I Dynamics of Electrical Drives
I Dynamics of Electrical Drives
d m
T TL J m J m
d dJ
dt dt dt
d m
For drives with constant inertia, (dJ/dt) = 0; thus,
T TL J
dt
Where, T = developed motor torque
TL = Load torque referred to motor shaft.
J = polar moment of inertia of motor load system referred to motor shaft
ωm = angular velocity of motor shaft
This equation shows that, torque developed by the motor is Counter
balanced by a load torque TL and a dynamic torque J(dω/dt).
• Torque component J(dω/dt) is called the dynamic torque
because it appears during the transient operation.
• Moment of inertia of a drive may be expressed as;
J m kg m 2
GD 2
2
4g
Where, ρ and D – radius and diameter of gyration, respectively
G – weight, N
g – 9.81 m/c2 acceleration due to gravity
Analysis of the fundamental torque equation shows that;
When T > TL, dω/dt > 0. i.e. the drive undergo acceleration.
When T < TL, dω/dt < 0. i.e. the drive will undergo deceleration.
Deceleration occurs also at negative values of motor torque ( i.e. during
braking operation).
When T = TL, dω/dt = 0, i.e the drive will run at a steady state speed.
Speed –torque conventions and multi-quadrant
operations.
d
T TL J
dt
Selection of the sign to be placed before each of the torque depends on the
operating conditions and on the nature of Load torque.
Power developed by a motor is given by the
product of speed and torque.
1. Modes of operation
An electrical drive operates in three modes.
a) Steady State
b) Acceleration including starting
c) Deceleration including stopping.
d m
T Tl J
dt
• The steady state operation for a given speed is realized by the
adjustment of steady state motor speed torque curve such
that the motor and load torques are equal at this speed.
0
T
Principle speed control
• Acceleration and deceleration modes are transient operations.
Constant speed or single speed drives: - are drives where the driving
motor runs at a nearly fixed speed.
Variable speed drives: - are drives needing step less change in speed and
multispeed drives.
a) Continuous duty
a) Continuous duty: -
• The selection of the motor capacity for such a drive is simple if
we know approximately the constant power input required by
the machine.
• In order to select a motor for a rating equal to the known
power input requirement , one may be sure that this rating is
the maximum permissible with respect to heating because the
manufacturer designs and rates it so as to attain maximum
utilization of the material used at rated output.
• For continuous duty at constant or slightly varying load, a motor
is selected from the relevant catalogue for a capacity
corresponding to the power required.
• Although losses during starting are greater than those under rated
load, they may be neglected because starting under continuous
duty is very infrequent and practically no influence on motor
heating.
b) Fluctuating and intermittent duty
- Equivalent current, torque and power methods
the equivalent current Ieq is: -
P I
Pc I R
2 2 2
R t P I R t ... P I n R tn
t1 t 2 ... t n
2 c eq 1 c eq 2 c
eq
Pc I eq R
P t t ... t
I 2
t
I 2
t ... I 2
ntn R
t1 t 2 ... t n t1 t 2 ... t n
2 c 1 2 n 11 2 2
I t I 2t 2 ... I n t n
I eq
2 2 2
t1 t 2 ... t n
11
I I2
I4
I1 In
I3
0
t
t1 t2 t3 t4 tn
I eq
T
1 2
i dt
T 0
I
Load diagram
of Fluctuating load
0
t
- After Ieq is determined, a motor with next higher current rating
from commercially available rating is selected. Then this rating
is checked for its practical feasibility .
DC motor
- This motor can be allowed to carry larger than the rated current
for a short duration. ( Short time overload capacity of the motor)
- A normally designed DC machine is allowed to carry up to 2
times the rated current.
Let the ratio of maximum allowable current (short time overload
current capacity) to rated current be λ.
I max Where, Imax is the maximum value of current
and Irated is the motor rated current
I rated
If the above condition is not satisfied, the motor rating is calculated from: -
I rated
I max
Induction and Synchronous motors
- In case of induction and synchronous motors, for stable
operation, maximum load torque should be well within the
breakdown torque of the motor.
Tmax
Trated
- The e ui ale t u e t ethod assu es o sta t losses to
remain constant for all operating points. Therefore, this method
should be carefully employed when these losses vary.
- It is also not applicable to motors with frequency (or speed)
dependent parameters of the equivalent circuit;
e.g. in deep bar and double squirrel cage rotor motors where
the rotor winding resistance and reactance vary widely
during starting and braking.
-When torque is directly proportional to current;
e.g. dc separately excited motor,
T t T 2t 2 ... T n t n
Teq
2 2 2
t1 t 2 ... t n
11
- When a motor operates at nearly fixed speed, its power will be
directly proportional to torque. Hence, for nearly constant
speed operation, power rating of the motor can be obtained
directly from;
p 1 t1 p 2t 2 ... p n t n
Peq
2 2 2
t1 t 2 ... t n
Example
A constant speed drive has the following duty cycle.
i) Load rising from 0 to 400 KW ; 5 min
ii) Uniform load of 500 KW; 5 min
iii) Regenerative power of 400 KW returned to the supply; 4 min
iv) Remains idle for ; 2 min
1 400
Pi x dx
5 2
400
5 0 5
KW
3
400
5 5002 5 4002 4
2
Prms 3
367KW
16
Since Pmax = 500 KW is less than two times Prms, motor rating = 367 KW
c) Short time duty
- In short time duty, time of motor operation is considerably less
than the heating time constant and motor is allowed to cool
down to the ambient temperature before it is required to
operate again.
- A motor with continuous duty power rating Pr can be overloaded
by a factor K ( K>1) such that the power rating becomes KPr and the
maximum temperature rise reaches the permissible value (θper).
θper
a
θ vs t curves for short time duty loads
(a) - with power KPr
(b) - with power pr b
0
t
Intermittent periodic duty
- During a period of operation, if the speed changes in wide limits,
leading to changes in heating and cooling conditions, methods of
equivalent current, torque or power described previously can
not be employed.
- Let us consider an intermittent load where the motor is
alternatively subjected a fixed load Pr’ of du atio tr and stand
still condition of ts.
- As the motor is subjected to a periodic load, after the thermal
steady state is reached the temperature rise will fluctuate
between a max. value θmax and a minimum value θmin.
- For this load, the motor rating should be selected such that,
θmax ≤ θper where θper is the max. permissible temperature rise
of the motor.
- At the end of working (running) max. temperature will be;
tr tr
max ss (1 e ) mine
r r ……………….. .
T
P’r P’r tr and ts are thermal time constants
of motor for working and standstill
θ
θmax θ
tr ts t
ss 1 e t r / r t s / s
Combining 5.22 and 5.23, we can get;
max 1 e t / r
…………………….. .
r
For full utilization of the motor, θmax = θper . Further θper will be the motor
ss
temperature rise when it is subjected to its continuous rated power Pr .
max P1r
P1s ……………………….. .
K 1
1 e tr / r t s / s
1 e t r / r
………… .
Example
5.2. A motor has a heating time constant of 60 min and cooling
time constant of 90 min. When run continuously on full load
of 20 KW, the final temperature rise is 40oC.
i) What load the motor can deliver for 10 min if this is followed
by a shut down period long enough for it to cool.
ii) If it is on an intermittent load of 10 min followed by 10 min
shut down, what is the maximum value of load it can supply
during the on load period.
Sol.
Alpha(α) is assumed to be zero, since constant and copper losses
are not available separately.
i) When α = 0, the overloading factor is;
K 2.25
1 1
1 e t r /
1 e 10 / 60
10 10
1 e tr / r t s / s 1 e
60 90
K 1.257
0.2425
1 e t r / r
1 e 10 / 60
0.1535
Permitted load = 1.257x20 = 25.14 KW
Work out
2. Half hour rating of a motor is 100 KW. Heating time constant is
80 min and the maximum efficiency occurs at 70% full load.
Determine the continuous rating of the motor.
E K em
- Basic equations applicable to all dc motors are:-
V E I a Ra motor
T K eI a
K e K e
V Ra
2
T
2. Starting
- Maximum current that a dc motor can safely carry during
starting is limited by the maximum current that can be
commutated with out sparking. Usually it is necessary to limit the
current to a safe value during starting.
3. Braking
- Regenerative braking
- Dynamic braking
- Plugging
4. Transient analysis different types of dc motors
5. Energy losses during transient operations
6. Speed control
- Armature voltage control
- field flux control
- Armature resistance control
Methods of armature voltage controls – Variable armature
voltage for speed control, starting, braking and reversing of
dc motors can be obtained by the following methods.
ton = on-time.
toff = off-time.
T = ton + toff = Chopping period.
α = ton/toff.
Thus the oltage a e o t olled a i g dut le α.
Vo = f x ton x Vs
f = 1/T = chopping frequency.
CONTROL STRATEGIES
• The average value of output voltage Vo can be controlled
through duty cycle by opening and closing the semiconductor
switch periodically.
• The various control strategies for varying duty cycle are the
following:
As we can recall;
• Separately Excited DC motor has
field and armature winding with
separate supply.
Vf Rf if Lf
di f Where Rf and Lf are field resistor and
inductor, respectively
dt
• Instantaneous armature current
Va Ra ia La eg
dia
dt
Where, Ra and La are armature resistance and inductance respectively
eg = Kvωif - back emf (speed voltage)
Kv – constructional constant
d
the load torque plus the friction and inertia, i.e.
Tm J B TL
dt
The STEADY-STATE TORQUE AND SPEED
The motor speed can be easily derived
Va I a Ra
Kv I f
If Ra is a small value (which is usual), or when the motor is lightly
loaded, i.e. Ia is small;
Va That is, if the field current is kept
Constant, the motor speed depends
Kv I f only on the supply voltage
Tm Kt I f I a B TL
The developed torque is;
Pm Tm
The required power is;
Ra ia La E V,
dia 0 ≤ t ≤ ton duty interval
dt
• In this interval, armature current increases from ia1 to ia2.
• At t = ton, Tr is turned off. Motor current freewheels through
diode DF and motor terminal voltage is zero during interval
ton ≤t ≤ T. f ee heeli g i te al . This i te al is des i ed the
equation;
Ra ia La E0
dia
ton ≤ t ≤ T
dt
• Motor current decreases from ia2 to ia1 during this interval.
• Ratio of duty interval ton to chopper period T is called duty ratio
or duty cycle ( ).Thus,
Duty int erval ton
T T
Va Vdt V
t
1 on
T 0
V E
Ia
Then
Ra
V
m 2T
Ra
K K
Regenerative braking
• Transistor Tr in a Chopper for regenerative braking is operated
periodically with a period T and on period of ton.
• The mechanical energy converted into electrical by the motor,
now working as a generator, partly increases the stored magnetic
energy in armature circuit inductance and remainder is
dissipated in armature resistance and transistor.
Va Vdt V
T
1
T ton
E V
Then,
Ia
Ra
T KI a
Since Ia is reversed,
V
2T
Ra
K K
Dynamic braking
Fig.6.6. Circuit for dynamic braking of separately excited motor by chopper control
• Du i g the i te al 0 ≤ t ≤ ton, ia increases from ia1 to ia2. A part of
generated energy is stored in inductance and rest is dissipated in Ra
and Tr.
• During interval ton ≤ t ≤ T, ia decreases from ia2 to ia1. The energy
stored in inductance are dissipated in braking resistance RB, Ra and
diode D. Transistor Tr controls the magnitude of energy dissipated
in RB and therefore, controls its effective value.
• If ia is assumed to be rippleless dc, then energy consumed (EN) by
EN I a RB (T ton )
a chopper operation is;
2
T
2 RB (1 )
P
•Effective value of RB is; RBE
Where, on
t Ia
T
Example
1. A 230 V, 960 rpm and 200 A separately excited dc motor has an
armature resistance of 0.02 ohm. The motor is fed from a
chopper which provides both motoring and braking operations.
The source has a voltage of 230 V. Assuming continuous
condition,
i) Calculate duty ratio of the chopper for motoring operation at
rated torque and 350 rpm.
ii) Calculate duty ratio of the chopper for braking operation at
rated torque and 350 rpm.
iii) If max. duty ratio of the chopper is limited to 0.95 and max.
permissible motor current is twice the rated, calculate max.
permissible motor speed obtainable without field weakening
and power fed to the source.
iv) If motor field is also controlled in (iii), calculate field current as
a fraction of its rated value for a speed of 1200 rpm.
At rated operation; E 230 (200 0.02) 226V
Sol.
i)
E 226 82.4V
350
At 350 rpm;
960
960 962rpm
226.5
Max. permissible motor speed = 226
iv) As in (iii) E = 226.5 V for which at rated field current speed = 960
rpm. Assuming linear magnetic circuit, E will be inversely
proportional to field current. Field current as a ratio of its rated
value = 960/1200 = 0.8
6.3. Induction motor control.
What to control? Speed and Torque of the motor . These
parameters should be controlled to suit the load requirement.
• Availability of semiconductor devices (thyristors, power
transistors, IGBT, GTO, etc) allowed the development of variable
speed IM drives.
Let’s e all pe fo a e pa a ete s of IMs.
'
R1 X1 I '
2
X 2
I1 Io
'
V1 Xm
R
2
Pag
Pag
Fig. 6.8. Simplified equiv. circuit.
• Slip is defined as
; N s 1 S nr
N s nr
S ---------- 6.3.1.
S
ms
OR
4f
Where, ms
m ms (1 S )
p
------------------------------ 6.3.2
1. I '
j X 1 X 2 '
V
R2 '
R1
2 ------------------------------ 6.3.3
s
2. Pg 3I '2 2
R2 ' ----------------------------------- 6.3.4.
s
3. Pcu 3I 2 R2
'2 '
----------------------------------- 6.3.5.
1 s
4. Pm Pg Pcu 3I 2 R2
s
'2 '
--------------------- 6.3.6.
T
m ms
Pm 3 '2 R2 '
5. I2 ------------------------ 6.3.7
s
2 R2 '
3
T
V
m
X 1 X 2 '
s
R2 '
R1
2
----------- 6.3.8
s
2
Speed control of IM
• The following methods are employed for speed control of IM.
i) Pole changing
ii) Stator voltage control
iii) Supply frequency control
iv) Eddy current coupling
v) Rotor resistance control
vi) Slip power recovery
we will focus on the most commonly used ones. (ii, iii, v)
ωms TL
V
V’
0
T
fig. 6.9. Stator voltage control
• If stator copper loss, core loss, and friction windage loss are
ignored, then motor efficiency is;
(1 s )
Pm ------------------- 6.3.9
Pg
• The above equation shows that, the efficiency falls with
decrease in speed. The speed control is essentially obtained by
dissipating a portion of rotor input power in rotor resistance.
Thus, not only the efficiency is low, the power dissipation occurs
in rotor itself, which may overheat the rotor .
• Because of these reasons, this drive is employed in fan and
pump drives of low power ratings and for narrow speed range.
PF cos1
I1
---------------------- 6.3.10
I rms
Sol.