Brushless Mortor|Basic

Methods of Sensorless 120° Commutation Driving Startup 1: Startup on Detection of Induced Voltage from Synchronous Operation

2023.08.30

Points of this article

・Upon startup of sensorless 120 commutation driving of a 3-phase full-wave brushless motor, because the position of the permanent magnet is not known when stopped, one of the following methods is used: ① startup on detection of the induced voltage from synchronous operation; ② startup on detection of the stopped permanent magnet position

・In method ①, a synthetic magnetic field is formed in a rotation direction regardless of the position of the permanent magnet, and upon switching at fixed times to start rotation of the permanent magnet and detecting the induced voltage that occurs, normal control is initiated.

・This method has the following problems.
--A synthetic magnetic field is formed regardless of the position of the permanent magnet, and so depending on the state, a torque in the opposite direction may act; depending on the stopped position of the permanent magnet, more time may be required for startup.
--Ordinarily, the positional relationship between the permanent magnet and the formed synthetic magnetic field in order for sufficient torque to occur is a difference of 90°, but because the synthetic magnetic field is formed regardless of the permanent magnet position, operation may be started from an angle such as 70° or 60°, so that a large startup torque cannot be obtained.

・To deal with these problems, method ② is adopted.

In the previous article, basic 120° commutation driving was used to explain sensorless driving of a 3-phase full-wave brushless motor. Here, startup methods specific to sensorless driving of 3-phase full-wave brushless motors are explained. As basic startup methods, two methods will be explained over the course of two articles: a method in which the induced voltage from synchronous operation is detected for startup, and a method in which the position of the stopped permanent magnet is detected to perform startup.

Problems with Startup of Sensorless 120° Commutation Driving of a 3-phase Full-Wave Brushless Motor

As explained in “Principles of Rotation of 3-Phase Full-Wave Brushless Motors” and “Position Detection in 3-Phase Full-Wave Brushless Motors”, in startup of a 3-phase full-wave brushless motor, when sensors are present the sensors can be used to ascertain the positions of the N and S poles of the permanent magnet (rotor) when stopped. Therefore, startup is performed by beginning to pass currents through the coils so as to generate a synthetic magnetic field at 90°, as in the diagram on the right.

When sensors are not present (that is, in sensorless driving), as explained in “Driving 3-Phase Full-Wave Brushless Motors: Sensorless 120°Commutation Driving“, the position detection is performed by using the induced voltage occurring in the coil which is not passing a current when the permanent magnet rotates. Hence while the motor is stopped, the position of the permanent magnet cannot be ascertained, and so a procedure for motor startup is needed. One such procedure is to detect the induced voltage due to synchronous operation in order to start the motor.

Methods of Sensorless 120° Commutation Driving Startup 1: Startup on Detection of Induced Voltage from Synchronous Operation

As stated previously, in sensorless driving, the position of the permanent magnet when stopped cannot be determined, and so it cannot be known what currents should be passed in the three coils upon startup. As one means to deal with this, synchronous operation is used to rotate the permanent magnet, the induced voltage that occurs is detected, and 120° commutation driving is then performed; this is explained using the diagram below.

: If the permanent magnet is in the position in ①, then ordinarily currents would be passed in the coils so as to form a synthetic magnetic field in the 6 o’clock direction; but because the permanent magnet position is unknown, a synthetic magnetic field is generated in a direction determined in advance (in the diagram, the 5 o’clock direction), regardless of the permanent magnet position.

: When this state is maintained for a fixed length of time, the S(N) pole of the permanent magnet is drawn toward the synthetic magnetic field N(S) pole, and the permanent magnet moves (rotates) clockwise a small amount.

③, ④: However, the movement is not yet sufficient to cause an induced voltage, and so a synthetic magnetic field is next generated in the 7 o’clock direction. The permanent magnet then similarly moves clockwise.

⑤, ⑥: Next a synthetic magnetic field is generated in the 9 o’clock direction; the permanent magnet moves still further in the clockwise direction, and begins to rotate.

This operation is continued, and the time until the next switching is shortened little by little, so that the permanent magnet rotation rate increases, and gradually the induced voltage rises to a level at which detection is possible. When a state is reached in which the induced voltage can be detected, normal sensorless 120° communication driving commences.

In other words, in this method a synthetic magnetic field is created in a rotation direction regardless of the position of the permanent magnet, and by switching at fixed times to start rotation of the permanent magnet, an induced voltage occurs and is detected, and normal control is begun.

In this method, if at the start the synthetic magnetic field switching occurs too quickly, the permanent magnet may not be able to follow, and so a method must be used in which the switching period begins slowly and is gradually quickened.

Function Block and Operation Waveforms of Induced Voltage Detection from Synchronous Operation

A function block diagram and operation waveforms for the operations explained above are presented.

A startup period generation oscillator sends a ST_CLK signal to a driving basic waveform generation block, and the signal causes a synthetic magnetic field to be generated in a direction determined in advance, regardless of the above-described permanent magnet position; the synthetic magnetic field is then switched in the direction of rotation according to the period of the signal.

BEMF_DET is a signal used to notify detection of an induced voltage. When this signal enters the startup period generation oscillator, the ST_CLK signal is stopped, BEMF_DET is input to the driving basic waveform generation block, generation of a synthetic magnetic field based on the induced voltage begins, and normal control commences.

Below are waveform examples illustrating the series of operations described above. The ST_CLK signal and BEMF_DET signal as well as the signal resulting from their addition (see the block diagram), and the output voltage waveforms A1 to A3, are relevant to the present explanation. The fact that the period of the BEMF_DET signal becomes shorter and shorter indicates that the rotation rate is increasing.

This startup method has the following issues.

  • ・A synthetic magnetic field is created regardless of the position of the permanent magnet, so that depending on the magnet state, a reverse-direction torque may act, and for some stopped positions of the magnet, time may be required for startup.
  • ・Originally, the relative positions of the permanent magnet and the created synthetic magnetic field should differ by 90° in order to generate a large amount of torque. But because the synthetic magnetic field is created irrespective of the permanent magnet position, motion may start from an angle such as 70° or 60°, so that the required large startup torque is not obtained.

The other method mentioned at the beginning of this article addresses these problems; in this method, the stopped position of the permanent magnet is detected to perform startup. The next article will describe this method.

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