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FOC Motor Control

Bike

I am currently using standard Brushless DC (BLDC) control which uses a 6 step method of controlling the motor. However, there is a different method of control called Field Oriented Control (FOC) which is more efficient and gives maximum torque. If you want less theory and a post about setting this up on a VESC controller, go to VESC FOC setup.

BLDC operation ⚙️

A BLDC motor is a bit of a misnomer because it's operating principle is closer to that of an AC motor than a DC motor. The reason it is called a DC motor is because the controller usually takes in a DC power source, so it looks to be running on DC from the end user's point of view.

It is constructed of usually a multiple of 3 coils where each multiple corresponds to a different phase wire. As seen in Fig 1.1 the three phases are 120 degrees out of phase with each other. Fig 1.1 is a simplified version of a BLDC motor because the coils can only be on or off.

simple-BLDC-motor

Fig 1.1 A simple binary version of a BLDC motor

A more realistic model of the BLDC motor has three sinusoidal waveforms (seen in Fig 1.2) for each phase instead of square waveforms as seen in Fig 1.1. Once these 3 phases are applied to the motor, it should rotate at a frequency equal to the frequency of the sine waves divided by the number of multiples of phases. So the example in Fig 1.1 would rotate at the same frequency because it has one multiple of coils.

phases
phases

Fig 1.2 The ideal phase voltages of a BLDC

Sensored vs sensorless 🔬

When applying the control signals to the motor, it is very important to know the position of the motor, since the phase of the sine wave is dependent on the exact position of the rotor. There are two methods of position measurement 1) sensored and 2) sensorless.

1. Sensored

Usually hall effect sensors are used to monitor how the permanent magnets of the rotor are oriented with regards to the stator. This gives very accurate phase information even when the rotor is stationary. Hall effect sensors measure magnetic fields through the hall effect and convert this measurment to some kind of signal. The sensors used in BLDC motors are usually latching sensors, which means that they have a HIGH impedance output when it detects a North/South pole and a LOW impedance output when the opposite pole is sensed.

hall-sensors
hall-sensors

Fig 2.1 The hall sensors that are in my hub motor

The three sensors are each placed at one of the phase wires. Therefore, three square waves are produced as the motor rotates, which are 120 degrees out of phase with each other (as seen in Fig 2.2). These signals are used to determine the rough position of the motor.

hall-sensor-output
hall-sensor-output

Fig 2.2 The hall sensor outputs as the motor rotates

2. Sensorless

Sensorless sensing uses the voltage induced in the windings by the permanent magnets to estimate the motor's position. This voltage is a result of Back ElectroMotive Force (BEMF). According to faraday's law, a changing magnetic field induces a voltage in a coil. Two of the three phases of the motor are driven, while the other phase is not driven but instead used to measure this back EMF as seen in Fig 2.3. The BEMF is at zero when the magnetic field is aligned with the coil. Therefore, a simple zero crossing detector can be used to detect the alignment of the motor.

back-emf-sensorless

Fig 2.3 Sensorless operation of a BLDC motor

This method of position sensing has some drawbacks however. Firstly, it requires a control method similar to trapezoidal control, which is not a very efficient control method. One of the phases cannot be driven for a period, which reduces the maximum torque output of the motor. Secondly, the motor cannot sense its position without moving. Therefore, when the motor is stationary, the motor has to either move in a random direction to figure out it's initial position, or activate one of the coils until the motor aligns to that coil's position.

6 step trapezoidal control 📈

Trapezoidal control is one of the simplest control methods for BLDC motors. This control method has 6 discrete voltage steps as seen in Fig 3.1. There are three voltage levels 1) battery negative 2) battery positive and 3) floating. It is at the floating voltage level that BEMF can be measured for position estimation if sensorless commutation is being used.

trapezoidal-control
trapezoidal-control

Fig 3.1 The output of each of the 6 phases of trapezoidal control

This control method is not ideal however because the torque is not always perpendicular to the magnetic field and the signal should ideally be sinusoidal. FOC is needed for this type of control, but that is explained in the next section. This form of control acts like carrots being placed in front of a character, as seen in Fig 3.2. When the character reaches the carrot, another carrot is placed in front of them. This leads to a choppy motion if the speed of the character is proportional to its distance from the carrot.

carrot

Fig 3.2 Carrot method has variable speed

FOC control 🌊

Field Oriented Control (FOC) attempts to create the optimal control signal for a motor. The previous example of carrots being placed in front of a character is improved by placing the carrot at a fixed distance at all time, as seen in Fig 4.1. The distance from the character is constant and optimally far away so that it moves smoothly and most efficiently 😄

carrot

Fig 4.1 Carrot on stick method has constant speed

Direct and quadrature axes

But it's not really that simple 😅 Firstly, let's look at the magnetic fields inside the motor. The stator is the stationary part of the motor (which is where the coils are, which are controlled by the motor controller) and the rotor is the rotating part of the motor (which is where the permanent magnets are housed). Fig 4.2 shows the magnetic fields of the rotor and stator. The rotor magnetic field is created by the permanent magnets inside and therefore is constant and aligned with the position of the rotor. The stator magnetic field is created by the controller, in this case it is showing trapezoidal control. When using a 6 step trapezoidal control algorithm, the torque and speed are not constant.

trapezoidal-torque-problem

Fig 4.2 A motor with 6 step control produces uneven torque and speed

Maximum torque occurs when the two magnetic fields are orthogonal to each other, which is what FOC tries to achieve. This can be seen in Fig 4.3.

foc-magnetic-fields

Fig 4.3 The same motor using FOC which gives maximum torque

It is also important to introduce two other vectors at this stage. 1) The direct vector and 2) the quadrature vector. The direct vector (denoted by d) is the component of the stator magnetic field that is inline with the rotor magnetic field. The quadrature vector (denoted by q) is the component of the stator magnetic field that is orthogonal to the rotor magnetic field. These two vectors can be seen in Fig 4.4. The goal is to maximise the length of the quadrature vector and minimise the length of the direct vector.

direct-quadrature-vectors
direct-quadrature-vectors

Fig 4.4 The direct and quadrature vectors

These figures have been taken from a YouTube series by Matlab with an episode on FOC at: https://www.youtube.com/watch?v=YPD1_rcXBIE

3 phase signals to components

Now obviously the controller doesn't output the direct and quadrature components 😅 The controller works with a 3 phase output. It can be difficult to control these three signals with traditional PID methods however. Therefore, a transform is used to determine the 3 phase outputs for particular values of the direct and quadrature components.

park-and-clarke-transform
park-and-clarke-transform

Fig 4.5 The purpose of the Park and Clarke transforms

Clarke transform

The Clarke transform changes the basis of the three phases ABC to a new basis XYZ. These new bases are used to project the 3 phases to the 2 control vectors (quadrature and direct).

To start, it is important to understand how the ABC bases are represented. The traditional representation is composed of a 2D image with the ABC bases rotated 120 degrees apart. This is really a projection of the ABC bases from a 3D model.

ABC-bases
ABC-bases

Fig 4.6 A 3D representation and the traditional 2D representation of ABC

ABC-bases-animation

Fig 4.7 An animation of the projection from 3D to 2D

ABC-vectors-animation

Fig 4.8 An animation of the 2D projection

Now that the ABC bases are represented, we can transform these bases into a set of bases that contain a vector that is orthogonal to the projection. This collapses the 3D problem to a 2D problem. The Z axis in the new XYZ basis is the common mode portion, which can be discarded. There are two simple transformations that take place. 1) ABC is rotated around the A vector by 45 degrees. 2) The new bases are rotated around the new Y axis. This creates the new XYZ bases.

XYZ-clarke-transformation
XYZ-clarke-transformation

Fig 4.9 The steps of the Clarke transform

XYZ-clarke-animation

Fig 4.10 An animation of the XYZ bases and original ABC bases

And this is what the matrix form of the transformation looks like. The two matrix transformations that were described before can be combined into one single matrix. That's the Clarke transform in a nutshell and it is more difficult and important than the Park transform.

the-clarke-transform-matrix
the-clarke-transform-matrix

Fig 4.11 The Clarke transformation matrix

Park transform

Once the Clarke transform is performed, the Park transform can be applied. The Park transform by contrast to the Clarke transform is a piece of cake 🍰 In a sentence, "The Park transform is simply a clockwise rotation around the Z axis". The rotation angle ( θ ) is the estimated angle of the rotor relative to the magnetic field being created.

the-park-trasnformation
the-park-trasnformation

Fig 4.12 The Park transformation

And again, here is the matrix for said transformation. This transformation matrix can be combined with the Clarke transformation in order to create the DQZ transform matrix.

the-park-matrix
the-park-matrix

Fig 4.13 The Park transformation matrix

Basic FOC block diagram
FOC-block-diagram
FOC-block-diagram

Fig 4.14 The FOC block diagram

Now that we have an idea of the transforms and reasoning behind FOC, let's start by looking at the right of the diagram in Fig 4.14, where the 3 phase inverter and motor are arranged. The phase currents from the motor are converted to the 2D bases using the Clarke transformation. Then, the Park transformation is used to rotate the frame of reference to that of the rotor. This rotor angle is estimated by an observer.

Now that the quadrature and direct currents are calculated, they are fed into two PID controllers. The first controller tries to maintain the direct current at 0 because it does not create any torque. The second controller controls the quadrature current using another PID controller to monitor the speed.

The new phase voltages have been estimated and are converted from quadrature and direct voltages to 3 phase voltages using the inverse Clarke and Park transformations. A PWM generator creates a rough estimate of these voltages. The inverter then drives the motor and the cycle repeats.

ENOUGH OF THE THEORY! 📚

For further reading about how to setup FOC on a VESC, look at this link.

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