Procedure and apparatus for braking a synchronous motor

Abstract: The invention relates to a procedure and an apparatus for braking a synchronous motor (2) magnetized with permanent magnets. According to the invention, there is connected to the input connectors (38,40,42) of the synchronous motor a non-linear braking resistor (60) by means of which the stator windings of the synchronous motor (2) are closed.

Description: The present invention relates to a procedure as defined in the preamble of claim 1 and to an apparatus as defined in the preamble of claim 5 for the braking of a synchronous motor. Safe operation of an elevator in the case of a malfunction, such as a power failure, is ensured by using a mechanical brake, which is often additionally backed up by employing electric, so-called dynamic braking. In dynamic braking, mechanical energy of the elevator is transmitted via the motor to a load external to the motor. At least this prevents acceleration of the elevator even if the mechanical brake should be inoperative. When an asynchronous motor is used, dynamic braking is only possible if a d.c. current is supplied into the primary winding. This generally requires special arrangements and the use of accessories such as separate rectifying equipment designed for the purpose. In the case of a d.c. motor, the braking can be implement by connecting a resistor to the rotor circuit, as disclosed in US 5,291,106. In this case it is required that the magnetization of the motor is in working order. In the case of a synchronous motor, dynamic braking can be implemented in a manner corresponding to the d.c. motor. The braking power and the current flowing through the braking resistor become large if the stator windings are shorted when the motor runs at full speed. On the other hand, at a low speed it is necessary to make sure that a sufficient torque is gererated to achieve a low sink speed. This is shown in US 4,667,776 even in case of an asynchronous motor. The object of the invention is to develop a new and advantageous dynamic braking system for a synchronous elevator motor. To achieve this, the procedure of the invention is characterized by the features of claim 1. The apparatus of the invention is characterized by the features of claim 5. Other preferred embodiments of the invention are characterized by the features presented in the subclaims. The solution of the invention allows dynamic braking of a synchronous motor to be achieved at a very low cost. To implement the solution in practice, only one contact pair is required, which is needed in any case to discharge the intermediate circuit capacitor of the frequency converter. A non-linear resistance ensures that the sink speed is as low as possible. The same safety level is achieved for an elevator driven by a synchronous motor as for one with a worm gear, which means that the elevator will not fall down fast even if the brake should fail. This is specifically achieved by an embodiment of the invention in which the winding is shorted at zero speed or the braking resistance is adjusted to a sufficiently low value. The solution of the invention can be used in connection with various power supply devices controlling the motor, by mounting the dynamic braking resistors either in the d.c. intermediate circuit or on the motor terminals. In the following, the invention is described in detail by the aid of one of its embodiments by referring to the drawings, in which Fig. 1 presents a circuit solution as provided by the invention, Fig. 2 presents the characteristic of the dynamic braking resistor, and Fig. 3 presents another solution according to the invention. Fig. 1 illustrates the basic circuit arrangement of a frequency converter with an intermediate circuit, used for the control of a synchronous motor 2. The frequency converter comprises a mains bridge 4, which rectifies a three-phase mains supply voltage applied to the input conductors 12, 14 and 16. Connected between the supply mains and the mains bridge is a mains filter 18 consisting of coils and capacitors, and a three-phase mains switch 20. The mains bridge feeds the rectified voltage into the intermediate circuit conductors 22 and 24, which are interconnected by capacitors 23 and 25 connected in series. Connected in parallel-inverse with each diode 6 - 11 is a transistor 26 - 31. By appropriately controlling these transistors, it is possible to return braking power into the mains if desired. Connected to the intermediate circuit conductors 22 and 24 is the motor bridge 5 of the frequency converter, which consists of a bridge circuit of transistors 32 - 37. The output from the a.c. side of the motor bridge is connected to the motor input terminals 38, 40 and 42 to pass a current to the stator windings. Transistors 32 - 37 are so controlled that the supply voltage of the synchronous motor has an amplitude and frequency as required by the operation. The mains bridge is controlled by control unit 44 and the motor bridge by control unit 46. On the basis of measured and reference quantities, such as current and voltage measurements, speed measurement 49 and speed reference 50, the control units 44,46 generate control pulses and apply these to the control inputs of the transistors via control conductors 51. When the present invention is used, the control of the transistors can be implemented using one of several techniques known in themselves. The control unit also controls the mains switch 20 via control conductor 68. Connected in parallel-inverse with the transistors 32 - 37 are diodes 52 - 57. The synchronous motor is magnetized with permanent magnets, so the motor preserves its magnetization during possible power failures. The motor is mechanically linked to the traction sheave (not shown) of the elevator to enable the elevator car to be moved by means of hoisting ropes. Connected between conductors 22 and 24 in the intermediate circuit of the frequency converter are braking resistors 58 and 60 in series with a braking transistor 62. During normal operation, control unit 46 controls transistor 62 in such a way that the power generated by the motor is at least partially consumed in the braking resistors. Braking resistor 58 is a normal braking resistor used to consume the returning power. Braking resistor 60 has a non-linear voltage-current characteristic as shown in Fig. 2. Its resistance is larger for high voltage values than for low voltages, corresponding to the use of a metallic resistor subject to heating as e.g. in the incandescent bulb. In other words, a resistor is used in which a rise in temperature increases the resistance in the operating range. The braking resistor may also be a PTC resistor or a VDR resistor. Connected in parallel with braking resistor 58 and transistor 62 is a contactor 64 which can be used to connect only braking resistor 60 between the intermediate circuit conductors 22 and 24. Moreover, connected in parallel with the non-linear braking resistor 60 is a contactor 66 by means of which the resistor 60 can be shorted. Contactors 64 and 66 are connected in series, allowing them to be used to short the intermediate circuit conductors 22 and 24. According to the invention, dynamic braking is activated when the system detects an anomalous operating condition, such as a break in the power supply, or an overspeed condition in which the overspeed governor is triggered. At the same time, contactor 64 is closed, with the consequence that the stator circuit of the motor is closed via supply conductors 38, 40 and 42, diodes 52 - 57 and the non-linear resistor 60. The contactor is controlled by the electromotive force generated in the motor windings. The frequency converter is preferably disconnected from the mains by means of the mains switch 20. If the motor is running at a high speed at the closing instant of the contactor 64, e.g. when the overspeed governor is triggered, the voltage across the resistance is high and, correspondingly, the resistance is also high, so that the current and therefore the braking torque is limited to the maximum value thus determined. If it is assumed e.g. in the case of Fig. 2 that the relative value u/[pu]=1 (pu=per unit) of the voltage corresponds to full speed and the relative value i/[pu]=1 of the current corresponds to acceleration, then it can be assumed that the balanced torque for full load is about 1/3. In the case of a linear resistor, the speed would be about 33 %, whereas in the case of a non-linear resistor the speed is about 17 %. The resistor used in the above example is an incandescent lamp type resistor. In this case, a current peak may occur at the instant the connection is made. This can be obviated by initially connecting a linear resistor in series with the non-linear resistor. In the example of Fig. 1, this is implemented using a normal braking resistor 58 and a transistor 62 to connect it. During normal operation, resistors 58 and 60 and the braking transistor are used to control braking. Braking resistor 60 can be replaced with a number of resistors in series that are shorted by respective contactors as the speed changes. In this case the non-linearity in the resistance value is determined on the basis of the control of the contactors. The contactor 66 connected in parallel with resistor 60 is used to short the resistor 60 when the motor speed is zero. In this way a higher braking torque is achieved in case the brake fails. In this event the contactor can be fed with the voltage across resistor 60 or with a voltage obtained directly from the motor winding, in which case the fall in the motor speed automatically drops out the contactor 66. In the solution of the invention depicted in Fig. 1, it should be noted that there is no contactor between the braking resistor and the motor windings, but the braking resistor is connected directly via the diode bridge to the stator windings of the motor, which means that operation is ensured even during a power failure, provided that the magnetization of the motor is in operation, which is best achieved by using a synchronous motor magnetized with permanent magnets. Fig. 3 presents another embodiment of the invention, in which the synchronous motor 2 is fed by a frequency converter 70 which may be like the one in Fig. 1 or a different type. As in Fig. 1, the converter 70 is connected to the supply mains and to the motor 2. The frequency converter 70 is controlled by a control unit 146 generating control pulses that are passed via conductors 151 to the switches in the frequency converter 70. By means of a contactor 42, star-connected non-linear resistors 78, 80 and 82 are connected to the output terminals of the frequency converter. Contactor 84 is controlled by the control unit 146 in a manner corresponding to the control of contactor 64 in Fig. 1. In this embodiment, dynamic braking thus occurs completely outside the frequency converter. The invention has been described above by the aid of some of its embodiments. However, the presentation is not to be regarded as constituting a limitation of the sphere of patent protection, but its embodiments can be varied within the limits defined by the following claims.

Claims: Procedure for braking a synchronous motor (2) magnetized with permanent magnets, which synchronous motor (2) has input connectors (38,40,42) for the supply of a voltage into the stator windings, whereby at least one braking resistor (60;78,80,82) connected to the input connectors ( 38,40,42) of the synchronous motor is used to close the stator windings, of the synchronous motor (2), characterized in that a no-linear braking resistor (60;78,80,82) is used to close the stator windings of the synchronous motor (2), whereby the resistance value of the non-linear braking resistor (60;78,80,82) is chosen to increase as the voltage increases. Procedure as defined in claim 1, in which the synchronous motor (2) is fed by a frequency converter (3) with an intermediate circuit (22,24), characterized in that the braking resistor (60) is connected to the intermediate circuit (22,24) of the frequency converter. Procedure as defined in claim 2, characterized in that the stator windings are short-circuited when the speed of the motor (2) is substantially zero. Procedure as defined in claim 3, in which the motor is magnetized with permanent magnets, characterized in that a contactor (64) is used to connect the braking resistor (60), which contactor can be controlled by the electromotive force of the motor. Apparatus for braking a synchronous elevator motor (2) provided with input connectors (38,40,42) for the supply of a voltage into the stator windings, whereby at least one braking resistor (60;78,80,82) is connected to the input connectors (38,40,42) of the synchronous motor by means of which the stator windings of the synchronous motor (2) can be closed, characterized in that the braking resistor is a non-linear braking resistor (60;78,80,82), whereby the resistance value of the braking resistor (60) increases as the voltage increases. Apparatus as defined in claim 5, in which the synchronous motor (2) is fed by a frequency converter (3) provided with an intermediate circuit (22,24), characterized in that the braking resistor (60) and a switch (64) that connects the braking resistor are mounted between the d.c. conductors (22,24) of the intermediate circuit (22,24) of the frequency converter. Apparatus as defined in claim 6, characterized in that it is provided with a switch (66) connected in parallel with the braking resistor (60), allowing the stator windings of the motor (2) to be short-circuited. Apparatus as defined in claim 5 or 6, in which the synchronous motor is magnetized with permanent magnets, characterized in that the braking resistor (60) can be connected by a switch (64) that can be controlled by the electromotive force of the motor (2).

Inventors: AULANKO ESKO, HAKALA HARRI, MUSTALAHTI JORMA, AULANKO, ESKO, HAKALA, HARRI, MUSTALAHTI, JORMA
Applicants: KONE CORP, KONE CORPORATION
Application year: 1995
Main classification: H02P3
IPC codes: H02P3, H02P6, B66B1