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| United States Patent | 5612605 |
| Link to this page | http://www.wikipatents.com/5612605.html |
| Inventor(s) | Tao; Jinghan (Shorewood, WI) |
| Abstract | A method and/or apparatus used with a voltage/frequency driver for
controlling a motor that maintains a motor driving magnetizing flux at low
frequencies and maintains a constant desired motor speed despite
relatively high slip at low frequencies. The voltage/frequency driver
controls both magnetizing flux and motor speed without requiring sensing
or calculating hardware in addition to hardware typically included with a
voltage/frequency driver. |
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Title Information  |
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Drawing from US Patent 5612605 |
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Auto boost for voltage/frequency motor controller |
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| Publication Date |
March 18, 1997 |
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| Filing Date |
November 17, 1995 |
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| Parent Case |
CROSS REFERENCE
This application is a continuation-in-part of application Ser. No.
08/532,134, filed on Sep. 22, 1995, now abandoned. |
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Title Information  |
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References  |
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| *references marked with an asterisk below are user-added references |
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U.S. References |
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| | Reference | Relevancy | Comments | Reference | Relevancy | Comments | 5440219 Wilkerson 318/802 Aug,1995 |      Your vote accepted [0 after 0 votes] | | 5355295 Brennen 363/40 Oct,1994 |      Your vote accepted [0 after 0 votes] | | 5349517 Brennen 363/40 Sep,1994 |      Your vote accepted [0 after 0 votes] | | 5325042 Murugan 322/10 Jun,1994 |      Your vote accepted [0 after 0 votes] | | 5319535 Brennen 363/40 Jun,1994 |      Your vote accepted [0 after 0 votes] | | 5272428 Spiegel 318/803 Dec,1993 |      Your vote accepted [0 after 0 votes] | | 5123080 Gillett 388/811 Jun,1992 |      Your vote accepted [0 after 0 votes] | | 5010287 Mukai 318/801 Apr,1991 |      Your vote accepted [0 after 0 votes] | | 4893479 Gillett 62/213 Jan,1990 |      Your vote accepted [0 after 0 votes] | | 4549122 Berkopec 388/806 Oct,1985 |      Your vote accepted [0 after 0 votes] | | 4538100 Tuten 318/808 Aug,1985 |      Your vote accepted [0 after 0 votes] | | 4297625 Newell 318/696 Oct,1981 |      Your vote accepted [0 after 0 votes] | | |
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Foreign References |
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References  |
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| Market Size |
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Estimate the gross annual revenues of the relevant market
sector:
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| Reasonable Royalty |
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What percentage of gross sales should the inventor or assignee be paid?
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Public's "Guesstimation" of Royalty Value
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| Market Size | N/A | [No votes] | | x | Market Share | N/A | [No votes] | | x | Reasonable Royalty | N/A | [No votes] |
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Market Review  |
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Technical Review  |
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Claims  |
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I claim:
1. A method to be used with a motor controller for controlling magnetizing
flux between a motor stator and a rotor, the flux being proportional to a
magnetizing current, the controller providing a stator current signal and
a related stator voltage signal which is indicative of the stator voltage
provided by the controller, the method comprising the steps of:
(a) determining an acceptable magnetizing current range in which the
magnetizing current generates enough magnetizing flux to drive the motor;
(b) deriving a current phase angle;
(c) combining the phase angle and the stator current to produce a
magnetizing current estimate;
(d) comparing the magnetizing current estimate to the acceptable
magnetizing current range; and
(e) where the magnetizing current estimate is outside the acceptable
magnetizing current range, adding a voltage boost to the stator voltage
having a polarity tending to drive the magnetizing current to a level
within the acceptable current range.
2. The method of claim 1 wherein the motor is characterized by a rated
voltage when the motor is driven at a rated frequency with no load and the
step of determining an acceptable magnetizing current range includes the
steps of, while running the motor at the rated frequency and voltage with
no load, monitoring the stator current and setting the acceptable
magnetizing current range between 80 percent and 120 percent of the
monitored stator current.
3. The method of claim 2 wherein the step of setting the range includes
setting the range between 95 percent and 105 percent of the monitored
stator current.
4. The method of claim 1 wherein the step of deriving a current phase angle
includes the steps of comparing a zero crossing of the stator voltage
signal with a following and consecutive zero crossing of the stator
current signal to provide a phase angle period and converting the phase
angle period to degrees.
5. The method of claim 1 wherein the step of combining includes the steps
of multiplying the sine of the phase angle by the stator current signal.
6. The method of claim 1 wherein the motor is characterized by a safe
maximum stator current, and the method further includes the steps of,
prior to adding the voltage boost, determining if the stator current is
greater than a maximum stator current and is therefore an excessive stator
current and, if the stator current is the excessive stator current,
determining if the excessive stator current is caused by a load
fluctuation and is therefore a load generated current and:
if the excessive stator current is not the load generated current,
decreasing the voltage boost and skipping to step b; and
if the excessive stator current is the load generated current, skipping to
step b.
7. The method of claim 6 wherein the motor stator is characterized by a
stator resistance which causes a stator resistive drop and the controller
provides a maximum phase angle signal and a maximum boost level and the
acceptable magnetizing current range is characterized by an acceptable
maximum current level, the step of determining if the excessive stator
current is the load generated current includes the steps of:
determining if the voltage boost is greater than the stator resistive drop
and:
(A) if the voltage boost is greater than the stator resistive drop,
concluding that the excessive stator current is not the load generated
current; and
(B) if the voltage boost is less than the stator resistive drop,
determining if the voltage boost is greater than the maximum boost level,
and:
(i) if the voltage boost is greater than the maximum boost level:
(1) determining if the phase angle is greater than the maximum phase angle
signal and, if the phase angle is less than the maximum phase angle
signal, concluding that the excessive stator current is the load generated
current, if the phase angle is greater than the maximum phase angle
signal, concluding that the excessive stator current is not the load
generated current; and
(ii) if the voltage boost is less than the maximum boost level:
(i) determining if the magnetizing current estimate is greater than the
maximum acceptable current level and, if the magnetizing current estimate
is less than the maximum acceptable current level, concluding that the
excessive stator current is not the load generated current, if the
magnetizing current estimate is greater than the maximum acceptable
current level, skipping to step (B) (i) (1) above.
8. The method of claim 6 wherein the motor is characterized by a rated
current and the safe maximum stator current is 1.5 times the rated
current.
9. The method of claim 7 wherein the maximum voltage boost is 0.25 times
the rated voltage.
10. The method of claim 7 wherein the maximum phase angle signal indicates
a maximum phase angle of 50 degrees.
11. The method of claim 1 wherein the controller provides the stator
voltage at a driver frequency and the method is also used for adjusting
the driver frequency as a function of actual slip to maintain a constant
motor speed despite variations in load, the controller also providing
rated current, rated slip, and rated frequency values, the method further
including the steps of, prior to step f, combining the stator current, the
rated frequency, the rated slip, and the rated current to derive a
frequency modifier value and adding the frequency modifier value to the
driver frequency to compensate for actual slip.
12. The method of claim 11 wherein the stator current, rated frequency,
rated slip, and rated current are combined according to the equation:
##EQU15##
where f.sub.rate is the rated frequency, s.sub.rate is the rated slip,
I.sub.rate is the rated current, and I.sub.s is the stator current.
13. An apparatus to be used with a motor controller for controlling
magnetizing flux between a motor stator and a rotor, the flux being
proportional to magnetizing current, the controller providing a stator
current signal and a related stator voltage signal which is indicative of
the stator voltage provided by the controller, the apparatus comprising:
(a) a range calculator for determining an acceptable magnetizing current
range in which the magnetizing current generates enough magnetizing flux
to drive the motor;
(b) an angle calculator for deriving a current phase angle;
(c) a current calculator for combining the phase angle and the stator
current to produce a magnetizing current estimate;
(d) a current comparator for comparing the magnetizing current estimate to
the acceptable magnetizing current range; and
(e) a voltage boost module for, where the magnetizing current estimate is
outside the acceptable magnetizing current range, adding a voltage boost
to the stator voltage, the polarity of said voltage boost calculated to
drive the magnetizing current to a level within the acceptable current
range.
14. The apparatus of claim 11 wherein the motor is characterized by a rated
voltage when the motor is driven at a rated frequency with no load and the
range calculator includes a current sensor to monitor the stator current
while the controller drives the motor at the rated frequency and rated
voltage with no load, and a range setter that sets the acceptable
magnetizing current range between 80 percent and 120 percent of the
monitored stator current.
15. The apparatus of claim 14 wherein the range setter sets the range
between 95 percent and 105 percent of the monitored stator current.
16. The apparatus of claim 13 wherein the current estimator includes a
multiplier for multiplying the sine of the phase angle by the stator
current signal to produce the magnetizing current estimate.
17. The apparatus of claim 13 wherein the motor is characterized by a safe
maximum stator current, and the apparatus further includes a limit module
that, prior to adding the voltage boost, determines if the stator current
is greater than a maximum stator current and is therefore an excessive
stator current and, if the stator current is an excessive stator current,
determines if the excessive stator current is caused by a load fluctuation
and is therefore a load generated current and, if the excessive stator
current is not the load generated current, directs the voltage boost
module to add a voltage boost having a polarity which will reduce the
stator current and, if the excessive stator current is the load generated
current, returns control to the angle calculator.
18. The apparatus of claim 13 wherein the controller provides the stator
voltage at a driver frequency and the method is also used for adjusting
the driver frequency as a function of actual slip to maintain a constant
motor speed despite variations in load, the controller also providing
rated current, rated slip, and rated frequency values, the apparatus
further including a frequency module that generates a frequency modifier
value by combining the stator current, the rated frequency, the rated
slip, and the rated current and adds the frequency modifier value to the
driver frequency to compensate for actual slip.
19. The apparatus of claim 18 wherein the stator current, rated frequency,
rated slip, and rated current are combined according to the equation:
##EQU16##
where f.sub.rate is the rated frequency, s.sub.rate is the rated slip,
I.sub.rate is the rated current, and I.sub.s is the stator current.
20. A method to be used with a motor controller, the controller providing a
stator voltage to the motor at a driver frequency, the method for
controlling magnetizing flux between a motor stator and a rotor and for
adjusting the frequency of a stator voltage to provide a desired motor
speed despite a motor slip, the controller providing a stator current
signal and a related stator voltage signal which is indicative of the
stator voltage, the magnetizing flux being proportional to magnetizing
current, the controller also providing rated current, rated slip, rated
frequency, and rated voltage values characteristic of the motor, the
method comprising the steps of:
(a) during a calibration period, while running the motor at the rated
frequency and voltage with no load, monitoring the stator current and
setting an acceptable magnetizing current range between 80 percent and 120
percent of the monitored stator current,
(b) after the calibration period, combining the stator current signal, the
rated frequency, the rated slip, and the rated current to provide a
frequency modifier value;
(c) adding the frequency modifier value to the driver frequency;
(d) comparing a zero crossing of the stator voltage signal with a following
and consecutive zero crossing of the stator current signal to provide a
phase angle period;
(e) converting the phase angle period to degrees;
(f) multiplying the sine of the phase angle by the stator current signal to
produce a magnetizing current estimate,
(g) comparing the magnetizing current estimate to the acceptable
magnetizing current range; and
(h) where the magnetizing current estimate is outside the acceptable
magnetizing current range, adding a voltage boost to the stator voltage
having a polarity tending to drive the magnetizing current to a level
within the acceptable current range.
21. The method of claim 20 wherein the step of setting the range includes
setting the range between 95 percent and 105 percent of the monitored
stator current.
22. The method of claim 20 wherein the stator current signal, rated
frequency, rated slip, and rated current are combined according to the
equation:
##EQU17##
where f.sub.rate is the rated frequency, s.sub.rate is the rated slip,
I.sub.rate is the rated current, and I.sub.s is the stator current. |
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Claims  |
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Description  |
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FIELD OF THE INVENTION
The present invention relates to AC motors and more particularly to an
apparatus and method to be used with a voltage/frequency controller to
provide an automatic voltage boost at low frequencies in order to maintain
magnetizing motor flux in a desired range.
DESCRIPTION OF THE ART
Many motor applications require that the motor be driven at various speeds.
Motor speed can be adjusted with an adjustable speed drive (ASD) which is
placed between a voltage source and an associated motor that can excite
the motor at various driver frequencies.
One commonly used type of ASD uses a pulse width modulated (PWM) invertor
and associated PWM controller which can control both the magnitude V.sub.s
and frequency f.sub.s of a stator voltage provided across stator windings
of a motor. The stator voltage V.sub.s provides a stator winding current
I.sub.s that lags the voltage V.sub.s by a phase angle .theta..
Referring to FIG. 2, a simplified equivalent circuit for a single phase of
a three phase motor includes a stator resistance R.sub.s in series with
the parallel combination of a rotor resistance R.sub.r and a magnetizing
inductance L.sub.m. The rotor resistance R.sub.r is equal to real
resistance r.sub.r divided by slip s. Stator current I.sub.s splits
between the magnetizing inductance L.sub.m and the rotor resistance
R.sub.r in a manner dependent on the stator voltage frequency f.sub.s and
a slip s associated with a specific motor load. The magnetizing current
I.sub.mag flowing through the inductor L.sub.m in turn generates a
magnetizing flux .PHI..sub.m between the stator and the rotor which
effects rotation of the rotor as well known in the art.
When a multiphase induction motor is fed by a variable frequency multiphase
supply such as a PWM invertor it is desirable to insure that a magnetizing
flux .PHI..sub.m maintains and keeps, for given operating conditions, a
magnitude within a preferred range. In particular, it is often desirable
to maintain the magnetizing flux level close to its rated value as the
motor operating conditions (i.e. motor speed and the torque) vary. The
rated flux level is the flux level attained when the motor operates at a
rated frequency with rated voltage and zero load. By maintaining a
constant magnetizing flux near the rated value a drive can generate the
highest possible torque per amp of stator current and therefore results in
the best possible utilization of the available current capability of the
drive.
Unfortunately, the magnetizing flux .PHI..sub.m varies considerably at
different voltages and frequencies and as a function of motor load. In
addition, as winding temperature changes the resistive values in FIG. 2
typically change by as much as 20% which can affect the magnitude of
magnetizing current and thus the amount of magnetizing flux.
Referring still to FIG. 2, a reactance X.sub.m associated with the
magnetizing inductance L.sub.m can be expressed as:
X.sub.m =2.pi.f.sub.s L.sub.m ( 1)
where f.sub.s is the frequency of the stator voltage V.sub.s. Equation 1
indicates that the reactance X.sub.m is small at low frequencies. When the
reactance X.sub.m is small, the magnetizing potential E.sub.m across the
inductor L.sub.m is reduced, this reduction being reflected in an
increased potential drop across the stator resistor R.sub.s. Because
magnetizing flux .PHI..sub.m reflects magnetizing potential E.sub.m, as
potential E.sub.m decreases, so does the flux .PHI..sub.m. Less flux
.PHI..sub.m leads to severe under excitation and intolerable loss of
torque capability at low frequencies. In many instances resulting torque
loss at low frequencies makes it near impossible to start a motor.
PWM drivers incorporating vector control circuitry provide one solution to
the low frequency magnetizing flux problem. These circuits derive accurate
magnetizing and torque producing current feedback vectors and adjust
stator voltage V.sub.s and frequency f.sub.s as a function of the feedback
vectors to maintain the magnetizing flux .PHI..sub.m in the desired range.
While vector control drives function well, they require hardware to
monitor many different operating parameters and complex circuitry to
calculate and provide required feedback signals to enable precise vector
control. For this reason, vector control drives are typically expensive
and, for some applications, are prohibitively expensive.
Another less expensive type of drive is a voltage/frequency (V/F) drive.
V/F drives, like the vector control drives, are capable of altering both
stator winding voltage V.sub.s and frequency f.sub.s to adjust magnetizing
flux. However, to minimize costs, these drives typically do not include
additional sensing hardware or circuitry required to provide a magnetizing
current feedback vector for use in controlling the magnetizing flux.
Instead, V/F drives are typically programmed to maintain voltage-frequency
relationships which are known to provide sufficient magnetizing flux for
motor operation at most frequencies. For example, to optimally drive a
motor at a rated frequency f.sub.rate, the magnitude of the stator voltage
should be equal to a rated or name-plate voltage V.sub.rate when the motor
is driven with no load. The rated voltage V.sub.rate is calculated to
provide the rated flux level (i.e. the optimal flux load). Similarly, for
most frequencies, optimal motor operation results when:
##EQU1##
where f.sub.s is a frequency less than f.sub.rate and V.sub.s corresponds
to the frequency f.sub.s. Hence, most V/F drives simply maintain the
relationships expressed in Equation 2. Unfortunately, at low frequencies,
even where the relationships expressed in Equation 2 are maintained, the
magnetizing flux .PHI..sub.m is insufficient to drive a motor.
One technique used with V/F drives to drive a motor at low frequencies is
to provide a stator voltage boost V.sub.b at low frequencies. The boost
V.sub.b increases the stator voltage V.sub.s and hence both the
magnetizing potential E.sub.m and the associated magnetizing flux
.PHI..sub.m. If the increased flux .PHI..sub.m is sufficient the motor
will operate.
Unfortunately, the magnitude of a voltage boost V.sub.b required to
increase the magnetizing flux to an effective range is not readily
apparent. Where the boost magnitude is too small, the boost will be
ineffective and torque will not be able to sustain motor operation. In
this case, the user must increase the boost voltage V.sub.b manually and
try to start the motor again. Where the boost magnitude is too large, the
motor can be overexcited and stator and rotor iron can be heavily
saturated. With saturation, heating problems can develop which can damage
motor components and reduce their useful life. Thus, the boost magnitude
is typically increased only minimally during successive starting attempts
until the proper boost level is attained. This protocol is time consuming
and not very exact.
Moreover, where the proper boost level for a specific load is attained
through iterative boost changes, the fixed boost level will not be
suitable when the motor load is changed. For example, if the magnitude of
the boost is set during a full load condition, at no load, the boost will
likely be much too large for driving purposes. The excessive boost will
cause excessive stator currents and saturate the motor iron. There is no
good way to change the boost manually when the motor is continuously
running and therefore, as load changes, conventional methods are
insufficient.
Other solutions used with a V/F drive include providing additional hardware
and computing capability. However, for many applications, as with vector
control drives, this solution is cost prohibitive.
Another problem with V/F drives is that at low frequencies motor operation
is characterized by an increase in slip. Thus, where a stator voltage
frequency f.sub.s is provided which should drive the motor at a desired
speed RPM.sub.d, because of increased slip at low frequencies, the actual
motor speed RPM.sub.a is less than desired.
Thus, it would be advantageous to have a method and/or apparatus to be used
with a V/F drive that could maintain a magnetizing flux level that drives
a motor at low operating frequencies despite an increased relative
magnitude of the stator resistive drop without requiring additional
sensors or complex calculating circuitry. In addition, it would be
advantageous if the V/F drive could also adjust driving frequency to
precisely match actual motor speed to a desired motor speed using sensors
and calculating hardware already provided in most V/F drives.
SUMMARY OF THE INVENTION
The present invention includes both a method and an apparatus for
automatically providing a voltage boost via a V/F driver to a motor
operating at low frequency in order to maintain magnetizing flux
.PHI..sub.m within an effective motor driving range. The magnetizing flux
.PHI..sub.m is proportional to the magnetizing current I.sub.mag and thus,
by controlling the current I.sub.mag the flux .PHI..sub.m can also be
controlled. The magnetizing current I.sub.mag can be increased by
increasing the stator voltage V.sub.s and decreased by decreasing V.sub.s.
Typical V/F drives are equipped with a stator current sensor for sensing
stator current I.sub.s. Because the V/F drive provides the stator voltage
V.sub.s, the phase angle .theta. between the stator voltage V.sub.s and
current I.sub.s can be determined. As explained in more detail below, the
magnetizing current I.sub.mag is related to the stator current I.sub.s
according to the equation:
I.sub.mag .apprxeq.I.sub.s sin .theta. (3)
A close approximation of the magnetizing current I.sub.mag can be
determined using Equation 3. The approximate magnetizing current I.sub.mag
can be compared to a desired magnetizing current corresponding to the
desired magnetizing flux .PHI..sub.m and the stator voltage V.sub.s can be
altered accordingly to maintain the flux .PHI..sub.m in the desired range.
Thus, one object of the present invention is to provide a simple means by
which a magnetizing current approximation can be determined which can then
be compared to a desired magnetizing current, the result of the comparison
used to adjust actual magnetizing current and hence to maintain
magnetizing flux .PHI..sub.m in a range sufficient to drive the motor.
Another object is to provide magnetizing flux compensation using a V/F
drive at low frequencies using hardware already provided on most V/F
drives. V/F drives already include a stator current sensor and the phase
angle .theta. can easily be calculated by comparing the stator current
I.sub.s and stator voltage V.sub.s, which is known because it is supplied
by the drive. Thus, all the information required in Equation 3 is readily
attainable.
The present invention also provides frequency compensation to alter the
stator voltage frequency as a function of the stator current I.sub.s. At
low frequencies, motor slip is increased and therefore, driving frequency
must be adjusted in order to attain a desired motor speed. An equation has
been derived which relates rated motor parameters and the sensed stator
current to a frequency modifier value which can compensate for speed loss
due to slip.
Thus, another object is to provide frequency compensation at low
frequencies using information readily available to V/F drives and using
hardware already existing in V/F drives. The present method requires only
a single calculation using the sensed stator current value and known rated
motor values.
Other and further aspects of the present invention will become apparent
from the description that follows and by reference to the accompanying
drawings.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a schematic diagram of a motor controller according to the
present invention;
FIG. 2 is a schematic of an equivalent circuit for a single phase of a
three phase motor;
FIG. 3 is a phasor diagram showing the relationship between stator voltage,
stator current, magnetizing current, and other motor parameters;
FIG. 4 is a graph illustrating stator winding voltage and current signals
generated by the PWM invertor of FIG. 1;
FIG. 5 is a flow chart indicating operation of the V/F booster of FIG. 1;
and
FIG. 6 is a block diagram of the V/F booster in FIG. 1.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT
For the purposes of understanding the principles of the present invention,
reference will now be made to the embodiments illustrated in the drawings
and specific language will be used to describe the same. It will
nevertheless be understood that no limitation of the scope of the
invention is thereby intended, such alternations and further modifications
in the illustrated device, and such further applications of the principles
of the invention as illustrated therein being contemplated as would
normally occur to one skilled in the art to which the invention relates.
The present invention will be described in the context of the exemplary PWM
invertor 10 shown in FIG. 1. The invertor 10 is shown connected to a
voltage/frequency V/F driver 11, a DC voltage source 18, and a motor 19. A
V/F booster 20 is connected to and communicates with the V/F driver 11.
Note that while the boost 20 is shown as a separate component, it is
contemplated that the boost 20 could be implemented within the driver 11
and therefore, the boost 20 need not be a separate component. The invertor
consists of six solid state switching devices 12-17 (BJT, GTO, IGBT or
other transistor technology devices may be used) arranged in series pairs,
each switching device 12-17 being coupled with an inverse parallel
connected diode 23-29.
Each series arranged pair of switching devices 12 and 13, 14 and 15, and 16
and 17, make up a separate leg 39, 40 or 41 of the invertor 10 and have a
common node which is electrically connected to a unique motor terminal 30,
31, or 32 (and thus to a unique stator winding 35, 36, or 37). Each
switching device 12-17 is also electrically connected by a firing line
51-56 to the V/F driver 11 and indirectly through the driver to a voltage
boost module 20. A split DC voltage source 18 creates a high voltage rail
48 and a low voltage rail 49 and each leg 39, 40, 41 connects the high
voltage rail 48 to the low voltage rail 49.
To avoid repetitive disclosure, the PWM invertor 10 will be explained by
referring only to leg 39 as all three legs 39, 40, and 41 of the invertor
operate in the same manner.
The V/F driver 11 operates to turn the switching devices 12, 13 of leg 39
ON and OFF in a repetitive sequence that alternately connects the high and
low voltage rails 48, 49 to, and produces a series of high frequency
voltage pulses at, terminal 31. The high frequency voltage pulses average
over a given period to produce a low frequency alternating stator voltage
V.sub.s at terminal 31.
Referring to FIG. 4, an exemplary sequence of high frequency pulses 60 that
an invertor 10 might provide to motor terminal 31 can be observed along
with an exemplary low frequency alternating stator voltage V.sub.s. By
varying the widths of the positive portions 63 of each high frequency
pulse relative to the widths of the negative portions 64 over a series of
pulses 60, a changing average voltage value which alternates sinusoidally
can be generated. The changing average value defines the low frequency
alternating stator voltage V.sub.s that drives the motor 19. The stator
winding voltage V.sub.s produces a stator winding current I.sub.s that
lags the stator voltage V.sub.s by a phase angle .theta..
Referring to FIGS. 2 and 4, when the voltage V.sub.s is supplied across the
stator phase, there is a stator resistive voltage drop across stator
resistor R.sub.s and an inductive potential drop E.sub.m across the
inductor L.sub.m and the rotor resistor R.sub.r in parallel. The inductive
potential magnitude and resulting current I.sub.mag are proportional to
the magnetizing flux .PHI..sub.m which must be maintained within a desired
range in order to drive a motor. At low frequencies, the ratio of stator
resistance drop R.sub.s I.sub.s to magnetizing potential E.sub.m increases
to the point where the magnetizing potential E.sub.m cannot generate
sufficient flux .PHI..sub.m to drive the motor.
In addition, at low frequencies, motor slip increases so that, actual motor
speed is often less than the desired speed. Thus, for a motor to operate
as desired at low frequencies, first, the magnetizing flux .PHI..sub.m
must be adjusted to account for the increased stator resistive drop
R.sub.s I.sub.s. Second, the driving frequency must be altered to
compensate for increased slip.
A. Flux Compensation
Referring to FIG. 2, the current I.sub.s is supplied to the motor phase and
divides between the rotor resistor R.sub.s and magnetizing inductor
L.sub.m. Because the magnetizing flux .PHI..sub.m is proportional to the
magnetizing current I.sub.mag within a certain range, the flux .PHI..sub.m
can be maintained within a desired range if the magnetizing current
I.sub.mag can be maintained within a corresponding desired range. Thus,
first a desired corresponding magnetizing current range must be determined
and then, an approximate magnetizing current value must be derived for
comparison and correction purposes.
The desired current range covers current values that are approximately
equal to an optimal current value. It has been determined that, while an
optimal magnetizing flux and corresponding magnetizing current exist, a
motor will operate if the flux and current are approximately optimal.
Thus, in some cases if the actual magnetizing current is within .+-.20
percent of the optimal magnetizing current, flux will be sufficient and
the motor will operate. In nearly all cases, if the actual current is
within .+-.10 percent of the optimal current, the motor will operate. The
preferred range is within .+-.5% of the optimal magnetizing current.
Each motor has a rated voltage V.sub.rate at which the stator voltage
should be maintained when the motor is driven at a nameplate or rated
frequency f.sub.rate with no load. The rated voltage V.sub.rate is
calculated so that, at the rated frequency f.sub.rate, the rated voltage
V.sub.rate generates an optimal magnetizing flux level.
Referring again to FIG. 2, because the affective rotor resistance R.sub.r
is equal to the real rotor resistance r.sub.r divided by the slip s, and
because the slip s is very small when the motor is driven with no load,
during no load excitation, the affective rotor resistance R.sub.r is
extremely high. High rotor resistance R.sub.r minimizes rotor current
I.sub.r and therefore, during no load excitation, nearly all stator
current I.sub.s flows through inductor L.sub.m so that the magnetizing
current I.sub.mag is nearly equal to the stator current I.sub.s. Thus,
during a calibration period, by measuring the stator current while driving
the motor at the rated frequency f.sub.rate and with the rated voltage
V.sub.rate with no load, an optimal magnetizing current Iomag can be
measured.
After determining the optimal magnetizing current I.sub.omag during the
calibration period, the driver can be programmed with any suitable desired
magnetizing current range near the optimal value. While the current range
could be within .+-.20% of the I.sub.omag, to ensure proper motor
operation, preferably, the range is .+-.5% of the optimal magnetizing
current I.sub.omag. After the driver is programmed with the magnetizing
current range, the driver must be programmed to assess actual magnetizing
current I.sub.mag during loaded motor operation.
FIG. 3 is a phaser diagram which relates to the equivalent circuit shown in
FIG. 2 and depicts the relationship between stator voltage V.sub.s and
current I.sub.s as well as other motor parameters of interest during
loaded motor operation. In FIG. 3 the stator voltage V.sub.s leads the
current I.sub.s by phase angle .theta..
The stator voltage V.sub.s includes both the magnetizing potential E.sub.m
as well as the stator resistive drop I.sub.s R.sub.s. It can be seen that
when the resistive drop I.sub.s R.sub.s increases, the magnetizing
potential E.sub.m must decrease given a specific stator voltage V.sub.s.
The stator current I.sub.s includes both a torque producing component
I.sub.torque and the magnetizing component I.sub.mag which is the
parameter of interest. The stator voltage V.sub.s lags the magnetizing
potential E.sub.m by an angle .zeta. which becomes relatively small at low
frequencies. Because the angle .zeta. decreases at low frequencies, a good
approximation of the magnetizing current I.sub.mag can be determined
according to Equation 3.
The stator voltage V.sub.s is provided by the driver and therefore its
instantaneous value is known. The V/F drive monitors the stator current
I.sub.s. By subtracting the zero crossing time of the stator voltage
V.sub.s from the following consecutive zero crossing time of the stator
current I.sub.s and converting the resulting period to degrees, the phase
angle .theta. can be determined. Then, Equation 3 can be used to find a
good approximation of the magnetizing current I.sub.mag.
The current approximation I.sub.mag can then be compared to the acceptable
magnetizing current range and, where the current approximation I.sub.mag
is not within the acceptable range, the stator voltage V.sub.s can be
adjusted to alter the stator current I.sub.s and thus provide the correct
magnetizing current I.sub.mag.
Clearly, there are some limitations on how much the stator voltage V.sub.s
can be increased or boosted prior to risking motor component damage. The
most important limitation is the level of | | |