance as a derivative with respect to time (17) from the curve of the inductance from FIG. 6. As a result of the application of the (mains) AC voltage, the change in inductance (dL/dt) increases rapidly to a maximum positive value (global maximum) then decrease again. During this fall, the above-described physical conversion processes of the electrical energy progress so far that the armature disk moves towards the coil carrier. The beginning of the movement of the armature disk is assigned to the turning point (19) in the curve of the change in inductance. This turning point corresponds to point (W) in the curve of FIGS. 4 and 5. A current value can be assigned to this turning point (19), which is used in the method described above in order to be able to carry out a preventive function control of the brake. The movement of the armature disk is reflected in the further course of the change in inductance (dL/dt) (17) through an increase. This local maximum (18) reflects the movement of the armature disk. Subsequently, the change in inductance drops during the movement of the armature disk, in order to remain at a constant value. This method presented here for determining the current value at the beginning of the movement of the armature disk can also be used to control a spring-loaded brake with DC.

LIST OF REFERENCE SYMBOLS

[0042] 1. Spring-loaded brake as a block structure [0043] 2. Electro-magnetic energy converter [0044] 3. Magneto-mechanical energy converter [0045] 4. Potential and Kinetic Energy [0046] 5. Energy source [0047] 6. Current curve—DC switch-on [0048] 7. Voltage curve—DC—switch on [0049] 8. Current curve—pulsating DC—switching on [0050] 9. Voltage curve—pulsating DC—switch on [0051] 10. Synchronized moving average of current [0052] 11. Synchronized moving average voltage [0053] 12. Starting point of the control [0054] 13. Linked flux [0055] 14. Curve of current [0056] 15. Curve of inductance [0057] 16. Change in inductance when the armature disk moves [0058] 17. Curve of the change in inductance over time (dL/dt) [0059] 18. Local maximum in the curve of the change in inductance [0060] 19. Point of inflection in the curve of the change in inductance [0061] I Current [0062] U Voltage [0063] a Area a [0064] b Area b [0065] T parameter time [0066] F parameter linked flux [0067] W Beginning of movement of the armature disk [0068] Rs Resistance of the coil [0069] X Value of the ratio [0070] Y Prescribed value [0071] L Inductance