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System And Method For Sensorless Control Of Electric Machines Using Magnetic Alignment Signatures

Abstract: A system and method for position sensorless control of an AC electric machine is disclosed. A drive system for driving an AC electric machine provides a primary current excitation to drive the AC electric machine, the primary current excitation comprising a current vector having a magnitude and angle. The drive system injects a carrier signal to the AC electric machine that is superimposed onto the current vector, with the carrier signal being selected to generate a carrier response signal that has sensitivity to magnetic alignment information of the AC electric machine at its operating point. The drive system measures at least one magnetic alignment signature of the AC electric machine from the generated carrier response signal and controls an orientation of the current vector using the measured at least one magnetic alignment signature, so as to achieve a desired magnetic operation of the AC electric machine. FIGS. 5A, 5B

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Patent Information

Application #
Filing Date
10 October 2017
Publication Number
16/2018
Publication Type
INA
Invention Field
ELECTRICAL
Status
Email
ipr@singhassociates.in
Parent Application
Patent Number
Legal Status
Grant Date
2023-11-15
Renewal Date

Applicants

GENERAL ELECTRIC COMPANY
1 River Road Schenectady, NY 12345 USA

Inventors

1. HUH, Kum-Kang
1 Research Circle Niskayuna, NY 12309 US
2. PAN, Di
1 Research Circle Niskayuna, NY 12309 US

Specification

TECHNICAL FIELD
Embodiments of the invention relate generally to electric machines and, more particularly, to a sensorless method for controlling an electric machine via the use of signatures that are produced by the saturation behavior of the electric machine dependent on an alignment of excitation current provided to the stator thereof.
BACKGROUND
The usage of electric machines in various industries has continued to become more prevalent in numerous industrial, commercial, and transportation industries over time. With an electric machine, be it an interior electric machine (IPM) machine, permanent magnet (PM) assisted synchronous reluctance machine, or a synchronous reluctance machine, position determination of the rotor or the magnetic field is a critical informational element for torque control of the machine.
For purposes of determining rotor position in an electric machine, an encoder, tachometer, or resolver may be used as the position sensor. For measuring the magnetic field position in the electric machine, magnetic field sensors such as Hall effect sensors may be used. The sensors/devices utilized for determining the rotor position and magnetic field may be used in combination with one another, with it being recognized that position sensor or rotor position sensors and magnetic field sensors for measuring magnetic field orientation or strength may both be employed for the purpose of electric machine control. It is recognized, however, that the position sensor (e.g., encoder), along with its cabling and interface electronics, contributes to a significant portion of the motor drive system cost and overall complexity and is often a major reliability concern. The cost, complexity, and reliability issues associated with the use of position sensors in determining rotor position has led to the advent of systems and methods of sensorless position sensing and control of electric machines (i.e., not requiring rotor position or speed sensors).

Because of the tremendous potential of cost reduction and reliability improvement, sensorless control has been a major research challenge. Most of the sensorless control methods that are available in industries are so called Back-EMF tracking approaches. Back-EMF tracking methods utilize the voltage of the motor winding induced by the time variation of the flux-linkage caused by the rotation of the rotor. These methods perform very well near the rated speed where the back-EMF voltage is close to rated voltage. However, as the speed is reduced, the back-EMF magnitude is reduced and performance is deteriorated. Eventually, as the speed is close to zero, these methods become unstable and fail, because the back-EMF diminishes and becomes unobservable. This limits back-EMF tracking methods to HVAC type of applications where open-loop starting is acceptable.
Owing to its tremendous potential of cost reduction, reliability improvement, and elimination of interfaces, zero and near zero speed (or frequency) sensorless control has been a major research challenge for decades, and high frequency injection methods have been the most promising solution for the sensorless operation on or near zero frequency for AC electric machines with saliency. High frequency signal injection is used to track the rotor angular position and velocity of various AC electric machines having a rotor providing an impedance that varies with rotor position or flux position, such as described in U.S. Pat. Nos. 5,585,709; 5,565,752; 6,131,258; 6,069,467; 5,886,498; and 6,639,380, for example. In employing a high frequency signal injection technique, small signal saliency and small signal saliency angle is the key information used for sensorless control, with such saliency being defined using small signal impedance.
However, with respect to previously employed encoderless controls that employ high frequency injection, it is recognized such encoderless controls have failed to find success in recovering the full, or near full, torque capability of the machine due to the loss of small signal saliency at high-load levels for the machine, this being due to magnetic saturation at such high-load levels. That is, as the torque level (thus

the current level) is increased, the q-axis starts to saturate and eventually small signal inductance of the q-axis becomes lower than the d-axis inductance, thereby making saliency tracking sensorless control infeasible. Moreover, a cross saturation effect causes the saliency angle to shift away from the d-axis, causing position estimation angle error even though the q-axis small signal inductance is still larger than d-axis. Therefore, existing high frequency injection methods have been limited to applications where torque density requirement is low and also the dynamic performance requirement is modest. Especially, for such applications as traction drives where very high torque density is desired, existing sensorless control methods could achieve only a small fraction of the desired torque requirement, let alone the dynamic performance.
In an effort to address the saliency tracking limitations of the previously described high frequency injection method for zero frequency encoderless control, efforts have been made to incorporate design features into an electric machine (e.g., IPM machines or synchronous reluctance machine) that enable increased torque control without the use of any position sensor. That is, a special rotor structure - i.e., a "D-ring" - that increases magnetic saliency for high frequency excitation has been incorporated into the electric machine, wherein this high frequency excitation can be used for sensorless/encoderless motor control. The rotor structure introduces electrical circuits (shorted circuit, closed circuit with passive or active elements) to a specific orientation of the rotor so that it couples with the stator winding magnetically. The position of the rotor is measured by applying a high frequency carrier voltage to the stator and by indirectly measuring the current of the rotor, by measuring the (reflected) high frequency carrier current response in the stator. If the rotor circuit is aligned in phase with the high frequency injection, the impedance of the motor is reduced. This variation of impedance is used to track rotor position. As a result, small signal saliency up to necessary loading level is introduced and maintained without impact on the electric machine performance, efficiency, and reliability.

While the inclusion of such a special rotor structure or D-ring has enabled increased torque control of an electric machine via the use of high frequency injection sensorless controls, it is recognized that inclusion of such a D-ring in the electric motor may still not provide for full sensorless control of an electric machine, as even with a D-ring it is difficult to maintain a desired level of saliency during operation of the machine due to the severe saturation at very high torque level. .
Therefore, it is desirable to provide a system and method for sensorless control of an electric machine that allows for control over a full operating range of speed and torque. It is further desirable for such a system and method to provide such sensorless control in a manner that overcomes the shortcomings associated with saliency tracking based control methods, such as the effects of magnetic saturation and phase error in position tracking and control of the machine.
BRIEF DESCRIPTION OF THE INVENTION
In accordance with one aspect of the invention, a drive system for driving an AC electric machine is configured to provide a primary current excitation to drive the AC electric machine, the primary current excitation comprising a current vector having a magnitude and angle. The drive system is also configured to inject a carrier signal to the AC electric machine that is superimposed onto the current vector, with the carrier signal being selected to generate a carrier response signal that has sensitivity to magnetic alignment information of the AC electric machine at its operating point. The drive system is further configured to measure at least one magnetic alignment signature of the AC electric machine from the generated carrier response signal and control an orientation of the current vector using the measured at least one magnetic alignment signature, so as to achieve a desired magnetic operation of the AC electric machine.

In accordance with another aspect of the invention, a method for position sensorless control of an AC electric machine includes generating a primary current excitation to drive the AC electric machine, the primary current excitation comprising a current vector having a current magnitude and current angle. The method also includes superimposing a high-frequency carrier voltage or current onto the current vector to generate a selected carrier response current or voltage, respectively, that has sensitivity to magnetic alignment information of the AC electric machine. The method further includes determining one or more magnetic alignment signatures of the AC electric machine from the carrier response current or voltage and controlling the current angle of the current vector driving the AC electric machine based on the one or more magnetic alignment signatures, in order to achieve a desired magnetic operation of the AC electric machine.
In accordance with yet another aspect of the invention, a drive system for use with an AC electric machine not having suitable sensitivity for saliency tracking sensorless control is provided. The drive system is configured to generate a primary excitation current vector to drive the AC electric machine, the primary excitation current vector having a current magnitude and current angle. The drive system is also configured to inject a carrier signal onto the primary excitation current vector, the carrier signal comprising one of a carrier voltage and a carrier current that is superimposed on the primary excitation current vector. The drive system is further configured to measure at least one magnetic alignment signature of the AC electric machine that is derived from a carrier response signal generated from the injected carrier signal and control an orientation of the primary excitation current vector using the measured at least one magnetic alignment signature, so as to achieve a desired magnetic operation of the AC electric machine.
Various other features and advantages will be made apparent from the following detailed description and the drawings.

BRIEF DESCRIPTION OF THE DRAWINGS
The drawings illustrate preferred embodiments presently contemplated for carrying out the invention.
In the drawings:
FIGS. 1A and IB are illustrations of multi-phase AC electric machines with a stationary reference frame and rotor frame defined thereon.
FIG. 2 is an illustration of an operating point current command vector relative to a defined rotor frame and current frame.
FIG. 3 is an illustration of an operating point current command vector relative to a saliency frame.
FIGS. 4A-4C are graphs illustrating small signal magnetic alignment signatures at various current levels for an exemplary IPM motor.
FIG. 5A is a block diagram of a drive system that implements a sensorless control scheme via a high frequency current injection and magnetic alignment signature sensing, according to an embodiment of the invention.
FIG. 5B is a block diagram of the signal injector, signal extractor, magnetic alignment error estimator and position observer in the drive system of FIG. 5A illustrating operations performed by each respective device, according to an embodiment of the invention.
FIG. 6A is a block diagram of a drive system that implements a sensorless control scheme via a high frequency voltage injection and magnetic alignment signature sensing, according to an embodiment of the invention.
FIG. 6B is a block diagram of the signal injector, signal extractor, magnetic alignment error estimator and position observer in the drive system of FIG. 6A

illustrating operations performed by each respective device, according to an embodiment of the invention.
FIG. 7 is a graph illustrating injection of a high frequency signal to a primary excitation current vector on a current reference frame, with the high frequency signal being tangential to the primary current vector, according to an embodiment of the invention.
FIG. 8 is a graph illustrating injection of a pulsating, high frequency current signal on the current reference frame, according to an embodiment of the invention.
FIGS. 9A-9C are graphs illustrating characteristics of the magnetic alignment signatures resulting from d-axis current injections in the current frame, according to an embodiment of the invention.
FIGS. 10A-IOC are graphs illustrating characteristics of the magnetic alignment signatures resulting from d-axis current injections in the current frame, where a D-ring structure is incorporated into the AC electric machine, according to an embodiment of the invention.
FIG. 11 is a graph illustrating injection of a pulsating, high frequency voltage signal on the current reference frame, according to an embodiment of the invention.
FIGS. 12A-12C are graphs illustrating Characteristics of the Current Frame d-axis Voltage Injection Signatures of an IPM machine, according to an embodiment of the invention.
FIG. 13 is a graph illustrating injection of a pulsating, high frequency, phase compensated current signal on a current reference frame, according to an embodiment of the invention.
FIGS. 14A-14C are graphs illustrating Characteristics of the Angle Compensated Current Frame Voltage Injection Signatures of an IPM machine with Carrier

Current aligned on di-axis at MTPA points, according to an embodiment of the invention.
FIGS. 15A-15C are graphs illustrating Characteristics of the Angle Compensated Current Frame Voltage Injection Signatures of an IPM machine with D-ring structure with Carrier Current aligned on di-axis at MTPA points, according to an embodiment of the invention.
FIG. 16A is a block diagram of a magnetic alignment error estimation using a forward mapping technique, implemented by the magnetic alignment error estimator of FIGS. 5B and 6B, according to an embodiment of the invention.
FIG. 16B is a block diagram of a magnetic alignment error estimation using an inverse/reverse mapping technique, implemented by the magnetic alignment error estimator of FIGS. 5B and 6B, according to an embodiment of the invention.
FIG. 17 is a graph illustrating estimation of a magnetic alignment error from the magnetic alignment signature using a forward mapping technique, according to an embodiment of the invention.
FIG. 18 is a block diagram illustrating a blending of multiple magnetic alignment errors, implemented by the magnetic alignment error estimator of FIGS. 5B and 6B, according to an embodiment of the invention.
FIG. 19 is a detailed view of the magnetic alignment error estimator of FIGS. 5B and 6B estimating a magnetic alignment error using multiple magnetic alignment signatures and for a current frame voltage injection, according to an embodiment of the invention.
FIG. 20 is a block diagram of a rotating vector injection performed by the signal injector of FIGS. 5B and 6B, according to an embodiment of the invention.

FIG. 21 is a table setting forth the various injection methods that might be injected and the various magnetic alignment signatures that might be measured, as compared to the prior art injection methods and measured magnetic alignment signatures, according to embodiments of the invention.
FIG. 22 is a block diagram of a vehicle incorporating the drive system of FIG. 5A or 6A to drive a traction motor, according to embodiments of the invention.
DETAILED DESCRIPTION
For purposes of better understanding the descriptions set forth herebelow, the following listing of the nomenclature and abbreviations which will be used is provided.
Reference frame unit vectors for AC machines
qs stationary frame quadrature axis; aligned with a-phase in general
ds stationary frame direct axis;
qr, q rotor synchronous frame quadrature axis
dr, d rotor synchronous frame direct axis
ql current frame quadrature axis
dl current frame quadrature axis
q quadrature axis of the specified reference frame (rotor frame if not
specified)
d quadrature axis of the specified reference frame (rotor frame if not
specified)
Complex vectors for AC machine variables (and vector generalization)

/ bold characters used for complex vectors and complex coefficients
bold characters used for vectors and matrices
fqd =fq~J'fd complex vector representation for ac machine variables
fqd =[fq fd^T ^D vector representation of a complex vector
j complex number operator sj-l
j rotation matrix of 90 degrees (matrix equivalent of j)
Superscripts for reference frame identification
fs complex vector or 2D referred from the stationary reference frame
fr complex vector referred from the rotor reference frame
/ complex vector referred from the rotor reference frame
(reference frame subscript is omitted)
/' complex vector referred from the current reference frame
Symbols for physical quantities
v voltage
/' current
A, flux linkage
e back-EMF voltage
6, a> angular position and angular velocity of a reference frame
6r, a>r electrical rotor angular position and rotor angular velocity
6m , a>m mechanical rotor angular position and rotor angular velocity
Tem electromagnetic torque of a electric machine
TL load torque

Superscripts for variable identifications
differentiated quantity
estimated quantity
scaled quantity
commanded or reference quantity
Electric machine parameters
P number of poles
M number of stator phases
Ls , L stator inductance
r resistance matrix of an asymmetric machine
L inductance matrix of an asymmetric machine
Lq q-axis inductance
Ld d-axis inductance
Lqd ■> Ljq mutual inductances between q and d axis windings
With respect to the subsequent discussion of AC electric machines, reference frames are defined in order to represent the physical quantities of the phase winding domains variables as two-dimensional space vectors. For purposes of better explanation, reference is made to FIGS. 1A and IB - which illustrates cutaway views of AC electric machines 30 and the placements of various reference frames thereon, including the stationary (or stator) reference frame and the rotor reference frame.
Among the multiple-phases of the stator windings 32 of the machine, one phase is used as the reference and is ordered as the 1st stator phase. The stationary reference frame quadrature axis (qs-axis) 34 is defined as the unit vector in which direction the air-gap magnetomotive force (MMF) is maximum when the positive current is applied to the 1st stator phase. The stationary reference frame direct axis (cP-axis)


Where M is the number of stator phases and j is a complex number operator. The same stator variable can be represented as a 2-dimensional vector as:

This stationary reference frame variable can be transformed to rotor reference frame using the following operation:

Inverse transformation to stationary reference frame from the rotor reference frame variable can then be performed according to:

According to embodiments of the invention, a system and method for sensorless control of an electric machine that allows for control over a full operating range of speed and torque are provided. A drive system that drives the electric machine includes a signal injector that operates to inject high frequency carrier signals,

which are then combined/superimposed with a primary excitation vector. Here, primary component of an electric machine variable, such as voltage, current, and flux and etc., is a low frequency component of the variable that is not the high frequency carrier injection signal or the carrier response signal. A rotor position estimator of the drive system monitors a magnetic alignment signature of the electric machine derived from small signal inductances and/or small signal reluctances in order to estimate a magnetic alignment of the electric machine and provide sensorless control thereof. The injection of the high frequency carrier signal may be provided as either rotating vector injection, pulsating vector injection, or a blended rotating and pulsating vector injection, and an optimal magnetic alignment signature may be measured and tracked, such that rotor position estimation and sensorless control of the electric machine may be provided.
As used herein, the term "sensorless," denotes the absence of traditional rotor position or velocity shaft transducers such as encoders, resolvers, or tachometers, while the term "magnetic alignment signature" is understood to refer to a measurable parameter or signature that is derived from saturation behavior or the saliency of the electric machine dependent on a magnetic alignment (i.e., current angle y) of excitation current provided to the stator thereof. That is, for an electric machine with inductance saliency - such as an interior permanent magnet synchronous motor (IPMSM), PM assisted synchronous reluctance machine, synchronous reluctance machine, saliency pole wound field machine, etc. - the high inductance magnetic path of the machine is saturated by excitation current much easier compared to the low inductance path. Therefore, given a high enough excitation current, the magnetic saturation is intensified as the excitation current is aligned closer to the high inductance axis - which, for example, would be the q-axis of an IPM machine and/or the d-axis of a salient pole wound field synchronous machine. This magnetic saturation results in a significant drop in small signal inductance of the high inductance axis, while - to the contrary - as the excitation current is aligned closer to the low inductance axis (e.g., d-axis of an IPM machine),

the magnetic core of the electric machine comes out of saturation. This saturation behavior of an electric machine has strong sensitivity to the alignment of the motor current orientation relative to the rotor position and can be used for estimation of the rotor position of the electric machine, for purposes of sensorless control. “Magnetic alignment” can be defined using current angle, an angle that can be defined as the angle of the current vector either in reference to a rotor features such as rotor pole or rotor magnet orientation, or in reference to the flux orientation of the electric machine such as the stator flux or rotor flux. Typically, the current angle has strong relationship with the output torque produced by the electric machine, such that mapping between torque and the signatures can be established as well. It’s reasonable to use magnetic alignment signatures to characterize the output torque of the electric machine.
The saturation phenomena of the electric machine can be characterized by the inductances at the operating point (I, γ) of the machine, mainly the small signal inductances. An operating point current command vector 44 for the given operating point (I, γ) is illustrated in FIG. 2, with the operating point current command vector Irqd 44 in the rotor reference frame being defined as:

where γ is the current angle and j is a complex number operator.
According to embodiments of the invention, one or more magnetic alignment signatures of the electric machine may be measured in order to determine “magnetic alignment information” of the electric machine. As will be explained in greater detail below, the operating point of the electric machine and the dynamic state of

the machine dictate a preferred high frequency signal injection method and preferred magnetic alignment signature for determining magnetic alignment information of the electric machine, with load conditions, current level, and electric machine type, for example, determining the use of rotating vector injection, pulsating vector injection, or a blended rotating and pulsating vector injection, and measurement of a particular magnetic alignment signature.
One magnetic alignment signature that is measurable responsive to the providing of an operating point current command vector Irqd 44 to the electric machine is a small signal inductance in the rotor reference frame. Given the operating point current command vector Irqd and the corresponding operating point flux Λrqd, the small signal inductances in the rotor reference frame can be defined as:

where Lq is the q-axis inductance, Ld is the d-axis inductance, Lqd and Ldq are cross inductance values, δiqd is the small signal current variation vector from the operating point Irqd, and δλqd is small signal flux variation vector from the operating point flux Λrqd.
The inverse function of this small signal inductance can be also measured. These signatures can be referred to as inverse inductance or as reluctance R, and can be defined as:


Rotor frame signatures can be measured only if the rotor angle is known. Practically, without the knowledge of orientation of the rotor frame, the magnetic alignment signatures are measured in reference to a different frame from the actual rotor frame.
Another magnetic alignment signature that is measurable responsive to the providing of an operating point current command vector Irqd 44 to the electric machine is a small signal inductance in the saliency frame, with illustration of operating point current command vector 44 in the saliency frame being provided in FIG. 3. Using high frequency injection methods, orientation of the magnetic saliency can be measured and magnetic alignment signatures can be represented in reference to the saliency frame. With respect to use of small signal inductance in the saliency frame as a magnetic alignment signature, it is recognized that – for a salient electric machine – the saliency reference frame should ideally be equivalent to the rotor reference frame. However, due to cross saturation and saliency crossover due to saturation of the magnetization path, the saliency frame deviates from the rotor frame. With the minimum inductance axis being defined as the d-axis of the saliency frame (where the inductance is minimized), the small signal inductances in the saliency frame can be defined as:

where Lmax is the maximum inductance and Lmin is the minimum inductance.
The maximum inductance Lmax and the minimum inductance Lmin can be derived as follows:



The inverse of maximum inductance Lmax can be defined as minimum reluctance 9Uin. The inverse of minimum inductance Lmin can be defined as maximum reluctance <*max . The average value of ^ and &min can be defined as average reluctance as 9tz.
To quantitatively assess the saliency, saliency os may be defined as the ratio of the maximum inductance Lmax to the minimum inductance Lmin according to:

A saliency angle error ea can also be derived according to:

Use of rotating vector excitation allows the estimation of the complete Lmax, Lmin, and saliency angular position 6a. Pulsating injection methods that track the d-axis can estimate the saliency angular position 6a and Lmin, but Lmax cannot be estimated. Conversely, pulsating injection methods that track the q-axis can estimate Lmax, but not Lmin .
Based on these limitations of measuring small signal inductance in the saliency frame, another magnetic alignment signature that might be useful is small signal inductances or reluctances in the current reference frame, with illustration of an operating point current command vector in the current frame being provided in FIG.

2. The small signal inductances or reluctances in the current reference frame are measurable responsive to the providing of an operating point current command vector Irqd 44 to the electric machine, with the current angle of the small signal inductances or reluctances being explicitly known through current measurement.
The small signal inductance in the current reference frame can be defined as:

where Liq is the q-axis inductance in the current frame, Lid is the d-axis inductance in the current frame, δiiqd is the perturbed current on the d-axis or q-axis in the current frame as induced by the injected high frequency signal, and Liqd and Lid q are cross inductance values present due to cross saturation in the AC electric machine.
The small signal reluctance in the current reference frame can be defined as:

which can be further divided into individual reluctance values (and defined in terms of inductance) according to:
where R iq is the q-axis reluctance in the current frame, R id is the d-axis reluctance in the current frame, δiiqd is the perturbed current on the d-axis or q-axis in the

current frame as induced by the injected high frequency signal, and &qd and 9Lidq are cross reluctance values present due to cross saturation in the AC electric machine.
The small signal signatures in the rotor, saliency, and current reference frames described above have sensitivity to magnetic alignment, i.e., to the current angle y, with FIGS. 4A-4C illustrating these small signal signatures at various current levels for an exemplary IPM motor. The range of current angle in these plots was limited between 0° and 90°. The range covers the typical motoring operating range. The braking operating range will be between 90° and 180° and the signatures will have a mirror image around the 90° point, except for the cross inductance and cross reluctance terms, which will have inverse mirror image. Typically, the current angle y has strong relationship with torque produced by the electric machine, such that mapping between torque and the signatures can be established as well when torque can be measured or estimated.
As can be seen in FIG. 4A, for no load or very low current operating points, where the desired current vector direction is close to the q-axis, the current frame cross inductance Liqd (as well as the current frame cross reluctance &iqd) has very good sensitivity while the rest of the signals are not very sensitive.
However, as the current level is increased, the operating point current angle y deviates from the q-axis and increases towards 90°. As is shown in FIG. 4B, for a 40% current level, rotor frame q axis inductance Lq and rotor frame q axis reluctance 9k show strong and wide sensitivity range around the operating current angle y. This q-axis variation shows up in the current frame and saliency frame signatures. The current frame d-axis inductance Lid and current frame d-axis reluctance ^ show good sensitivity range around the operating current angle y. Rotating vector injection methods can extract saliency frame inductances Lmin, Lmax, and L, as well as saliency frame reluctances 9Uax, 9Uin, and tffc, which can provide even wider

sensitivity range if combined together. However, saliency tracking based on pulsating vector injection will have limitations, because it can extract only one signature between Lmm and Lmax, or between 9Uax and 9Um, such that sensitivity range is significantly limited around the operating point current angle. This is due to the sharp change of signature sensitivity near current angle near 35°, where saliency crosses over from q-axis to d-axis. It should be noted that saliency tracking sensorless operating fails already at 40% current level, due to close proximity to the saliency crossover at the desired operating point.
As shown in FIG. 4C, as the current level is further increased, the saturation of the q-axis gets deeper, leading to stronger and wider sensitivity of the rotor frame q-axis inductance Lq and rotor frame q axis reluctance 9lq. Sensitivities of the current frame d-axis inductance L'd and the current frame d-axis reluctance 91 'd also strengthen significantly. However, as the rotor frame q-axis inductance Lq drops below Ld, the sensitivity ranges of the current frame d-axis inductance L'q and the current frame d-axis reluctance 91'd start to reduce near the rotor frame q-axis. To the contrary, sensitivities and ranges of the current frame q-axis inductance L'q and the current frame q-axis reluctance 91 'q strengthen significantly. Accordingly, rotating injection would be very effective, since the combination of saliency frame inductances Lmm, Lmax, and Ls as well as saliency frame reluctances 9Uax, 9min, and 9te, also provide very strong sensitivity and range. Alternatively, while minimum inductance Lmm or maximum inductance Lmax tracking pulsating injection both have decent sensitivity, they are not as strong as the previously mentioned signatures.
In summary, as shown in FIG. 4A-4C, the presented magnetic alignment signatures (current frame signatures or saliency frame signatures) combined have strong sensitivity and wide sensitivity range to magnetic alignment over the entire 0-100% current range. This establishes the potential of 100% full torque sensorless operation of the IPM machines using magnetic alignment signatures.

Referring now to FIGS. 5A and 6A, block diagrams of drive systems 60, 62 configured to implement a sensorless control technique for controlling operation of an AC electric machine are provided, according to embodiments of the invention. The drive systems 60, 62 provide AC drive power to an AC electric machine 64 composed of a stator and rotor (not shown) using sensorless rotor tracking of the machine, with such sensorless rotor tracking being achieved by measuring one or more of the small signal magnetic alignment signatures described previously above. The drive systems 60, 62 may be implemented with various types of electric machines that are capable of being driven with AC power to provide such sensorless rotor tracking, such as synchronous motors, including synchronous permanent magnet and synchronous reluctance motors, and induction motors. Additionally, the drive systems 60, 62 may provide such sensorless rotor tracking whether the AC electric machine 64 is used as a motor or a generator.
According to embodiments of the invention, the AC electric machine 64 operated by drive system 60, 62 may be any of an interior permanent magnet (IPM) machine, a permanent magnet (PM) assisted synchronous reluctance machine, a synchronous reluctance machine, and an inductance machine. Thus, while embodiments of the invention are described and illustrated here after specifically with regard to operation of an IPM machine, it is to be understood that such discussion of these embodiments also extends to other electric machine types and constructions, including PM assisted synchronous reluctance machines, synchronous reluctance machines, and inductance machines as mentioned.
In FIGS. 5A and 6A, embodiments of drive systems 60, 62 are shown in which an electric machine power converter 66 and control system 67 are utilized to drive the AC electric machine 64, with high frequency signal injection and parameter signature tracking being used to determine and track a rotor position of the AC electric machine 64. In one embodiment, and as shown in FIGS. 5A and 6A, electric machine power converter 66 is provided as a voltage source drive, although

it is recognized that the electric machine power converter 66 could instead be provided as a current source drive. Voltage source drives 66 for AC machines are well known and may be constructed in various ways, depending on the requirements for driving the electric machine. While control system 67 and the control scheme implemented thereby are shown separately from power converter 66, it is recognized that the control system could be provided either as a controller separate from power converter 66 or as a controller or processor incorporated into power converter 66, according to embodiments of the invention.
As shown in FIGS. 5A and 6A, command signals are provided to the voltage source drive 66 from control system 67, with control system 67 including torque and flux controller 68 and a current controller or regulator 70. System inputs in the control system 67 are torque T* and flux level X* commands received by the torque and flux controller 68. Responsive to the torque T* and flux level X* commands, the torque and flux controller 68 outputs a current reference isq*d to current controller 70, which subsequently outputs commands to voltage source drive 66. Operation of drive system 60, 62 thus results in providing of a primary current excitation (in the form of a current vector having a magnitude and angle) to the AC electric machine 34 to drive the electric machine according to a desired operation.
Also included in the control system 67 is a signal injector 72 that operates to inject high frequency carrier signals to the AC electric machine, with such signals being combined with (i.e., superimposed on) the primary current excitation current vector generated by drive system 60, 62. In the embodiment of FIG. 5A, the signal injector 72 is configured to inject a high frequency current signal onto the current reference isq*d at adder 74 to create a net current signal or command that is provided to current controller 70. In the embodiment of FIG. 6A, the signal injector 72 is configured to inject a high frequency voltage signal onto the output commands from current controller 70 at adder 76 to create a net signal that is provided to voltage source drive 66.

the rotor position information to be able to control an AC electric machine, especially at zero or low frequency operation.
Since a voltage source drive is typically used for electric machine drive systems 60, 62, current control is necessary to achieve the desired current isq*d at the electric machine. If a current source drive is used, current control may not be necessary. In that case, the motor terminal voltage reference vsq*d is not available, making measurement of motor terminal voltage vsqd necessary.
For providing sensorless control for electric machine 64, the drive system 60, 62 targets the enabling of position estimation for zero or low frequency operation, by injecting high frequency carrier voltage vsqdc or current iq*dc to the electric machine 64 and by extracting key magnetic alignment signatures (previously described) that enable the rotor position estimation. Specific injection methods for injecting the high frequency carrier and measuring/analysis of specific magnetic alignment signatures may be employed by the drive system 60, 62 to extract the magnetic alignment signatures, with preferred injection methods and preferred magnetic alignment signatures that are chosen being dependent on the operating point of the electric machine 64 and on the dynamic state of the machine, so as to improve and maximize the performance of the position estimation.
As shown FIGS. 5A and 6A, a motor terminal voltage reference vsqd can be used instead of the measured motor terminal voltage vsqd, assuming the voltage error is sufficiently low or can be compensated sufficiently. However, it is recognized that it may be challenging to accurately estimate and compensate the voltage error caused by switching device non-idealities such as propagation delay, non-linear device voltage drop, and dead-time, as well as the variation of DC bus voltage. Therefore, direct measurement of motor terminal voltage vsqd is often preferred when improvement of voltage accuracy is desired. Similar logic would apply to the


alignment signatures can be extracted from a different orientation other than the current frame d-axis or the current frame q-axis. If the extraction is performed from a different orientation, the magnetic alignment signature will be a composite
signature of both Lqd and L'd. For example, the excitation frame d-axis signature can
have (Lq'dsm9ex+L'dCOs9ex) and the excitation frame q-axis signature can have (Lqd
cos9ex+L'dsm9ex), where 9ex is the angle of the extraction frame relative to the current frame.
Having the current injection carrier selected to be sin#c, inductive voltage is extracted using the multiplication of cos 6C. On the other hand, resistive voltage can also contain magnetic alignment signatures, and a resistive voltage term can be also extracted using a similar extraction method. More specifically, resistive voltage can be extracted by multiplying sin 6C to the carrier response.
Illustration of the operations performed and variables applied by the signal extractor 78 in Equations [17] and [18] are illustrated in the block diagram of FIG. 5B.
Profiles of the selected magnetic alignment signatures that can be extracted with a current frame d-axis current injection (being derived from Equations [17] and [18]) are illustrated in FIGS. 9A-9C for an exemplary IPM machine. For the extracted pulsating voltage vector components Vqlc and Vdc and the current frame inductance values L'd and L'qd that are proportional thereto, it is recognized that Vqc (which is proportional to Llqd ) is very sensitive to current angle near 0% current, as illustrated in FIG. 9A, when the motor is operating at the MTPA operation point (MTPA operating line indicated at 89). However, as the current level approaches the range of 20-30%, sensitivity and range of Vqc drops significantly, such that it is not an ideal magnetic alignment signature to track past this point. Conversely, Vdc, specifically (tecIc)/Vdc, which is the inverse of Lld, has strong sensitivity at a current level of 30% and above, as shown in FIG. 9B, such that (tecIc)/Vdc can be

used as an alternative magnetic alignment signature that may be tracked at current levels of 30% and above with sufficient sensitivity. As another alternative, ((ocIc)/V^dc may also be utilized as the magnetic signature, as shown in FIG. 9C.
By combining both signatures Llqd and Lld, sensorless control can be achieved. However, the signature level of 1/Lld at the MTPA operation point is quite close to the maximum signature level. This may limit the dynamic performance of the sensorless control and thus, in order to improve the dynamic performance as well as the sensitivity of the signatures, the current injection orientation can be rotated towards the q-axis of the current frame (qi-axis) for motoring operation and towards the negative q-axis of the current frame for braking operation, when the current level is high enough and when higher dynamic performance is required. This rotation angle 8comp , as provided/indicated in signal injector 72 of FIG. 5A, may be pre-programmed depending on the operating point and operating requirements of the AC electric machine. The rotating angle can also be increased in response to the magnetic alignment signature itself. That is, if the signature level gets close to its limit, the excitation angle can be increased to extend the sensitivity range. This way, the torque pulsation caused by the injection current can be maintained at a low level during steady state operation.
In addition to or alternative to rotating the current injection orientation to extend the sensitivity range of the magnetic alignment signature and improve the dynamic performance, additional design features might be incorporated in the AC electric machine (e.g., IPM motor) that provide further improved signature signal strength and sensitivity, so as to enable full torque control. According to an embodiment of the invention, a component - termed herein as a special rotor structure or "D ring" - may be incorporated into the AC electric machine, with the special rotor structure introducing magnetic saliency for high frequency excitation, wherein this high frequency excitation can be used for sensorless motor control. The special rotor structure may be in the form of any of the rotor structures shown and described in


Here, the pulsation carrier angle a>ct can be defined as a carrier angle variable 6C and used for both signal injection and for signature extraction as shown in FIG. 6B, and can also be used in the current controller to support the carrier voltage current injection regulation as shown in FIG. 6A. Especially when the voltage injection carrier frequency doesn't have sufficient spectral separation from the current regulation bandwidth, current regulator is desired not to attenuate the injection voltage by creating a cancelling control effort for disturbance rejection. An injection voltage regulator can also be implemented, using the carrier angle 0C.
As illustrated in FIG. 11, in the stationary reference frame, this pulsating vector 90 can be written as

where 6t is the angular position of the current vector in reference to the stator q-axis. Illustration of the operations performed and variables applied by the signal injector 72 in Equations [19] and [20] are illustrated in the block diagram of FIG. 6B.
Upon injection of a pulsating high frequency voltage signal by signal injector 72, a carrier current response can be derived according to:




of the reluctance signature and (a>cIqc)/Vc and (cocIqdc)/Vc is significantly reduced, with it being recognized that torque pulsation can be allowed to increase by increasing the qi-axis current, in order to improve the sensitivity of the signatures.
As previously indicated, inclusion of a D-ring structure in the AC electric machine serves to provide improved signature signal strength and extend the sensitivity range of the magnetic alignment signature, so as to enable full torque sensorless control of the electric machine. FIGS. 15A-15C illustrate magnetic alignment signature strengths and sensitivities for the qi-axis carrier current component I'qc
and reluctance signature (a>cIqc)/Vc and (cocIqdc)/Vc, with it being seen in comparison to FIGS. 14A-14C that the signature sensitivity and sensitivity range can be improved/extended, even though the angle compensation is used to achieve minimum torque pulsation at MTPA points 89.
It can therefore be seen that extraction of a magnetic alignment signature is enabled based on injection of a high frequency carrier signal onto the primary excitation current. As can be seen from Equations [17]-[18] and [21]-[22] above, the signature derived is dependent on the high frequency injection method employed - with it being recognized that, for example, d-axis inductance or reluctance in the current frame, L % 91 % may be measured as the signature. The extracted signature may thus generally be designated as a magnetic alignment signature m.
As seen in each of FIGS. 7B and 8B and now also in FIG. 16A, upon extraction of a desired magnetic alignment signature, the signature value is provided to magnetic alignment error estimator 80 (along with the operating point (I,y)) - with the magnetic alignment signature being indicated as voltage vector components Vqc and Vldc in FIG. 7B (allowing for estimation of the current frame d-axis inductance L'd and the pulsating frame cross inductance L'qd), as current vector components I^c and I%c in FIG. 8B (allowing for estimation of the current frame d-axis reluctance 91 'd and the pulsating frame cross reluctance 9Vqd), and generally as m in FIG. 16A. Via

magnetic alignment error estimator 80, the characteristics of the selected magnetic alignment signature m can be used to estimate a magnetic alignment error s.
The magnetic alignment signature m can be characterized for the range of operating points (I,y) as well as for the selected excitation method described previously. Physical modeling and analysis can be used to produce the characteristics or experimental calibration can be used as well. Even though an operating point lies in a 2-dimensional space of (7, y), typically, desired operation resides on a single line in the space that meets certain requirements, such as maximum torque per ampere (MTPA). Therefore, the mapping doesn't need to cover the entire 2-dimensional space. As shown in FIG. 17, given the operating point (7, y) with current angle y, the desired signature value m* as well as the desired signature error gain Km is produced from the mapping 96 - with FIG. 17 illustrating that the signature error gain Km is the inverse of the slope of the mapping, i.e., slope = \IKm.
The above described approach (in FIG. 16A) utilizes a forward mapping for the signature profile to create an error from the signature error. This approach is effective when the magnetic alignment error s is small, and therefore the linear approximation of the profile is sufficient. However, when the error perturbation is large, inverse mapping can be utilized to generate the estimated magnetic alignment y from the signature value m, such as illustrated in FIG. 16B. In order to properly perform the inverse mapping, sections such as motoring and braking should be determined based on other signals such as commanded current angle, because the inverse mapping can have multiple inverse mapping points depending on the signature characteristics.
It is recognized that, according to embodiments of the invention, multiple magnetic alignment signatures may be used for determining magnetic alignment in the AC electric machine - depending on the operating point(s) of the electric machine, as illustrated in FIG. 18. In using multiple signatures, multiple signatures may be used from a collection of signatures available/measured in a single operating range

and/or different signatures may be used for different operating ranges. As an example, it may be desirable to use a current frame cross reluctance signature Jllqd for zero or low current range operation of the electric machine, while it may be desirable to use d'-axis reluctance Jld or the total reluctance 91 for medium to high torque range operation of the electric machine. In an occurrence of multiple signatures being extracted/used, mi, m.2... WIN, a magnetic alignment error can be determined for each of the multiple signatures, i.e., si, S2...SN, such as illustrated in FIG. 18 - where multiple error estimators are shown as included in magnetic alignment error estimator 80. In utilizing multiple magnetic alignment signatures in a single operating range, blending of the magnetic alignment errors si, S2...SN can be performed via signature selector/error blender 100, with a single error value s output therefrom. In utilizing different magnetic alignment signatures for different operating ranges, instead of a hard jumping between use of such signatures, soft blending can be used in order to reduce the transient response during switching of signatures - such that the use measuring/use of multiple signatures m at one time might occur. In such an embodiment, selection of an appropriate/desired signature may be made by signature selector/error blender 100 to select an error s depending on the operating point (7, y). It should also be noted that it is also possible to have multiple observers, each tracking its own position. The tracked position is then blended with other position estimates of the other observers to obtain the position signal used for reference frame transformation between stationary and synchronous frame. When such an approach is used, an additional algorithm should be employed to prevent a sudden jump in position. As an example, the rated limited linear transition can be used.
Referring now to FIG. 19, operations of the magnetic alignment error estimator 80 are illustrated for a specific implementation thereof where multiple magnetic alignments signatures are used. At zero and very low current level, the qi-axis

carrier current llqc is used. But, for higher current levels, carrier current magnitude Iqdc is used.
As shown in FIGS. 7A, 7B, 8A, 8B, the magnetic alignment error s is output from error estimator 80 and provided to position observer 82, with it being recognized that there are various options of using the estimated magnetic alignment error s for sensorless control. This error can be used to directly drive the current excitation angle 6t forward or backwards for direct magnetic alignment control. One reasonable approach is to use the error to drive an observer regulator in position observer 82 to estimate the rotor angular position Gr. The observer regulator can be implemented as a PI regulator, with a second order integral term of the error being added on top of the PI regulator in improve the ramping tracking capability. The observer regulator can also drive an integrator, with a combination of the observer regulator and the integrator being equivalent to a PLL (Phase Locked Loop). One simple alternative approach is directly using the low pass filtered magnetic alignment error signal, and adding it to the previous current angle y or the rotor angle to determine the next current angle or the rotor position^. This
estimated electrical rotor angular position Gr may be fed back to the torque and flux controller 68, current controller 70 and signal injector 72 to provide sensorless control of the AC electric machine 64.
So far, pulsation signal injection has been described as a sinusoidal waveform injection. However, other waveforms such as square wave can be used as well. Typically, in practice, the injection signal is implemented using pulse width modulation (PWM) of switches (not shown) in the power converter 66. As the injection frequency is increased closer to the PWM frequency, the injection waveform will be composed of fewer number of PWM cycles. To an extreme, injection frequency can be identical to the PWM switching frequency, where the leading half of the PWM cycle and the latter half of the PWM cycle have different


reluctance parameters can be calculated. Also, by extracting the vector components of the negative sequence component from the high frequency current response isqdc, saliency angle 6a can be calculated. The saliency frame inductance (Lmax, Lmin) and reluctance (Rmax, ^min) values can be converted to current frame inductances (Iiq, lld, lldq, lldq) and reluctances (Rq, Jlld, Jlldq, Jlldq) using the saliency angle 6a and the current vector angle 6>(.
In an embodiment where a rotating high frequency AC current isqdc is injected to stator windings of the AC electric machine that is superimposed on top of the primary excitation current, the rotating vector injection current can be defined by:

represented as a vector with magnitude Ic rotating at frequency u>c.
Given the saliency frame inductances Lmax and Lmin, and saliency angle 6a, a voltage response signature can be derived from the injected current isqdc according to:

By extracting the positive sequence component magnitude Vpc and the negative sequence component magnitude Vnc in Equation [32], inductance and reluctance parameters can be calculated. Also, by extracting the vector components of the negative sequence component from the high frequency voltage response v sqdc, saliency angle 6a can be calculated. The saliency frame inductance (Lmax, Lmin) and reluctance (0lmax, 0lmin) values can be converted to current frame inductances

0q, L'd, lidq, Iidq) and reluctances (^, ^, ^ ^) using the saliency angle 8a and the current vector angled,
Thus, as can be seen above, the advantage of rotating vector injection (voltage or current injection) is that it allows the extraction of all four components of the 2D inductance (liq, Ud, Udq, Udq) and 2D reluctance (Xq, JVd, JVdq, JVdq).
An additional embodiment of the invention may perform a high frequency signal injection via an elliptical excitation scheme. It is recognized that, especially for high current high torque operation, high sensitivity and wide sensitivity range of the current frame q-axis signatures are advantageous for sensorless control. However, it is also desired to minimize the excitation level along the q-axis to keep the torque pulsation manageable, such that an elliptical excitation scheme would be desired compared to a rotating vector injection.
For embodiments where a current frame injection scheme is employed, an elliptical excitation scheme can be used in order to manipulate the excitation level of the current frame q-axis, with qi-axis variables being scaled according to:

The resulting scaled inductance matrix can thus be derived as:

By selecting the excitation frame as well as the scale a of the q-axis of the excitation frame, any elliptical excitation can be implemented by applying the rotating vector injection in the domains of scaled variables. Also, the scaled magnetic alignment parameters can be extracted using the same technique as the rotating vector

injection, as described above in Equations [30] and [32]. The non-scaled magnetic alignment parameters can be simply calculated from the scaled parameters.
As set forth in detail above, embodiments of the invention thus provide a system and method for sensorless control of an electrical machine, where specific methods for injecting a high frequency carrier and measuring/analyzing magnetic alignment signatures may be employed, with preferred injection methods and preferred magnetic alignment signatures that are chosen being dependent on the operating point of the AC electric machine and on the dynamic state of the machine, so as to improve and maximize the performance of the position estimation. FIG. 21 presents a table summarizing the injection methods that might be injected and the magnetic alignment signatures that might be measured, according to embodiments of the invention, with the table also indicating the sensitivity of the listed signatures for a typical IPM machine and comparing the measured magnetic alignment signatures (in the current frame and the saliency frame) to saliency angle tracking and polarity detection as performed in the prior art.
Generally, FIG. 21 indicates that the saliency angle which is used in the prior art loses sensitivity to rotor position from medium torque levels and higher. On the other hand, the saliency frame signatures combined together provide fair sensitivity up to high torque level, however the region of the sensitivity for each Lmin and Lmax is quite limited. Therefore, it is necessary to combine both Lmin and Lmax, or extract L^to establish magnetic alignment sensitivity over a desired operating range. The current frame signatures establish fairly good magnetic alignment sensitivity in general. In the current frame signatures, the cross inductance or cross reluctance parameters are ideal magnetic alignment parameters for zero and low current level sensitivity. The current frame d-axis (di-axis) inductance and reluctance can establish good sensitivity from low to medium torque range and fair sensitivity at high torque level, while current frame q-axis (qi-axis) inductance and reluctance have strong sensitivity at high torque level. Accordingly, it is found that

use/measuring of a combination of current frame signatures can establish good magnetic alignment sensitivity over the whole operating range of the electric machine.
As shown in the table of FIG. 21, with a rotating vector inj ection of a high frequency signal (current or voltage) - which may be in the form of a rotating current vector injection, rotating voltage vector injection or elliptical excitation in the current frame - magnetic alignment signatures in the forms of all four inductance parameters (L'qd, L'dq, L'd, L'q) as well as the all four reluctance parameters (9t'qd, 91 'dq, 91 'd, 91 'q) may be extracted, along with the saliency frame parameters such as saliency frame minimum inductance Lmm, maximum inductance Lmax, and saliency angle Qa, and average inductance values L% Between those parameters, strong magnetic alignment sensitivity can be established across the whole operating range of the electric machine, although it is recognized that torque pulsation might be high in the electric machine when injecting signals utilizing rotating vector injection. Elliptical injection provides a good solution to manipulate the torque ripple while maintaining desired magnetic alignment sensitivity.
In one form of injecting a pulsating high frequency current signal, the signal may be injected on the current frame as either a d-axis injection, q-axis injection, switching d-axis/q-axis injection, or a profiled angle injection. For a pulsating current frame d-axis current injection, magnetic alignment signatures may be measured in the form of current frame cross inductance L'qd and a current frame d-axis inductance L'd, with the di-axis current injection resulting in low torque pulsation in the electric machine. Between these two magnetic alignment signatures, good magnetic alignment sensitivity can be established up to medium or fair sensitivity at high torque level. For a pulsating current frame q-axis current injection, magnetic alignment signatures may be measured in the form of current frame cross inductance L'dq and a current frame q-axis inductance L'q, each having good signal strength and sensitivity, with the q-axis injection resulting in a higher

torque pulsation in the electric motor. Both methods can be blended by a switching d-axis/q-axis injection or by profiling the injection angle depending on the current or torque level. For the blended approaches, the signatures are either measured conditionally or are blended with each other.
In one form of injecting a pulsating high frequency voltage signal, the signal may be injected on the current frame as either a d-axis injection, q-axis injection, switching d-axis/q-axis injection, or a profiled angle injection. For a pulsating current frame d-axis voltage injection, magnetic alignment signatures may be measured in the form of current frame cross inductance 9t'qd and a current frame d-axis inductance 91 'd. Between these two magnetic alignment signatures, good magnetic alignment sensitivity can be established up to medium or fair sensitivity at high torque level. For a pulsating current frame q-axis voltage injection, magnetic alignment signatures may be measured in the form of current frame cross inductance 9Udq and a current frame q-axis inductance 9t'q, each having good signal strength and sensitivity, with the q-axis injection resulting in a higher torque pulsation in the electric motor. Both methods can be blended by a switching d-axis/q-axis injection or by profiling the injection angle depending on the current or torque level. For the blended approaches, the signatures are either measured conditionally or are blended with each other. One special example for the profiled injection angle approach would be a minimum torque ripple approach at MTPA points, where the injection angle is profiled in a way that minimizes the torque ripple at the MTPA operating point.
In another form of injecting a pulsating high frequency signal (current or voltage), the signal may be injected as a minimum inductance axis (saliency d-axis) tracking injection or a maximum inductance axis (saliency q-axis) tracking injection. For a minimum inductance axis (saliency d-axis) tracking injection, the saliency frame minimum inductance Lmm and maximum reluctance 9tmax may be measured as the magnetic alignment signature along with the saliency angle Qa, with the a minimum

inductance axis (saliency d-axis) tracking injection resulting in low torque pulsation at low current levels and higher torque pulsation at high current levels. For a maximum inductance axis (saliency q-axis) tracking injection, the saliency frame maximum inductance Lmax and maximum reluctance dUm, may be measured as the magnetic alignment signature along with the saliency angle 6a, with the maximum inductance axis (saliency q-axis) tracking injection resulting in high torque pulsation in the electric motor.
Another method of injecting a pulsating high frequency signal is indicated in FIG. 21 as a "blended injection" - which combines rotating vector injection and pulsating injection. Such a blended injection may be employed to increase a q-axis injection during operation of the electric machine during transient or very high torque conditions, with elliptical injection providing a means to smoothly transition from pulsating injection to a rotating injection. For a blended current injection, the current frame cross inductance L'qd and L'dq as well as the current frame d-axis inductance L'd may always be measured, while current frame q-axis inductance L'q could be conditionally measured. For a blended voltage injection, the current frame cross reluctances dSqd and dSdq as well as the current frame d-axis reluctance 9Sd may always be measured, while the current frame q-axis reluctance 9Sq could be conditionally measured. Additionally, minimum inductance L min. maximum inductance Lmax, and average inductance values Lavg could also be conditionally measured.
Thus, as can be seen in the table of FIG. 21, magnetic alignment signatures measured according to embodiments of the present invention, resulting from a selected method of high frequency signal injection, provide for sensorless control of an electric machine over a full operating range of speed and torque. This is compared to prior art sensorless control techniques that utilize saliency tracking based control methods, which are prone to the effects of magnetic saturation and phase error in position tracking and control of the machine and do not provide

adequate sensorless control at low speed - high torque operation of the electric machine.
According to an embodiment of the invention, the drive system 60, 62 (FIGS. 5A and 6A), as discussed herein, may be used as a drive system for driving a traction or propulsion motor for virtually any vehicle. The magnetic alignment signature of an embodiment of the invention achieves strong sensitivity up to a very high torque level sufficient to enable the sensorless traction drive system for vehicle applications. Suitable vehicles for use include, but are not limited to, an off-highway vehicle (OHV), a locomotive, a mining vehicle, electric-motorized railcar, automobiles, trucks, construction vehicles, agricultural vehicles, airport ground service vehicles, fork-lifts, non-tactical military vehicles, tactical military vehicles, golf carts, motorcycles, mopeds, all-terrain vehicles, vessels, and the like. As an example, FIG. 22 illustrates an electric vehicle 102 having a vehicle propulsion system that incorporates an AC electric machine (EM) 104 that functions as a traction motor, with the traction motor 104 receiving power from one or more energy storage devices 106 and power converters 108 included in the vehicle 102. An output of the traction motor 104 connects to a vehicle traction system 106, to drive a differential 108 connecting a traction system drive shaft 110 to wheels 112. A drive system 114 in vehicle 102 drives traction motor 104 via a sensorless control technique, such as previously described with respect to drive system 60, 62 in FIGS. 5A and 6A, in order to provide propulsion to the vehicle 102.
A technical contribution of the present invention is that it provides a controller implemented technique for position estimation and sensorless control for an AC electric machine. The technique measures magnetic alignment signatures derived from a selected method of high frequency signal injection, with the magnetic alignment signatures being used to control an orientation of a primary excitation current vector provided to the AC electric machine, so as to achieve a desired magnetic operation of the AC electric machine.

Therefore, according to one embodiment of the invention, a drive system for driving an AC electric machine is configured to provide a primary current excitation to drive the AC electric machine, the primary current excitation comprising a current vector having a magnitude and angle. The drive system is also configured to inject a carrier signal to the AC electric machine that is superimposed onto the current vector, with the carrier signal being selected to generate a carrier response signal that has sensitivity to magnetic alignment information of the AC electric machine at its operating point. The drive system is further configured to measure at least one magnetic alignment signature of the AC electric machine from the generated carrier response signal and control an orientation of the current vector using the measured at least one magnetic alignment signature, so as to achieve a desired magnetic operation of the AC electric machine.
According to another embodiment of the invention, a method for position sensorless control of an AC electric machine includes generating a primary current excitation to drive the AC electric machine, the primary current excitation comprising a current vector having a current magnitude and current angle. The method also includes superimposing a high-frequency carrier voltage or current onto the current vector to generate a selected carrier response current or voltage, respectively, that has sensitivity to magnetic alignment information of the AC electric machine. The method further includes determining one or more magnetic alignment signatures of the AC electric machine from the carrier response current or voltage and controlling the current angle of the current vector driving the AC electric machine based on the one or more magnetic alignment signatures, in order to achieve a desired magnetic operation of the AC electric machine.
According to yet another embodiment of the invention, a drive system for use with an AC electric machine not having suitable sensitivity for saliency tracking sensorless control is provided. The drive system is configured to generate a primary excitation current vector to drive the AC electric machine, the primary excitation

current vector having a current magnitude and current angle. The drive system is also configured to inject a carrier signal onto the primary excitation current vector, the carrier signal comprising one of a carrier voltage and a carrier current that is superimposed on the primary excitation current vector. The drive system is further configured to measure at least one magnetic alignment signature of the AC electric machine that is derived from a carrier response signal generated from the injected carrier signal and control an orientation of the primary excitation current vector using the measured at least one magnetic alignment signature, so as to achieve a desired magnetic operation of the AC electric machine.
This written description uses examples to disclose the invention, including the best mode, and also to enable any person skilled in the art to practice the invention, including making and using any devices or systems and performing any incorporated methods. The patentable scope of the invention is defined by the claims, and may include other examples that occur to those skilled in the art. Such other examples are intended to be within the scope of the claims if they have structural elements that do not differ from the literal language of the claims, or if they include equivalent structural elements with insubstantial differences from the literal languages of the claims.

WE CLAIM:
1. A drive system for driving an AC electric machine, the drive system
configured to:
provide a primary current excitation to drive the AC electric machine, the primary current excitation comprising a current vector having a magnitude and angle;
inject a carrier signal to the AC electric machine that is superimposed onto the current vector, with the carrier signal being selected to generate a carrier response signal that has sensitivity to magnetic alignment information of the AC electric machine at its operating point;
measure at least one magnetic alignment signature of the AC electric machine from the generated carrier response signal; and
control an orientation of the current vector using the measured at least one magnetic alignment signature, so as to achieve a desired magnetic operation of the AC electric machine.
2. The drive system as claimed in claim 1 wherein, in injecting the carrier signal, the drive system is configured to perform a directional pulsating injection of the carrier signal on a current reference frame, the directional pulsating injection of the carrier signal comprising one of a pulsating current injection and a pulsating voltage injection.
3. The drive system as claimed in claim 2 wherein, in injecting the carrier signal, the drive system is configured to perform one or more of:
a current frame d-axis injection where the carrier signal is aligned tangentially to the current vector;
a current frame q-axis injection where the carrier signal is aligned with the current vector;
a current frame injection with a variable injection angle; and

an alternating current frame d-axis and q-axis injection.
4. The drive system as claimed in claim 3 wherein, for the directional
pulsating injection, the at least one magnetic alignment signature comprises:
at least one of a current frame d-axis inductance, a current frame cross inductance, and a composite of the current frame d-axis inductance and the current frame cross inductance, when the signal injector performs a current frame d-axis pulsating current injection;
at least one of a current frame q-axis inductance, a current frame cross inductance, and a composite of the current frame d-axis inductance and the current frame cross inductance when the signal injector performs a current frame q-axis pulsating current injection;
at least one of a pulsation axis inductance, a pulsation axis cross inductance, and a composite of the pulsation axis inductance and the pulsation axis cross inductance, when the signal injector performs a current frame current injection with a variable injection angle; and
at least one of a current frame cross inductance, a conditionally measured or blended measured current frame d-axis inductance and current frame q-axis inductance, and a composite of the current frame cross inductance and the conditionally measured or blended measured current frame d-axis inductance and current frame q-axis inductance, when the signal injector performs an alternating current frame d-axis and q-axis current injection.
5. The drive system as claimed in claim 3 wherein, for the directional
pulsating injection, the at least one magnetic alignment signature comprises:
at least one of a current frame d-axis reluctance, a current frame cross reluctance, and a composite of the current frame d-axis reluctance and the current frame cross reluctance, when the signal injector performs a current frame d-axis pulsating voltage injection;

at least one of a current frame q-axis reluctance, a current frame cross reluctance, and a composite of the current frame q-axis reluctance and the current frame cross reluctance, when the signal injector performs a current frame q-axis pulsating voltage injection; and
at least one of a pulsation axis reluctance, a pulsation axis cross reluctance, and a composite of the pulsation axis reluctance and the pulsation axis cross reluctance, when the signal injector performs a current frame voltage injection with a variable injection angle;
at least one of a current frame cross reluctance, a conditionally measured or blended current frame d-axis reluctance and current frame q-axis reluctance, and a composite of the current frame cross reluctance and the conditionally measured or blended current frame d-axis reluctance and current frame q-axis reluctance, when the signal injector performs an alternating current frame d-axis and q-axis voltage injection.
6. The drive system as claimed in claim 2 wherein, in injecting the
carrier signal, the drive system is configured to inject a pulsating high frequency voltage signal or current signal with angle compensation that reduces torque ripple in the AC electric machine; and
wherein, for the injection of the pulsating high frequency voltage signal with angle compensation, the at least one magnetic alignment signature comprises at least one of a pulsation axis reluctance, a pulsation axis cross reluctance, and a composite of the pulsation axis reluctance and the pulsation axis cross reluctance; and
wherein, for the injection of the pulsating high frequency current signal with angle compensation, the at least one magnetic alignment signature comprises at least of a pulsation axis inductance, a pulsation axis cross inductance, and a composite of the pulsation axis inductance and the pulsation axis cross inductance.

7. The drive system as claimed in claim 2 wherein, in injecting the
carrier signal, the drive system is configured to perform at least one of a profiled
current frame current injection and a profiled current frame voltage injection, so as
to customize a sensitivity of the magnetic alignment signature;
wherein, for the profiled current frame current injection, the at least one magnetic alignment signature comprises at least of a pulsation axis inductance, a pulsation axis cross inductance, and a composite of the pulsation axis inductance and the pulsation axis cross inductance; and
wherein, for the profiled current frame voltage injection, the at least one magnetic alignment signature comprises at least one of a pulsation axis reluctance, a pulsation axis cross reluctance, and a composite of the pulsation axis reluctance and the pulsation axis cross reluctance.
8. The drive system as claimed in claim 1 wherein, the drive system is
configured to perform a saliency tracking injection comprising at least one of a
minimum inductance axis tracking injection and a maximum inductance axis
tracking injection, the minimum inductance axis tracking injection being a saliency
frame d-axis tracking injection and the maximum inductance axis tracking injection
being a saliency frame q-axis tracking injection; and
wherein, for the saliency tracking injection, the at least one magnetic alignment signature comprises one or more of a maximum inductance Lmax and a minimum inductance L mm.
9. The drive system as claimed in claim 1 wherein, in injecting the
carrier signal, the drive system is configured to perform a rotating vector injection
comprising at least one of a rotating vector current injection, a rotating vector
voltage injection, and a, elliptical excitation in a current reference frame, the
elliptical excitation being one of an elliptical injection with a fixed orientation or
an elliptical injection with a rotating orientation that is varied based on the operating

point of the AC electric machine and a desired sensitivity and torque ripple trade¬off.
10. The drive system as claimed in claim 9 wherein, for the rotating
vector injection, the at least one magnetic alignment signature comprises at least
one of, or a composite of, a maximum inductance Lmax, a minimum inductance Lmm,
a composite signature comprising an average inductance Ls or average reluctance
0b;, a current frame d-axis inductance, a current frame q-axis inductance, a current
frame cross inductance, a current frame d-axis reluctance, a current frame q-axis
reluctance, and a current frame cross reluctance; and
wherein measuring of the maximum inductance Lmax and the minimum inductance Lmm, along with extraction of a saliency angle from the rotating vector injection, provides for conversion of the d-axis inductance and reluctance, q-axis inductance and reluctance, and cross inductance and reluctance to a desired reference frame of the AC electric machine.
11. The drive system as claimed in claim 1 wherein, in injecting the carrier signal, the drive system is configured to perform a blended injection comprising both a directional pulsating injection of the carrier signal on a current reference frame and a rotating vector injection.
12. The drive system as claimed in claim 11 wherein, for the blended injection, the at least one magnetic alignment signature comprises at least one of, or a composite of, a current frame d-axis inductance, a current frame cross inductance, a current frame d-axis reluctance, a current frame d-axis reluctance, a current frame cross reluctance, and one or more of a conditionally measured or blended current frame q-axis inductance, current frame q-axis reluctance, maximum inductance Lmax, minimum inductance Lmm, and average inductance Ls.

13. The drive system as claimed in claim 1 wherein the drive system is
configured to:
convert the carrier response signal to lower frequency signal than the carrier signal, so as to eliminate a carrier modulation frequency;
low pass filter the converted carrier response signal to determine vector components of the carrier response signal; and
extract the at least one magnetic alignment signature from the vector components of the carrier response signal.
14. The drive system as claimed in claim 1 wherein, for each respective
magnetic alignment signature of the at least one magnetic alignment signature, the
drive system is configured to:
perform a forward mapping operation for a plurality of desired operating points for the AC electric machine to determine a desired magnetic alignment signature value and desired signature error gain for the magnetic alignment signature; and
estimate a magnetic alignment error based on the magnetic alignment signature, the desired magnetic alignment signature value, and the desired signature error gain.
15. The drive system as claimed in claim 1 wherein, for each respective
magnetic alignment signature of the at least one magnetic alignment signature, the
drive system is configured to:
perform a reverse mapping operation for the magnetic alignment signature, at a desired operating point for the AC electric machine, to generate an estimated magnetic alignment signal; and
estimate a magnetic alignment error based on the estimated magnetic alignment signal and based on a current angle of the desired operating point for the AC electric machine.

16. The drive system as claimed in claim 1 wherein, when the at least
one magnetic alignment signature comprises multiple magnetic alignment
signatures, the drive system is configured to:
estimate a magnetic alignment error for each of the multiple magnetic alignment signatures; and
perform a soft blending operation when switching from use of a first magnetic alignment signature for controlling the orientation of the current vector to use of a second magnetic alignment signature for controlling the orientation of the current vector the soft blending operation reducing a transient response during switching of magnetic alignment signatures.
17. The drive system as claimed in claim 1 wherein the drive system is configured to determine a preferred injection method for injecting the carrier signal select one or more specific magnetic alignment signatures of the at least one magnetic signature to control the orientation of the current based on one or more of the operating point of the AC electric machine and a dynamic state of the AC electric machine.
18. The drive system as claimed in claim 1 wherein the magnetic alignment information includes at least one of a torque of the AC electric machine, the angle of the current vector in reference to a stator flux, the angle of the current vector in reference to a rotor flux, and the angle of the current vector in reference to a rotor pole axis.
19. The drive system as claimed in claim 1 wherein the AC electric machine comprises one of an interior permanent magnet (IPM) machine, a permanent magnet (PM) assisted synchronous reluctance machine, a synchronous reluctance machine, and an inductance machine.

20. A vehicle comprising the drive system as claimed in claim 1 therein, and wherein the AC electric machine comprises a traction motor driven by the drive system.
21. A method for position sensorless control of an AC electric machine, the method comprising:
generating a primary current excitation to drive the AC electric machine, the primary current excitation comprising a current vector having a current magnitude and current angle;
superimposing a high-frequency carrier voltage or current onto the current vector to generate a selected canier response cunent or voltage, respectively, that has sensitivity to magnetic alignment information of the AC electric machine;
determining one or more magnetic alignment signatures of the AC electric machine from the carrier response cunent or voltage; and
controlling the cunent angle of the current vector driving the AC electric machine based on the one or more magnetic alignment signatures, in order to achieve a desired magnetic operation of the AC electric machine.
22. The method as claimed in claim 21 wherein superimposing the high-frequency carrier voltage or current comprises injecting the high-frequency carrier voltage or cunent on a current reference frame of the AC electric machine, according to one or more of a d-axis injection, a q-axis injection, a variable injection angle, a profiled angle injection, and an alternating d-axis and q-axis injection.
23. The method as claimed in claim 21 wherein superimposing the high-frequency carrier voltage or current comprises performing a rotating vector injection, the rotating vector injection comprising injecting one or more of a rotating voltage vector, a rotating cunent vector, and an elliptical injection in a current

reference frame, the elliptical injection comprising one of an elliptical injection with a fixed orientation and an elliptical injection with a rotating orientation.
24. The method as claimed in claim 21 wherein superimposing the high-frequency carrier voltage or current comprises performing a saliency tracking injection according to one of a minimum inductance axis tracking injection and a maximum inductance axis tracking injection, the minimum inductance axis tracking injection being a saliency frame d-axis tracking injection and the maximum inductance axis tracking injection being a saliency frame q-axis tracking injection.
25. The method as claimed in claim 21 wherein superimposing the high-frequency carrier voltage or current comprises performing a blended injection that includes both a pulsating injection of the high-frequency carrier voltage or current on a current reference frame and a rotating vector injection of the high-frequency carrier voltage or current.
26. The method as claimed in claim 21 wherein the one or more magnetic alignment signatures comprises a signature or signatures other than a saliency angle, with the one or more magnetic alignment signatures comprising at least one of a current frame d-axis inductance, a current frame q-axis inductance, a current frame cross inductance, a current frame d-axis reluctance, a current frame q-axis reluctance, a current frame cross reluctance, a maximum inductance Lmax, a minimum inductance Lmm, an average inductance Ls, and a composite of two d-axis, q-axis, or cross- inductances or reluctances.
27. A drive system for use with an AC electric machine not having suitable sensitivity for saliency tracking sensorless control, the drive system configured to:

generate a primary excitation current vector to drive the AC electric machine, the primary excitation current vector having a current magnitude and current angle;
inject a carrier signal onto the primary excitation current vector, the carrier signal comprising one of a carrier voltage and a carrier current that is superimposed on the primary excitation current vector;
measure at least one magnetic alignment signature of the AC electric machine that is derived from a carrier response signal generated from the injected carrier signal; and
control an orientation of the primary excitation current vector using the measured at least one magnetic alignment signature, so as to achieve a desired magnetic operation of the AC electric machine.
28. The drive system as claimed in claim 27 wherein the carrier response signal has sensitivity to magnetic alignment information of the AC electric machine, the magnetic alignment information including at least one of a current angle of the primary excitation current vector, an angle between the primary excitation current vector and a rotor angle of the AC electric machine, and a torque of the AC electric machine.
29. The drive system as claimed in claim 27 wherein the inj ected carrier signal comprises a pulsating voltage vector or pulsating current vector, with the pulsating voltage vector or pulsating current vector being injected onto one or more of:
a current frame d-axis, a current frame q-axis, a variable angle on the current frame, a profiled angle on the current frame, and/or the current frame d-axis and q-axis in an alternating fashion; and/or
a saliency frame minimum inductance axis and/or a saliency frame maximum inductance axis, with the pulsating voltage vector or pulsating current

vector tracking the minimum inductance axis and/or a saliency frame maximum inductance axis.
30. The drive system as claimed in claim 27 wherein the injected carrier signal comprises a rotating voltage vector, a rotating current vector, and/or an elliptical excitation, the elliptical excitation being an elliptical excitation with a fixed orientation and/or an elliptical excitation with a rotating orientation.

Documents

Application Documents

# Name Date
1 201744035888-IntimationOfGrant15-11-2023.pdf 2023-11-15
1 201744035888-STATEMENT OF UNDERTAKING (FORM 3) [10-10-2017(online)].pdf 2017-10-10
2 201744035888-PatentCertificate15-11-2023.pdf 2023-11-15
2 201744035888-POWER OF AUTHORITY [10-10-2017(online)].pdf 2017-10-10
3 201744035888-FORM 1 [10-10-2017(online)].pdf 2017-10-10
3 201744035888-CLAIMS [10-11-2021(online)].pdf 2021-11-10
4 201744035888-DRAWINGS [10-10-2017(online)].pdf 2017-10-10
4 201744035888-CORRESPONDENCE [10-11-2021(online)].pdf 2021-11-10
5 201744035888-DRAWING [10-11-2021(online)].pdf 2021-11-10
5 201744035888-DECLARATION OF INVENTORSHIP (FORM 5) [10-10-2017(online)].pdf 2017-10-10
6 201744035888-FER_SER_REPLY [10-11-2021(online)].pdf 2021-11-10
6 201744035888-COMPLETE SPECIFICATION [10-10-2017(online)].pdf 2017-10-10
7 abstract 201744035888.jpg 2017-10-11
7 201744035888-OTHERS [10-11-2021(online)].pdf 2021-11-10
8 Correspondence by Agent_General Power Of Attorney_16-10-2017.pdf 2017-10-16
8 201744035888-FORM 3 [09-11-2021(online)].pdf 2021-11-09
9 201744035888-Information under section 8(2) [09-11-2021(online)].pdf 2021-11-09
9 201744035888-Proof of Right (MANDATORY) [13-11-2017(online)].pdf 2017-11-13
10 201744035888-FER.pdf 2021-10-17
10 Correspondence by Applicant_Assignment_17-11-2017.pdf 2017-11-17
11 201744035888-FORM 18 [28-07-2020(online)].pdf 2020-07-28
11 201744035888-FORM 3 [03-04-2018(online)].pdf 2018-04-03
12 201744035888-AMENDED DOCUMENTS [07-10-2019(online)].pdf 2019-10-07
12 201744035888-Certified Copy of Priority Document (MANDATORY) [11-05-2018(online)].pdf 2018-05-11
13 201744035888-FORM 13 [07-10-2019(online)].pdf 2019-10-07
13 Delaration_priority_17-05-2018.pdf 2018-05-17
14 201744035888-RELEVANT DOCUMENTS [07-10-2019(online)].pdf 2019-10-07
14 Correspondence by Agent_priority_17-05-2018.pdf 2018-05-17
15 201744035888-RELEVANT DOCUMENTS [07-10-2019(online)].pdf 2019-10-07
15 Correspondence by Agent_priority_17-05-2018.pdf 2018-05-17
16 201744035888-FORM 13 [07-10-2019(online)].pdf 2019-10-07
16 Delaration_priority_17-05-2018.pdf 2018-05-17
17 201744035888-Certified Copy of Priority Document (MANDATORY) [11-05-2018(online)].pdf 2018-05-11
17 201744035888-AMENDED DOCUMENTS [07-10-2019(online)].pdf 2019-10-07
18 201744035888-FORM 18 [28-07-2020(online)].pdf 2020-07-28
18 201744035888-FORM 3 [03-04-2018(online)].pdf 2018-04-03
19 201744035888-FER.pdf 2021-10-17
19 Correspondence by Applicant_Assignment_17-11-2017.pdf 2017-11-17
20 201744035888-Information under section 8(2) [09-11-2021(online)].pdf 2021-11-09
20 201744035888-Proof of Right (MANDATORY) [13-11-2017(online)].pdf 2017-11-13
21 201744035888-FORM 3 [09-11-2021(online)].pdf 2021-11-09
21 Correspondence by Agent_General Power Of Attorney_16-10-2017.pdf 2017-10-16
22 201744035888-OTHERS [10-11-2021(online)].pdf 2021-11-10
22 abstract 201744035888.jpg 2017-10-11
23 201744035888-COMPLETE SPECIFICATION [10-10-2017(online)].pdf 2017-10-10
23 201744035888-FER_SER_REPLY [10-11-2021(online)].pdf 2021-11-10
24 201744035888-DECLARATION OF INVENTORSHIP (FORM 5) [10-10-2017(online)].pdf 2017-10-10
24 201744035888-DRAWING [10-11-2021(online)].pdf 2021-11-10
25 201744035888-DRAWINGS [10-10-2017(online)].pdf 2017-10-10
25 201744035888-CORRESPONDENCE [10-11-2021(online)].pdf 2021-11-10
26 201744035888-FORM 1 [10-10-2017(online)].pdf 2017-10-10
26 201744035888-CLAIMS [10-11-2021(online)].pdf 2021-11-10
27 201744035888-POWER OF AUTHORITY [10-10-2017(online)].pdf 2017-10-10
27 201744035888-PatentCertificate15-11-2023.pdf 2023-11-15
28 201744035888-IntimationOfGrant15-11-2023.pdf 2023-11-15

Search Strategy

1 2021-01-2115-12-20E_21-01-2021.pdf

ERegister / Renewals

3rd: 25 Jan 2024

From 10/10/2019 - To 10/10/2020

4th: 25 Jan 2024

From 10/10/2020 - To 10/10/2021

5th: 25 Jan 2024

From 10/10/2021 - To 10/10/2022

6th: 25 Jan 2024

From 10/10/2022 - To 10/10/2023

7th: 25 Jan 2024

From 10/10/2023 - To 10/10/2024

8th: 08 Oct 2024

From 10/10/2024 - To 10/10/2025