Application basics of operation

Application basics of operation
of three-phase induction motors
Design
Duty Types
Selection
Dimensioning
Motor
Management
TM

Foreword
This technical manual for Three-Phase Induction Motors is the first publica-
tion of a series on the topic of "Motor Management".
With these published fundamentals the user will have a growing reference
work on the performance and operational data required for design and
application. The following topics will be covered:
• Starting and operating motors
• Protection of motors and drives
• Selection and operation of controls
• Communications
Electric motors can be found in almost every production process today.
Getting the most out of your application is becoming more and more
important in order to ensure cost-effective operations. "Motor Management"
from Rockwell Automation will help you
• to optimize the use of your systems
• to reduce maintenance costs
• to increase dependability
We are pleased that our publications may help you find economical and
efficient solutions for your applications.
Copyright © 1996 by Sprecher+Schuh AG Rockwell Automation, Aarau.
All information supplied is accurate to the best of our knowledge and without legal liability.
i

Three-phase Induction
Motors
ii
Table of Contents
1 Three-Phase Induction Motors 1.1
1.1 How they work 1.1
1.1.1 Stator 1.1
1.1.2 Rotor 1.1
1.1.3 Slip 1.3
1.1.4 Losses 1.4
1.2 Torque characteristic 1.6
1.2.1 Basic characteristic 1.6
1.2.2 Design measures 1.8
1.3 Operating characteristics 1.10
2 Duty Types of Electric Motors 2.1
2.1 Primary duty types S1... S9 2.1
2.1.1 S1: Continuous duty 2.2
2.1.2 S2: Temporary duty 2.3
2.1.3 S3: Intermittent periodic duty-type without starting 2.4
2.1.4 S4: Intermittent periodic duty with starting 2.5
2.1.5 S5: Intermittent periodic duty with starting and electrical braking 2.6
2.1.6 S6: Continuous-operation duty type 2.7
2.1.7 S7: Continuous-operation duty with starting and electrical braking 2.8
2.1.8 S8: Continuous-operation periodic duty with
related load/speed changes 2.9
2.1.9 S9: Duty with non-periodic load and speed variations 2.11
2.2 Mean values of power, torque, and current 2.12
2.3 Motor power and duty types 2.14
2.3.1 Power increase compared to S1 2.14
2.3.2 Mechanical limit rating 2.15
2.3.3 Power reduction compared to S1 2.15
3 Characteristic Load Torques 3.1
3.1 Load torques as a function of speed 3.2
3.1.1 Torque remains constant 3.2

iii
Motors
3.1.2 Torque increases proportionally to speed 3.3
3.1.3 Torque increases with the square of speed 3.5
3.1.4 Torque decreases in inverse proportion to speed 3.5
3.2 Load torques as a function of angle 3.6
3.3 Load torques as a function of path 3.6
3.4 Load torques as a function of time 3.6
3.5 Breakaway torque 3.6
4 Choosing and Dimensioning
Electric Motors 4.1
4.1 Motor capacity 4.2
4.1.1 Catalog data and application parameters 4.3
4.1.2 Determining the unit rating 4.4
4.1.3 Catalog data 4.4
4.1.4 Operating conditions 4.4
4.1.5 Procedure for motor dimensioning 4.4
4.2 Dimensioning using load torque 4.7
4.3 Calculation using the acceleration torque
or acceleration time 4.8
4.3.1 Acceleration torque 4.8
4.3.2 Acceleration time 4.8
4.4 Calculation using change-over frequency 4.11
4.5 Choosing with the use of catalog data 4.13
5 Symbols 4.14

1.1
1 Three-Phase Induction Motors
The three-phase induction motor, also called an asynchronous motor, is the most
commonly used type of motor in industrial applications. In particular, the squir-
rel-cage design is the most widely used electric motor in industrial applications.
1.1 Principles of Operation
The electrical section of the three-phase induction motor as shown in Figure
1.2.2 consists of the fixed stator or frame, a three-phase winding supplied from
the three-phase mains and a turning rotor. There is no electrical connection
between the stator and the rotor. The currents in the rotor are induced via the air
gap from the stator side. Stator and rotor are made of highly magnetizable core
sheet providing low eddy current and hysteresis losses.
1.1.1 Stator
The stator winding consists of three individual windings which overlap one
another and are offset by an electrical angle of 120°. When it is connected to the
power supply, the incoming current will first magnetize the stator. This magne-
tizing current generates a rotary field which turns with synchronous speed ns.
For the smallest pole number of 2p = 2 in a 50 Hz circuit the highest synchro-
nous speed is ns = 3000/min-1
. Synchronous speeds in a 50 Hz circuit are shown
in Table 1.2.1:
1.1.2 Rotor
The rotor in induction machines with squirrel-cage rotors consists of a slotted
cylindrical rotor core sheet package with aluminum bars which are joined at the
front by rings to form a closed cage.
The rotor of three-phase induction motors sometimes is also referred to as an
anchor. The reason for this name is the anchor shape of the rotors used in very
early electrical devices. In electrical equipment the anchor's winding would be
induced by the magnetic field, whereas the rotor takes this role in three-phase
induction motors.
Motors
ns = synchronous speed/minute
Synchronous speed ns = 60 f = frequency s-1
(per second)
p = pole pair number (pole number/2)
f
p

Table 1.2.1 Typical synchronous speeds in a 50 Hz circuit
Synchronous speeds are 20% higher in a 60 Hz circuit
Figure 1.2.2 State-of-the-art closed squirrel-cage three-phase motor
The stopped induction motor acts like a transformer shorted on the secondary
side. The stator winding thus corresponds to the primary winding, the rotor
winding (cage winding) to the secondary winding. Because it is shorted, its inter-
nal rotor current is dependent on the induced voltage and its resistance. The
interaction between the magnetic flux and the current conductors in the rotor
generates a torque that corresponds to the rotation of the rotary field. The cage
bars are arranged in an offset pattern to the axis of rotation in order to prevent
torque fluctuations (see Figure 1.3.1). This is called "skew".
At idle the rotor almost reaches the synchronous speed of the rotary field, since
only a small counter-torque (no-load losses) is present. If it were to turn exactly
synchronously, voltage would no longer be induced, current would cease to flow,
and there would no longer be any torque.
Motors
1.2
Pole
Number 2p 2 4 6 8 10 12 16 24 32 48
ns in rpm 3000 1500 1000 750 600 500 375 250 188 125

Motors
1.3
During operation the speed of the rotor drops to the load speed n. The difference
between the synchronous speed and the load speed is called slip s. Based on this
load-dependent slip s, the voltage induced in the rotor winding changes, which in
turn changes the rotor current and also the torque M. As slip s increases, the
rotor current and the torque rise. Because the three-phase induction motor acts
like a transformer, the rotor current is transformed to the stator side (secondary
side) and the stator supply current changes essentially to the same degree. The
electrical output of the stator generated by the power supply is converted via the
air gap into mechanical power in the rotor. The stator current therefore consists
of two components, the magnetization current and the actual load current.
a single offset cage bars
b double transposed cage bars
Figure 1.3.1 Forms of squirrel-cage rotor windings
1.1.3 Slip
The difference between the synchronous speed ns and the speed n in rated opera-
tion is called slip s and is generally expressed in percent. Depending on the size
of the machine, in rated operation it is roughly 10 to 3%. Slip is one of the most
important characteristics of an induction machine.
s = slip
Slip s = ns = synchronous speed
n = rotor speed
ns - n
ns

Figure 1.4.1 The rotor voltage UR is a proportional function of slip s. A rotor
voltage of 10% corresponds to a slip of 10%
The induced rotor voltage UR as shown in Figure 1.4.1 is proportional to the
slip s. In the stopped position, it peaks at n = 1 and s = 1, which also results in
the strongest current flow. This fact is confirmed in real-life applications by the
high starting current (starting current inrush). The torque also peaks during the
stop period at a certain rotor resistance. This behavior can be modified by design
variation. However the rotor resistance is not usually used for this purpose. The
following formula applies to the rotor speed:
1.1.4 Dissipation
Since the rotor speed n is less than the synchronous speed ns of the rotary field
by the amount of slip s, the mechanical rotor power P2 is also less than the elec-
trically transmitted rotating field power PD. The difference PVR is lost in the
rotor as heat. These winding losses are thus directly dependent on the slip s.
Beginning with the first instant of the starting process all the power induced in
the rotor is converted into heat.
The equation shows that the thermal danger is greatest for a stationary rotor at
s = 1, since all the electric power input is converted to heat dissipation in the
motor. Due to the increased starting current of induction motors the heat dissi-
pation is a multiple of the rated motor power. In addition, conventional self-
ventilated motors do not provide adequate cooling when stopped.
Motors
1.4
n = rotor speed
Rotor speed n = ns · (1 - s) ns = synchronous speed
s = slip
Dissipation in the rotor PVR = PD · s = ohmic loss PCuR in W

If we examine all power losses Pv in a motor, as shown in Figure 1.5.1, we find
the following individual losses:
The core loss PFe in the stator is caused by hysteresis and eddy current losses
which are dependent on the voltage and frequency. Therefore during operation
they are roughly constant. In the rotor, the losses are insignificant because of the
low frequency of the rotor current during operation. Ohmic losses occur in the
stator PCuS and in the rotor PCuR. Both are a square function of load. Windage
losses PLu and bearing friction losses PLa are likewise constant due to the essen-
tially constant speed in operation. Stray losses Pzus are caused mainly by eddy
currents in the metal components of the machine.
Legend:
P1 = electric power input
PFe = core loss in the stator
PCuS = ohmic loss in the stator
Pzus = stray loss
PD = rotor field power (air gap power)
PCuR = ohmic loss in the rotor
PLu = windage and ventilation loss
PLa = bearing friction losses
P2 = mechanical power output
Figure 1.5.1 Output and losses in a three-phase induction motor
1.5
Motors
• PFe Core loss in the stator ⇒ roughly constant in operation
• PCuS Ohmic loss in the stator ⇒ square function of current
• PCuR Ohmic loss in the rotor ⇒ square function of current
• PLu Windage loss ⇒ roughly constant in operation
• PLa Bearing friction losses ⇒ roughly constant in operation
• Pzus Stray losses ⇒ roughly constant in operation

1.2 Torque Characteristic
1.2.1 Principal Characteristic
Figure 1.6 shows the typical torque characteristics of induction motors with
squirrel-cage rotors which are identified by the following parameters. The accel-
eration torque is defined as the entire range of the torque characteristic from stop
to full speed.
Mn = rated torque
ML = load torque
MK = pull-out torque
MM = motor torque
nS = synchronous speed
An = nominal working point
MA = breakaway torque
MB = acceleration torque
MS = pull-up torque
nn = rated speed (0.94..0.99 . nS)
n = operating speed
A = working point
n0 = no-load speed (0.98..0.997 . nS)
Figure 1.6.1 Induction motor torque characteristic over speed
MA Locked-rotor torque at stop, also called the breakaway torque. The values
provided by the motor manufacturers should have tolerances from -15% to
+25%.
Mn Rated torque during rated operation at rated power Pn and at rated speed nn.
At no-load the torque is very low and covers internal friction. When the
motor is loaded, its speed drops slightly by the amount of slip s and the
torque increases. A standard motor must be able to deliver the rated torque
in continuous operation without exceeding its temperature limit.
In certain operating modes (S2, S3 and S6) the rated torque may also be
exceeded to a certain degree, if the temperature limit is not exceeded, across
the full operating range.
MK Pull-out torque. This is the maximum torque which the motor can deliver. If
the power is increased above the rated load Pn, slip s continues to increase,
speed n decreases, and the motor delivers a higher torque. This can be
increased up to a maximum value MK (pull-out torque) where the motor
becomes unstable, i.e., its speed suddenly decreases at this slip value (break-
down slip) and the motor speed goes to 0.
Motors
1.6

Motors
According to standards, the pull-out torque must be MK ≥ 1.6 Mn and it
must be possible to overload the motor for at least 15 seconds with this
value at the rated voltage and rated frequency. The catalog data may have up
to -10% tolerance. In most motors the pull-out torque is significantly greater
and usually reaches values of MK = 2...3.5 Mn. Therefore induction motors
are especially well suited for intermittent loads, provided the additional heat
can be dissipated.
MS Pull-up torque, also called the pull-through torque, is the smallest torque
during acceleration. In any case it must be greater than the simultaneously
effective load torque ML since otherwise the motor cannot be accelerated.
Minimum values for the pull-up torque are specified in the standards for
rated voltage operations.
ML Load torque, the counter-torque which represents the load during accelera-
tion.
MM Motor torque, also called the acceleration torque.
MB Acceleration torque as the difference of the motor torque MM minus the
load torque ML
In continuous duty with operating mode S1 and rated load Pn a properly sized
motor rotates with rated speed nn and delivers the rated torque Mn:
Torque M can however also be computed using the electrical data of the motor:
1.7
Mn = rated torque in Nm
Rated torque Mn = 9555 · Pn = rated power in kW
nn = rated speed/minute
U = voltage in V
I = current in A
Rated torque Mn = cosϕ = power factor
η = efficiency
n = speed
√3 · U · I · cosϕ · η · 9.55
n
Pn
nn

During starting, the breakaway torque MA must be greater than the breakaway
torque of the load and during the entire acceleration phase the motor torque MM
must remain above the load torque ML, as shown in Figure 1.6.1..
At the intersection of the two torque lines (operating point A) the motor operates
with constant speed n. In case of overload the working point A rises above the
nominal working point An. This is allowable only for a short time to avoid over-
heating the motor.
Working point A however should not be too low either, i.e., an oversized motor
should not be chosen. Below 50% of the rated load the efficiency η and the
power factor cosϕ fall dramatically and motors no longer run economically. A
larger motor also has a larger starting current IA since starting current is inde-
pendent of the load torque. Only the acceleration time would be shortened by a
larger motor.
1.2.2 Motor Design
The torque characteristics can be largely adapted to the application in three-
phase induction motors. Important properties here are a low starting current IA
and high starting torque MA. The torque characteristic and also the size of the
starting current are determined mainly by the type of rotor cage and the shape of
the rotor slot as shown in Figure 1.8.1
A high breakaway torque MA and a small starting current IA can be achieved by
a relatively high ohmic rotor resistance in the starting torque. Basically a more
or less large "current displacement effect" (skin effect) takes place during start-
ing; this applies to all types of rotor designs. The following designs are distin-
guished:
a single cage rotor for diecast version
b deep slot version
c double cage rotor
Figure 1.8.1 Slot shapes for squirrel-cage rotors
Motors
1.8

• Normal squirrel-cage rotors with single slot and round, rectangular or trape-
zoidal conductors usually made of aluminum with a relatively high starting
torque of 1.guatda.com/cmx.p8...2.5 x Mn and a high starting current of 5...10 x In.
• Current displacement rotors, also called deep-bar rotors. If the cage bars are
made tall and narrow, during power-up current displacement takes effect,
since then the rotor frequency is high. The current flows on the outside or
"skin" of the rotor. This effect causes a reduction of the effective conductor
cross section and therefore an increase of the ohmic resistance. The result is
good starting torque MA and a favorable low starting current IA. During
operation current displacement no longer has any effect, since the rotor fre-
quency is then very low and the motor has normal currents and torques.
• Double squirrel-cage rotors have the bar divided into two individual bars
which are usually electrically isolated from one another. The outside cage is
made with high, the inside cage with low ohmic resistance. This is done by
using an appropriate material (Cu, Al, Ms) and proper dimensioning of the
conductor cross sections. The effect is even more pronounced than in a cur-
rent displacement rotor. During start-up, current flows essentially only in the
outside cage; this reduces the starting current IA and causes a relative
increase of the starting torque MA. During operation the current is then dis-
tributed between the two cages according to their ohmic resistances.
• High-resistance squirrel-cage rotors, also called slip rotors, have a slot shape
as in a normal squirrel-cage rotor, but use brass conductors or high resistance
aluminum alloy instead of Al or Cu conductors. This causes the ohmic resis-
tance to increase. In contrast to the current displacement rotor, it remains
constant over the entire speed range and during operation leads to high slip
with a flexible speed characteristic and without a pronounced pull-out torque.
The starting torque MA is high according to the rotor resistance and the start-
ing current IA is reduced. Since the high ohmic resistance is maintained dur-
ing operation, relatively large losses occur, resulting in uneconomical opera-
tion. Therefore, these rotors are not widely used today, especially since the
desired characteristics can also be achieved with low-loss electronic devices,
such as drives and soft starters.
1.9
Motors

K = normal cage (Al)
TN = deep-bar rotor (Al or Cu)
DK = double cage rotor (Al or Cu or
Al outside and Ms inside)
W = high resistance squirrel-cage rotor MS
M = torque
n = speed
Figure 1.10.1 Fundamental torque characteristic of various types of cages
1.3 Operating characteristics
Operating characteristics are a graphical presentation of the behavior of:
• speed • current
• power factor • power
• efficiency • slip
as a function of load.
Figure 1.10.2 shows the operating characteristics of a typical induction motor.
Figure 1.10.2 Operating characteristics of an induction motor as a function
of load
n = speed nS = synchronous speed
P1 = power input P2 = power output
η = efficiency cosϕ = power factor
I = current input In = rated current
s = slip Pn = rated power
Motors
1.10

Motors
n The speed n decreases only slightly as load increases. Standard squirrel-
cage motors thus have "stiff" speed characteristics.
s Slip s increases roughly proportionally as load increases.
cosϕ The power factor cosϕ depends largely on load and it peaks typically dur-
ing overload. In the partial load range it is relatively unfavorable, since
even under partial loads magnetization is essentially constant.
η Efficiency η exhibits a relatively flat characteristic and is almost constant
above half-load. It generally peaks below the rated power Pn.
I Current I increases proportionally beginning roughly at half-load. Below
half-load it decreases only slowly until it becomes the no-load current IO.
(Constant magnetization)
P The power P1 increases roughly in proportion to load starting from the
no-load power. In the overload range it increases slightly faster since losses
also increase faster.
Since the efficiency η and power factor cosϕ can have a major effect on the
economic efficiency of a motor, knowledge of the partial load values is very
important. Both values determine the economic efficiency during operation. In
the partial load range they both drop. In addition, in low-speed motors the power
factor cosϕ is smaller than in high-speed motors. Therefore closely sized, high-
speed motors are not only less expensive purchase, but they also cost less to
operate.
1.11

2.1
2 Duty Types of Electric Motors
Normally, continuous duty three-phase induction motors are designed for the
rated power. Actuators are an exception. Most motors however are operated with
a duty type which is not continuous. Some motors are turned on only briefly,
others run all day, but are only briefly loaded, and numerous motors must accel-
erate a large flywheel or are run in a switched mode and electrically braked.
In all these different duty types a motor heats up differently than in continuous
duty. To prevent damaging the motor winding and rotor due to overheating, these
special heating processes must be taken into account.
2.1 Primary duty types S1... S9
For design purposes information on the duty type must be as accurate as possi-
ble, since the power yield can diverge greatly from continuous output. The num-
ber of possible duty types is thus theoretically unlimited. For the sake of agree-
ment between manufacturers and operators, nine main duty types S1 through S9
were detailed in IEC 34. Almost all cases which occur in practice can be
assigned to one of these duty types:
Motor manufacturers must assign the load capacity of the motor in one of these
defined duty types and where necessary provide the values for operating time,
load period, or relative duty cycle.
Motors
• S1: Continuous duty
• S2: Temporary duty
• S3: Intermittent periodic duty-type without starting
• S4: Intermittent periodic duty with starting
• S5: Intermittent periodic duty with starting and electrical braking
• S6: Continuous-operation duty type
• S7: Continuous-operation duty with starting and electrical braking
• S8: Continuous-operation periodic duty with related load/speed changes
• S9: Duty with non-periodic load and speed variations

In the descriptions and diagrams for duty types S1 through S9 the following
symbols are used:
The speed n is usually specified in revolutions per minute. Generally the rating
plate gives the rated speed nn at full load, but in catalogs also the synchronous or
rated speed is specified.
Duty types S1 through S9 cover many of the applications which occur in the
field. If the type of load cannot be assigned to any of the defined duty types, the
exact cycle description should be indicated to the manufacturer or a duty type
should be selected which conforms to least as heavy a load as the actual applica-
tion.
2.1.1 S1: Continuous duty
Operation with a constant load state as shown in Figure 2.2.1 with a duration
sufficient to reach thermal equilibrium. The load period tB is much greater than
the thermal time constant T
Figure 2.2.1 Duty type S1: Continuous duty
Motors
2.2
P = power in kW tBr = braking time in s, min
Pv = losses in kW tL = idle time s, min, or h
n = speed/min tr = relative duty cycle (%)
ϑ = temperature in °C tS = cycle duration in seconds
ϑmax = maximum temp. in °C tSt = stop period in s, min, or h
t = time in s, min, or h T = thermal time constant in minutes
tB = load period tA = starting time in s, min
JM = moment of inertia of the motor in kgm2
Jext = moment of inertia of the load referenced to the motor shaft in kgm2
Identification S1: Specification of power in kW, if necessary with
abbreviation S1.

2.1.2 S2: Temporary duty
Operation with a constant load state as shown in Figure 2.3.1 which however
does not last long enough to reach thermal equilibrium, and with a subsequent
interval which lasts until the machine temperature differs by not more than 2 K
from the temperature of the coolant.
It is temporary duty when the load period tB ≤ 3 T (thermal time constant).
Compared to continuous duty the motor can deliver more power during the load
period. Consult the manufacturer for details.
Figure 2.3.1 Duty type S2: Temporary duty
2.3
Motors
Identification S2: by specification of the load period tB and power
P in kW
- Example: S2: 10 min, 11 kW.
- For the operating time tB periods of 10, 30, 60 and 90 min are recommended.

Motors
2.4
2.1.3 S3: Intermittent periodic duty-type without starting
Operation as shown in Figure 2.4.1 which is composed of a sequence of similar
duty cycles with cycle duration tS at constant load and an interval which is gen-
erally so short that thermal equilibrium is not reached and the starting current
does not noticeably affect heating. This is the case when tB ≤ 3 T. The power
during this time should be higher than the continuous output of the motor.
Consult the manufacturer for details.
relative duty cycle
tr = · 100
Figure 2.4.1 Duty type S3: Intermittent periodic duty-type without starting
If no cycle duration is specified, tS = 10 min applies.
Recommended values for the relative duty cycle tr are 15%, 25%, 40%, and 60%.
Relative duty cycle tr = · 100
tB load period in s, min ts = cycle duration in s, min
tr = relative duty cycle in %
Identification: by specification of the load period tB, cycle duration
tS and power P, but also by the relative duty cycle tr in % and by
the cycle duration.
- Example: S3: 15 min / 60 min. 11 kW
- Example: S3: 25%, 60 min. 11 kW
tB
tB + tS
tB
tB + tS

Motors
2.1.4 S4: Intermittent periodic duty with starting
Operation as shown in Figure 2.5.1 which consists of a sequence of identical
duty cycles with cycle duration tS, whereby each cycle encompasses a distinct
starting time tA, time tB with constant load, and interval tSt.
relative duty cycle
tr = · 100
Figure 2.5.1 Duty type S3: Intermittent periodic duty with starting
Here it should be noted whether the motor stops under the effect of the load at
the end of the cycle, or whether it is being stopped by a mechanical brake. If the
motor continues to run after it is shut off so that the windings cool down signifi-
cantly, this should be indicated. If not indicated it is assumed that it will stop
within a very short time.
In this duty type the maximum no-load shifts Z0 are used as a basis from which
the maximum frequency of operation shifts is computed according to the load
torque, possible additional mass and a possible flywheel effect. Compared to
continuous duty S1 a power reduction can be noted.
2.5
Relative duty cycle tr = = · 100
tA = starting time s, min ts = cycle duration in s, min
tr = relative duty cycle in % tB = load period in s, min
tSt = stop period in s, min
Identification: by the relative duty cycle tr in %, number ZL of
starts per hour and power P
- Example: S4: 25%, 500 starts per hour, 11 kW
- plus information on the moment of inertia of the motor and load JM and Jext
during starting.
tA + tB
tS
(tA + tB) · 100
tA + tB + tSt
tA + tB
tA + tB + tSt

2.1.5 S5: Intermittent periodic duty with starting and electrical braking
starting time tA, time tB with constant load and time tB of high-speed electrical
braking. There is no interval.
relative duty cycle
tr = · 100
Figure 2.6.1 Duty type S5: Intermittent periodic duty with starting and electrical
braking.
Compared to continuous duty S1 a power reduction is necessary in this mode.
Motors
2.6
Relative duty cycle tr = = · 100
tA = starting time s, min tSt = stop period in s, min
tB = load period in s, min tr = relative duty cycle in %
ts = cycle duration in s, min tBr = braking time in s, min
Identification: similar to S4, but also identified with specification of
the type of braking (plug braking, regenerative braking, etc.)
- In case of doubt and when the starting and braking times are long relative to
the rated operating time, all three time intervals should be indicated
separately.
- Example: S4: 25%, 500 starts per hour, plug braking, 11 kW
- Additional information on the moment of inertia of the motor and load
JM and Jext during starting and braking.
tA + tB + tBr
tS
(tA + tB+ tBr) · 100
tA + tB+ tBr + tSt
tA + tB+ tBr
tA + tB + tBr + tSt

2.1.6 S6: Continuous-operation periodic duty
duty cycles with cycle duration tS, whereby each cycle encompasses a time tB
with constant load and an idle time tL, with no interval. After operating time tB
the motor continues to turn at no-load and due to the no-load current does not
cool down to the coolant temperature, but is ventilated during the idle time tL.
This is the operating state when tB ≤ T.
relative duty cycle
tr = · 100
Figure 2.7.1 Duty type S6: Continuous-operation intermittent duty
Compared to continuous duty S1, the power may be selected to be greater
during operating time tB. Consult the manufacturer for details.
2.7
Motors
Relative duty cycle tr = · 100 = · 100
tB = load period in s, min tL = idle time in s, min
ts = cycle duration in s, min tr = relative duty cycle in %
Identification: as in S3, by the duty cycle tB, cycle duration tS, and
power P
- Example: S6: 25%, 40 min, 11 kW
- If no indication is given for the cycle duration, tS = 10 min applies.
tB
tS
tB
tB+ tL
tB
tB + tL

2.1.7 S7: Continuous-operation duty with starting and electrical
braking
starting time tA, time tB with constant load P and time tBr with high-speed
electrical braking. There is no interval.
relative duty cycle tr = 1
Figure 2.8.1 S7: Continuous operation-duty with starting and electrical braking
Compared to continuous duty S1 a power reduction is necessary in this mode.
Motors
2.8
Relative duty cycle tr = 1
Identification: like S4, identified without indication of relative
duty cycle tr, but with indication of the type of braking (plugging,
regenerative braking, etc).
- In case of doubt and when the starting and braking times are long enough
in relation to the rated operating time, all three time intervals should be
indicated separately.
- Example: S7: 500 duty cycles per hour, braking by plugging, 11 kW.
- Additional information on the moment of inertia of the motor and load JM
and Jext during starting and braking.

2.1.8 S8: Continuous-operation periodic duty with related
load/speed changes
Operation as shown in Figure 2.10.1 which is composed of a sequence of simi-
lar duty cycles with cycle duration tS; each of these cycles comprises a time with
a constant load and a certain speed; then one or more times with different loads
which correspond to different speeds, for example, by pole reversal. There is no
interval or idle time.
This mode cannot be recorded with one simple formula. A suitable continuous
load must be used as the reference dimension for the load cycle:
2.9
Motors
Relative
duty cycle tr1 = = ·100
Relative
Relative
tA = starting time s, min ts = cycle duration in s, min
tB = load period in s, min tr = relative duty cycle in %
tBr = braking time in s, min
Identification: like S5, except that for each speed the time must
be specified during which these speeds occur within every cycle
period.
- Example: S8: 30%, 3000/m, 10 min, 1500/m 20 min. 2 cycles per hour.
11 kW
- Additional information on the moment of inertia of the motor and load JM
and Jext during starting and braking.
tA + tB1
tS
(tA + tB1) · 100
tA + tB1 + tBr1 + tB2 + tBr2 + tB3
(tBr1 + tB2) · 100
(tBr2 + tB3) · 100
tBr1 + tB2
tS
tBr2 + tB3
tS

Figure 2.10.1 Duty type S8: Continuous-operation periodic duty with related
load/speed changes
Relative duty cycle tr1 = 100
Compared to continuous duty S1 a power reduction is necessary in this duty
type. Exact computation is very complex and is possible only with detailed
information from the manufacturer.
Motors
2.10
tA + tB1
tA + tB1 + tBr1 + tB2 + tBr2+ tB3
tBr1 + tB2
tBr2 + tB3

Motors
2.1.9 S9: Duty with nonperiodic load and speed variations
In this mode of operation as shown in Figure 2.11.1 the load and the speed
change nonperiodically within the maximum operating range. Load peaks which
can be far above the rated power may occur frequently. The overload can be
taken into account by selective oversizing.
The duty type cannot be recorded with one simple formula. A suitable continu-
ous load must be used as the reference dimension for the load cycle:
Figure 2.11.1 Duty type S9: Duty with nonperiodic load and speed variations
Compared to continuous duty S1 the equivalent continuous output of duty type
S9 can be lower, the same, or even higher, depending on the load characteristic
and the length of the intervals.
2.11
Identification: Manufacturers and users generally agree on an
equivalent ("equ") continuous output instead of the varying load
for different speeds and irregular operation including overload.
Example: S9, 11 kW equ 740/min; 22 kW equ 1460/min

2.2. Mean values of power, torque and current
In many cases the actual use of a motor diverges from duty types S1 through S9
because the required power P or torque ML and thus current I are not constant.
Since losses Pv change with the square of the load, the individual values (pow-
ers, torques, currents) can be replaced by a mean power Pmi.
Figure 1.12.1 Determining mean power Pmi, mean torque Mmi and mean
current Imi (Ieff).
Mean power Pmi =
These values are determined by a quadratic conversion, as shown in Figure
2.12.1, using the individual outputs and the associated effective times. The maxi-
mum torque which occurs here should not exceed 80% of the pull-out torque for
a three-phase induction motor. However, this type of averaging is not possible
in S2.
Motors
2.12
P1 · t1 + P2 · t2 + P3 · t3
t1 + t2 + t3
2 2 2
Cycle

Motors
When the powers differ by more than a factor of 2, this averaging is too inaccu-
rate, and the calculations must be done with the mean current taken from the
motor characteristics.
Example: In an automatic industrial handling machine the following load cycles
are determined for a cycle duration of 10 minutes:
6 kW for 3 minutes, 3 kW for 2 minutes, 7 kW for 2 minutes, 2 kW for 3 min-
utes:
What is the mean load?
Pmi = = = 4.85 kW
2.13
P1 · t1 + P2 · t2 + P3 · t3 + ...
t1 + t2 + t3 + ...
2 2 2
6 · 3 + 3 · 2 + 7 · 2 + 2 · 3
3 + 2 + 2 + 3
2 2 2 2
Mean power Pmi =
Mean torque Mmi=
Mean current (Ieff) =
P1 · t1 + P2 · t2 + P3 · t3 + ...
t1 + t2 + t3 + ...
2 2 2
M · t1 + M2 · t2 + M3 · t3 + ...
t1 + t2 + t3 + ...
2 2 2
I1 · t1 + I2 · t2 + I3 · t3 + ...
t1 + t2 + t3 + ...
2 2 2

2.3 Motor power and duty types
Duty types S1 through S9 can be divided into two groups, whereby an increase
or decrease of the rated power over S1 is possible or necessary:
2.3.1 Power increase compared to S1
Since in duty types S2, S3 and S6 the machine is not being operated continuous-
ly at full load, but only in blocks, it can cool down again during the stop time
tSt, and therefore it can overloaded mechanically and thermally during the load
period tB. In determining the maximum increase the following variables play an
important part:
To some extent the calculation is not simple. Therefore, many manufacturers of
three-phase induction motors also offer computer programs for motor calcula-
tion. The proper motor can be found quickly and reliably with their aid.
Motors
2.14
Power increase compared to S1: ⇒ for S2, S3 and S6
Power reduction compared to S1: ⇒ for S4, S5, S7 and S8
Pn Rated power of the motor in kW
Pmech Mechanical limit rating of the motor in kW
Pth Thermal limit rating of the motor in kW
Mn Rated torque in Nm
MK Pull-out torque in Nm
T Thermal time constant in minutes (Table 2.18.1)
k0 Ratio of equivalent no-load/load losses (Table 2.18.2)
tr Relative duty cycle in %
h Ratio of ventilated/unventilated heat dissipation (Table 2.19.1)
z0 No-load reversing frequency per hour (Table 2.19.2)

2.3.2 Mechanical limit rating
When the power is increased in duty types S2, S3, and S6 the mechanical limit
rating Pmech must be noted. Standards state: "It must be possible to overload
multiphase induction motors regardless of their duty type and design for
15 seconds at the rated voltage and input frequency up to 1.6 times the rated
torque." Catalog data however are subject to tolerances up to -10% so that the
pull-out torque MK should be higher by a factor of ≤ 1.76 with respect to the
new increased torque Mmax. Therefore the mechanical limit rating can be
defined as follows with regard to catalog data:
2.3.3 Power reduction compared to S1
In duty types S4, S5, S7, S8 and S9 the motor power must be reduced, since in
all these cases starting losses or braking losses play a major part.
The computational method is based on the maximum no-load change-over fre-
quency z0 as shown in Table 2.19.2. This is the maximum allowable hourly
number of reversals without the motor becoming too hot. The maximum allow-
able change-over frequency z for a certain load conditions can then be deter-
mined using reduction factors such as the factor of inertia, counter-torque factor,
and load factor.
The factor of inertia FI takes into account the external moments of inertia such
as the moment of inertia of the motor JMot and load moment of inertia Jzus:
2.15
Motors
Mechanical limit rating Pmech ≤ ·
Pn = rated power in W
Mn = rated torque in Nm
Mk = pull-out torque in Nm
MK
Mn
Pn
1.76
Factor of inertia FI =
JMot = moment of inertia of the motor in kgm2
Jzus = load moment of inertia in kgm2
JMot + Jzus
JMot

If the speeds of the driven machine and the motor are not the same, all moments
of inertia must be converted to the motor speed nMot:
The counter-torque factor kg takes into account a mean load torque ML which is
present during acceleration and which must be overcome by the mean motor
torque MMot:
When gears with gear efficiency hG are used and thus speeds are different, the
load torques of the driven machine must be converted to the motor speed nn:
Motors
2.16
Converted load moment of inertia Jzus =
J = moment of inertia in kgm2
n = speed/min
J1 · n2
1 + J2 · n2
2 +...
n2
Mot
Counter-torque factor kg = 1 -
ML = load torque MMot = motor torque
ML
MMot
Converted load torques ML = + + ...
M = torque in Nm n = speed/min
η = gear efficiency
ML1 · n1
ηG1 · nn
ML2 · n2
ηG2 · nn

Due to the effect of the starting process with
respect to heating, the rated power Pn of the
motor should be chosen to be larger than is
required by the actual power demand P.
tA = starting time, tB = load time,
tSt = stop period, tS = cycle duration
Figure 2.17.1 Duty type S4 for periodic duty of an automatic machining
center
Due to the effect of the starting and braking
process with respect to heating, the rated
power Pn of the motor should be chosen to be
larger than is required by the actual power
demand P.
tA = starting time, tB = load time,
tBr = braking time, tSt = stop period,
tS = cycle duration
Figure 2.17.2 Duty type S5 for periodic duty of a circular saw
0 0.5 1 n/ns
Figure 2.17.3 Typical range of variation of the torque characteristic for
three-phase induction motors
2.17
Motors
power P
speed n
power P
speed n

The load factor kL with which the load is taken into account during operation.
In cases in which the load characteristic is not exactly known the following
applies:
Table 2.18.1 Typical heating time constant T in minutes for induction motors
Table2.18.2 Typical ratio of equivalent losses KO at no load to those in
operation
Motors
2.18
Load factor kL = 1 - (P / Pn)2
·
kL= Load factor
P = Required power in kW
Pn = Rated power of the motor
k0 = Ratio of equivalent no-load/load losses (Table 2.18.2
h = Ratio of ventilated /unventilated heat dissipation (Table 2.19.1)
tr = Relative duty cycle (see duty types S1...S9)
(1 - ko)tr
(1 - ko)tr + (1 - tr)h
Pn rated power 2 pole 4 pole 6 pole 8 pole
kW min min min min
0.09 … 1.1 7 … 10 11 … 10 12 —
1.5 … 3.0 5 … 8 9 … 12 12 12 … 16
4.0 14 11 13 12
5.5 … 18.5 11 … 15 10 … 19 13 … 20 10 … 14
22 … 45 25 … 35 30 … 40 40 … 50 45 … 55
55 … 90 40 45 … 50 50 … 55 55 … 65
110 … 132 45 … 50 55 60 75
kW
0.guatda.com/cmx.p09...1.5 0.35 0.45 0.5 0.5
2.guatda.com/cmx.p2...18.5 0.25 0.25 0.3 0.3
22
30...55 0.25 0.3 0.3 0.3
75...160 0.35 0.35 0.3 0.3

Equivalent losses are the sum of the percentages of individual losses which con-
tribute to heating of the winding, such as load, core and rotor losses.
Table 2.19.1 Typical ratio h of heat dissipation between unventilated and
ventilated motors
Table 2.19.2 Typical no-load change-over frequency z0 per hour
2.19
Motors
kW
0.guatda.com/cmx.p09...18.5 0.4 0.45 0.5 0.5
22...500 0.2 0.3 0.3 0.3
Size 2-pole 4-pole 6-pole 8-pole
56 2 300 5 000 8 000 -
63 3 000 8 600 8 000 -
71 4 000 6900 6 000 7 000
80 1 700 5 000 5 500 8 000
90S 2 000 3 000 7 900 11 000
90L 2 000 2 500 6 200 11 000
100L 1 000 4 000 5 100 10 000
112M 720 1700 3 200 2 500
132S 450 850 2 200 2 800
132M - 1000 1 700 3 000
160M 400 900 1 700 2 300
160L 400 900 1 600 2 300
180M 200 600 - -
180L - 550 800 1 200
200L 150 400 620 900
225S - 280 - 700
225M 90 270 450 670
250M 60 200 320 500
280S 41 130 260 400
280M 39 120 240 370
315S 34 100 180 300
315M 32 90 170 269

3.1
3 Characteristic Load Torques
Motors are correctly sized when they are operated on the average with the rated
torque Mn at the rated speed nn. Then they will deliver the rated output Pn and
consume the rated current In. The torque characteristic of most driven machines
can be assigned to typical and thus characteristic curves; this greatly facilitates
motor design.
Loads or driven machines are mechanical devices which are used to machine or
shape materials, such as machine tools, presses, calenders, centrifuge, etc., but
also conveyor systems such as cranes, conveyor belts, and traversing mecha-
nisms. Furthermore, pumps and fans can be combined into one group. In very
large and complex machinery such as rolling mills or paper-making machines,
the system is divided into parts and the individual motors are examined separate-
ly. The detailed structure of the driven machine is generally not considered for
the motor design. Usually it can be described accurately enough by the torque
characteristic ML = f(n) or ML = f(t), speed as a function of time n = f(t), by the
maximum allowable acceleration/deceleration and the entire moment of inertia,
relative to the drive shaft.
The characteristics generally differ greatly between no-load and full load. The
moment of inertia can also vary, depending on whether there is more or less
process material in the machine.
For motor dimensioning and for verification of starting and braking cycles,
knowledge of the behavior of the load torque ML as a function of speed is
extremely important.
Any driven machine applies a certain torque against the motor which is generally
dependent on speed. It is also called the steady-state torque and is dictated essen-
tially by the technological process. In general it acts against the direction of
motion, except in lifting mechanisms during the lowering motion, where it acts
in the direction of motion. In addition there are acceleration and deceleration
torques when the speed changes; they are determined by the moment of inertia.
The load torque characteristic in a motor is often typical and can therefore be
described with certain features. This is called the classification of driven
machines.
Motors

In order to gain an overview of the many different driven machine designs, they
are categorized by their typical load characteristics or output curves as shown in
Figure 3.2.1 and Figure 3.4.1. Here it should be observed that for example fans
and compressors exhibit different characteristics, depending on whether they are
run under full load or no load. It is better to start them unloaded.
Figure 3.2.1 Torque or output characteristic for typical loads as a function of
speed
a M ≈ const. ⇒ P proportional to n
b M ≈ proportional to n, ⇒ P proportional to n2
c M ≈ proportional to n2
⇒ P proportional to n3
d M ≈ proportional to 1/n ⇒ P ≈ const.
In many cases the mean load torque MLm is important. For a known torque
characteristic it can be determined according to the torque Mn after completed
acceleration.
3.1 Load torques as a function of speed
The physical principles of motor engineering teach that the mechanical power P
of a motor is a function of the torque M and speed n or angular velocity ω:
3.1.1 Torque remains constant
The torque of a driven machine results essentially from mechanical friction
which remains constant in a wide range of speeds, as shown in Figure 3.2.1 a.
During starting increased static friction must often be overcome.
Motors
3.2
M = const.
P = const.

Motors
3.3
Examples of mechanical loads with constant torque are:
- lifting mechanisms, elevators, winches
- machine tools with a constant cutting force
- conveyor belts, feed motors
- grinders without fan action
- piston pumps and compressors at constant pressure
- roller mills
- in part also shears and punches
- planers
- bearings, gearing
The mean load torque MLm in these applications corresponds roughly to the
rated torque MN of the load. Thus, in these applications the power P can be pro-
portionally reduced by reducing the speed n. Cutting the speed in half cuts the
power in half.
3.1.2 Torque increases in proportion to speed
This relationship arises as shown in Figure 3.2.1 for example in speed-propor-
tional friction (viscous friction) during rolling and processing of paper, textiles or
rubber tiles.
Examples are:
- calenders, extruders
- paper and textile glazing
- eddy-current brakes
The mean load torque MLm in these applications is roughly half the rated torque
Mn / 2. When the speed n is reduced the power P decreases by its square. When
speed n is cut in half the power P is only one fourth.
P = M · 2 π · n = M · ω
At a constant torque M the power P is proportionally a function of
the speed n
P ~ n
When the torque M increase proportionally, power P increases with
the square of the speed n:
P ~ n2

Figure 3.4.1 Typical load-torque characteristic of driven machines with start-up
A Various applications
a elevators, lifts, feed motors
b metal-cutting machine tools
c slow-speed vehicles, c' high-speed vehicles
d extruders
e calenders
B Compressors
f back-pressure piston compressors, f' unloaded
g back pressure rotary compressors, g' unloaded
h turbocompressors
C Fans
i back-pressure fans or centrifugal pumps, i' fans unloaded
k rotary piston blowers, k' unloaded
D Mills
l ball mills
m centrifugal mills
n hammer mills
o impact mills
Motors
3.4
motors compressors
millsfans
1.2
1.0
0.8
0.6
0.4
0.2
0
1.2
1.0
0.8
0.6
0.4
0.2
0
0.8
0.6
0.4
0.2
0
0.8
0.6
0.4
0.2
0
0 0.2 0.4 0.6 0.8 1.0 0 0.2 0.4 0.6 0.8 1.0
0 0.2 0.4 0.6 0.8 1.0 0 0.2 0.4 0.6 0.8 1.0

3.1.3 Torque increases with the square of speed
This relationship arises as shown in Figure 3.2.1 primarily when there is gas or
liquid friction.
Examples are:
- blowers and fans of all types
- propellers
- piston engines with delivery into an open pipe circuit
- centrifugal pumps
- stirring apparatus, centrifuges
- vehicles
The mean load torque MLm is roughly one third of the rated torque: Mn/3.
Because the torque M increases quadratically as the speed n increases, the power
P is a function of the cube of the speed. Cutting the speed in half requires only
one eighth of the power.
This relationship is important, for example, in pump and fan motors for heating
and ventilation motors. Instead of reducing the amount of delivery with a slide
valve or throttle valve, it is better to adjust the speed of the drive motor.
3.1.4 Torque decreases in inverse proportion to speed
As the speed increases, as shown in Figure 3.2.1, the torque drops. Examples
are:
- facing lathes
- rotary peeling machines
- winding machines
- coilers
The mean load torque ML can only be determined on a graph.
3.5
Motors
When the torque M increases quadratically, the power P increases
with the cube of the speed n.
P ~ n3
If the torque M decreases in inverse proportion to the speed n, the
power P remains constant.
P ≈ const.

3.2 Load torques as a function of angle
These characteristics appear in machinery with reciprocating motion, for exam-
ple, in table motors. They are also present in piston machinery (compressors in
heat pumps) due to intermittent loading. The electric input current of the drive
motor follows this motion cycle and can generate a rhythmically fluctuating
voltage drop in the line. Generally a so-called torque force diagram is plotted in
the planning of these applications.
3.3 Load torques as a function of path
They are typical, for example, in vehicles, or in table motors, cableways and con-
veyor belts.
3.4 Load torques as a function of time
These motors are loaded intermittently or periodically. Examples are:
- punches
- hoists
- conveyor systems
- rock crushers
- ball mills
3.5 Breakaway torque
Another important concept is the so-called breakaway or static torque which is
caused by static friction. In order for a motor to start reliably, this value should
be known as accurately as possible and the starting torque MA of the motor
should exceed the load torque. In large machines with slide bearings it may sig-
nificantly exceed the rated torque Mn.
Figure 3.4.1 shows certain torque characteristics of common driven machines.
Comparison with Figure 3.2.1 shows that most of them have a typical character-
istic and thus classification is possible.
Example: The speed of an induction motor operated with a load controller can be
infinitely adjusted between 50% and 100%. How does this affect the delivery
rate of a piston or centrifugal pump?
• Piston pump: The torque demand is almost independent of speed as shown in
Figure 3.2.1 a, and the torque remains almost constant. The delivery output is
therefore proportional to the speed. At half speed it also falls accordingly to
P' = P . 0.50 = 50%
Motors
3.6

Motors
• Centrifugal pump: In centrifugal pumps, as shown in Figure 3.2.1 c, there is
a quadratic relationship between torque demand and speed. Therefore the
power changes in the cube. At half-speed the power is thus P' = P . 0.53 =
0.125 = 12.5%. The delivery rate can therefore be reduced to one eighth of
the original value.
The example shows how automatic speed control greatly influences the power of
a driven machine.
3.7

4.1
4 Choosing and Dimensioning Electric Motors
Electric motors are energy converters for kinematic processes as they occur in
the technology of most driven machines. Examples are:
• Motor applications:
- machine tools
- cranes, elevators, vehicles
- pumps, fans, compressors
- presses, bending machines, rolling mills, calenders, etc.
• Actuator processes:
-slides and valves
- feed devices, robot applications
- kinematic processes in control linkages
All kinematic processes involve the quantities force - torque - power - energy
and time. Solids, liquids, or gases change their location as a function of time.
But other concepts such as velocity, acceleration, efficiency, etc., also play a part.
Electric motors draw energy from a utility supply and convert it into mechanical
energy. Auxiliary devices such as clutches, transmissions, gears, brakes and dri-
ven machines can be located between the motor and the actual load, i.e., the
moving solid, liquid, or gas. To choose and dimension a motor the relevant para-
meters of all element in the chain of energy flow, starting with the actual load,
must be determined with relative accuracy. Proper selection is therefore impor-
tant. For proper selection of a motor it is necessary to find an ideal motor for the
kinematic task at hand. Even more important than the appropriate motor type
with accessories such as gears, brakes, clutches, etc., is the proper sizing of the
motor.
An undersized motor will fail in continuous duty. An oversized motor causes
unnecessary expenses, runs uneconomically (greater procurement costs, poorer
operating efficiency and higher losses, requires more reactive power) and may
load the machine with an excessively high acceleration torque.
Motors

In any case, the basic application conditions will have to be defined, whereby the
following factors are significant:
• power transmission: As a single drive the motor can be coupled to the load
directly or via a transmission, or it can be used as a central motor connected
to intermediate shafts, belt and chain drives, etc.
• operating conditions such as overload capacity, frequency of starting, operat-
ing mode, peak torques, ambient temperature, etc., affect not only the motor
size requirement, but also the selection of motor accessories.
• space conditions and the layout possibilities of the entire system affect main-
ly the choice of motor accessories.
4.1 Motor Capacity
The three-phase induction motor is most widely used in drive technologies
because of its simple mechanical and electrical structure and due to its high reli-
ability. Its application is limited only by its torque and speed characteristics.
In the stator winding as well as in the rotor the current passage generates heat;
this heat may not exceed the temperatures specified for insulation materials IP
class. The temperatures which develop depend on the level of the motor load, its
variation over time, and cooling conditions. Motors should be sized such that at
constant load with rated power and rated cooling conditions they do not exceed
maximum temperatures.
• The torque required for accelerating the centrifugal mass increases motor
acceleration time. The starting current flowing during this time heats up the
winding dramatically.
• The maximum change-over frequency, i.e., the number of consecutive starts,
is limited. During frequent starting processes the motor reaches its allowable
temperature limit even without load torque and without an additional cen-
trifugal mass.
• The duty cycle is another important factor for selection. The cooling time at
switching intervals must be long enough to ensure that the temperature limit
is not exceeded during subsequent starting. If the duty cycle is short, the
motor can accept a higher load since it cannot heat up to the temperature limit
during this short time and cools down again during the intervals.
• Undersized motors can be thermally overloaded because of an overly long
starting time, whereas oversized motors would overload the transmission and
the driven machine during the starting process.
Motors
4.2

Motors
4.1.1 Catalog data and application parameters
For most application requirements a so-called "standard motor", usually an
induction motor, is used. The following information applies to this type of motor
unless indicated otherwise. Induction motors can be used in a wide range of
applications. In order to select a suitable motor in accordance with manufacturer
specifications minimum requirements must be established. The objective is to
establish requirements regarding
• power supply
• electrical and mechanical characteristics of the motor
• operating conditions
• investment, operating and maintenance costs
• service life
• environmental protection and accident protection measures.
Based on these requirements, a suitable motor and appropriate auxiliary devices
can be selected.
Table 4.3.1 Selection factors for motor type and rated power
4.3
Selection factor Motor feature
Torque ⇒ Power
Moment of inertia ⇒ Starting time
Typical load torques ⇒ Motor torque
Design analysis by ⇒ Optimization
- load torque - motor torque
- acceleration torque - starting time
- acceleration time - acceleration capacity
- reversing frequency - motor heating
Operating modes ⇒ Motor heating
Starting conditions ⇒ Torque characteristic
Braking and reversing ⇒ Brake heat
Thermal processes ⇒ Capacity

4.1.2 Determination of unit rating
The unit rating of a motor can be determined according to various aspects, since
every application requirement is different. The outline in Table 4.3.1 indicates
which selection factors are important:
4.1.3 Catalog data
The degree to which an individual motor meets requirements can be determined
by comparison of the motor to the manufacturer's catalog data. Table 4.5.1 lists
the most important parameters to be observed, depending on the application.
Some of these parameters have been standardized, others are specific to the
manufacturer or can be selected by the customer, generally from several alterna-
tives. Therefore the design engineer often has a certain freedom of choice in
defining the details of a motor. Many manufacturers offer modular motor
designs. The following specifications can usually be defined when ordering
• rotor design and thus the torque characteristic
• cooling system
• insulation class of the windings
• style
• type of installation
• degree of protection and protective devices as well as other data.
4.1.4 Operating conditions
For design purposes the operating conditions and the parameters of the driven
load are as important as the motor data.
Table 4.6.1 shows the most important data to be observed for design. In critical
cases the proper drive motor for the given motor task should be selected in
cooperation with the motor supplier.
4.1.5 Procedure for selecting motors
Most motors are operated in continuous duty S1. The first selection considera-
tion is the output in continuous duty. Since the service life of electrical machin-
ery depends largely on the continuous operating temperature, the choice must be
made carefully. As a second step, the suitability of the motor for the starting
conditions should be examined with respect to starting time or starting torque. In
motors with complex operating modes (S2 ... S9) basically the same consider-
ations apply, whereas consultations with the suppliers are usually necessary due
to the changing load conditions and the fluctuating winding temperatures.
Motors
4.4

Table 4.5.1 Catalog data for motors
4.5
Motors
Data to be defined Remarks
Electrical requirements
Type of current Operating voltage, for multi-
Three-phase current, voltage motors indicate all
single phase current V values and possible tolerances
Frequency Hz
Catalog Data
Type designation Manufacturer specifications
Rating For motors with several speeds,
rating per speed
Speed For motors with several poles, speed
per output
Rated current A Manufacturer specifications
Breakaway starting/rated current Manufacturer specifications
Torque Nm For special applications
Breakaway/rated torque Manufacturer specifications
Pull-up/rated torque Manufacturer specifications
Pull-out/rated torque Manufacturer specifications
Moment of inertia kgm2 Manufacturer specifications
Efficiency η % Manufacturer specifications
Max. blocking time s Manufacturer specifications
Max. starting time s Manufacturer specifications
Tolerances Established in standards
Type of design
Switching For star-delta starting, always
Delta, star specify delta
Rotor type
Cage rotor, wound rotor
Model IM.. IEC 34-7, Part 7
Type of protection IP.. IEC 34-7, Part 7
Type of cooling
Natural, inner cooling
Self, surface cooling
Separate, closed circuit cooling
Insulation class
B, F, H Indicate temp. limit, if required
Vibration amplitude Normal or reduced
Noise level db
Special regulations Elect. and mech. regulations
Terminal box Indicate type of protection
and design if necessary
Shaft ends Indicate type of protection
and design if necessary
Built-on, built-in components Indicate switch or plug, if necessary
Brakes, tachogenerator
Separately ventilation, space heater
Temperature measuring instruments For bearings or stator windings
- Thermistor protection
- Bimetallic switch Make contacts or break contacts
- PTC resistors

Table 4.6.1 Important data for motor design
Motors
4.6
Data to be defined Remarks
Counter-torque Nm Convert for motor shaft if nec.
- constant
- quadratically increasing
- special curve Discuss with manufacturer, if necessary
Moment of inertia of load kgm2
Convert for max. motor speed
Type of starting
- star-delta Intensified star-delta starting, if req.
- full load starting
- no-load starting
- other methods Soft starter or load controller, if req.
Electrical braking Plugging or dynamic braking
Operating mode
S1 Continuous operation
S2 min Temporary duty
S3 % Intermittent periodic duty-type without
starting
S4 %, c/h Intermittent periodic duty with starting
S5 %, c/h Intermittent periodic duty with starting
and electrical braking
S6 % Continuous-operation duty type
S7 c/h Continuous operation-duty with starting
and electrical braking
S8 %, c/h Continuous-operation periodic duty
with related load /speed changes
S9 Duty with nonperiodic load and speed
variations
Ambient temperature oC
Altitude meters above sea level
Direction of rotation clockwise, counterclockwise, or both
Speed adjustment method and from...to...
Climatic influences Also consider relative humidity
Bearing and shaft load
Axial force N Force direction with respect to shaft
position
Radial force N Indicate distance from shaft shoulder
Rotary forces N

4.2 Dimensioning using load torque
The load torque ML results from the counter-torque of the driven machine plus
the efficiency η with which all mechanical losses are recorded.
According to the load characteristics the load torque during acceleration can
- gradually build up (for example, fan)
- reach the rated value at the start (for example, hoists)
- be present only after acceleration (for example, wood-working machines)
- be present constantly or intermittently
For a constant load torque ML = const. and rated speed n, the calculation is done
using the following relation:
In a hoist, for lifting power P with a certain speed v and force F, and with con-
sideration of efficiency η, we find:
At any time during acceleration the load torque ML must be lower than the
respective motor torque MM. If this is not the case, no acceleration to higher
speeds takes place.
4.7
Motors
P = power in W
Power P = M = torque in Nm
n = speed/min
η = efficiency
M · n
9.55 · η
P = lifting power in W
Power P = F = lifting force in N
v = lifting speed in m/s
η = efficiency
F · v
η

4.3 Calculation using acceleration torque or acceleration time
4.3.1 Acceleration torque
A load can only be accelerated when the driving motor provides a greater torque
than the load requires at the time. The difference is called the acceleration
torque MB. The acceleration torque and the flywheel moment of the motor,
transmission, and system to be accelerated yield the acceleration time tA. In
many cases the simplified assumption is made that the load torque is constant
during acceleration. This assumption is reached by calculating an average load
torque and replacing the variable motor torque by a constant mean acceleration
torque which is determined from the characteristic.
For a certain starting time tA the required acceleration torque MB is computed as
follows:
4.3.2 Acceleration time
The acceleration time tA can be determined from the relation above, if the mean
acceleration torque MB is known. A relatively simple method of determining it
is shown in Figure 4.8.1. The motor torque MM and load torque ML are plotted
on graph paper and then the mean torques can be defined graphically, e.g.,
by counting the squares. The final diagram will show the mean acceleration
torque MB.
MM motor torque
ML load torque
Mbmi mean acceleration torque
nb operating speed
Figure 4.8.1 Determining the mean acceleration torque by balancing the area on
graph paper
Motors
4.8
Acceleration torque
MB = Mm - ML = J' · α = J' · = =
MM = motor torque in Nm ML = load torque in Nm
tA = starting time in s α = angular acceleration/s2
n = motor speed/min ω = angular speed/s
MB = mean acceleration torque in Nm
J' = moment of inertia in kgm2 reduced to the motor shaft
ω
tΑ
J' · n
9.55 · tA
J' · 2π · n
60 · tA

Motors
Example: Let a two-pole motor with n = 2980 rpm, P = 110 kW, J = 1.3 kgm2
at no-load have an average acceleration torque MB = 1.5 . Mn.
How long is
a) the starting time at no-load?
b) the starting time together with a load of JL = 1000 kgm2 at a
speed of nL = 300 rpm if it continuously demands the rated torque
during acceleration?
Solution: a) Starting time at no-load
Rated torque of the motor Mn = = = 352.5 Nm
Acceleration torque MB = 1.5 · Mn = 1.5 · 352 Nm = 528.7 Nm
Acceleration time tA = = = 0.76 s
b) Acceleration time with load
The moment of inertia of the load converted to the motor speed is:
J' = JL · (nL/n)2
= 1000 kgm2
· (300 rpm/2980 rpm)2
= 10.1 kgm2
The effective acceleration moment together with the load can be derived from
the difference of the mean acceleration torque of the motor minus the continu-
ously demanded rated torque of the load:
MB = 1.5Mn - Mn = 0.5·Mn
Acceleration time tA = = = 20 s
4.9
Acceleration time in s tA =
MB = mean acceleration torque in Nm
J' = moment of inertia reduced to the motor shaft in kgm2
n = motor speed/min
J’ · n
9.55 · MB
P · 60
2π · n
110 000 W · 60
2π · 2 980/min
J · n
9.55 · MB
1.3 kgm2
· 2 980 VPM
9.55 · 528.7 Nm
(J'+ JMot) · n
9.55 · MB
(10.1+1.3) kgm2
· 2 980 rpm
9.55 · 0.5 · 352.5 Nm

In choosing the motor the acceleration time tA, with consideration of the
change-over frequency, must be shorter than the maximum time specified by the
manufacturer. Unloaded motors and motors with only little additional centrifugal
masses such as clutches. etc. reach their idle speed very quickly. This is also
generally the case in starting with a load. Only when large centrifugal masses
must be accelerated are starting times very long. This is called heavy starting,
which is the case, for example, in centrifuges, ball mills, calenders, transport
systems and large fans. These applications often require special motors and the
corresponding switchgear. Figure 4.10.1 shows the reference values for the
starting time of standard motors as a function of rated power.
Figure 4.10.1 Typical reference values for starting time of standard motors
as a function of rated operating power
1 no-load starting (motor + clutch)
2 starting under load (without large centrifugal mass)
If the curve of the load torque ML is complex and the motor torque MM is not
constant, it is advantageous to divide the computation into individual zones as
shown in Figure 4.11.1 Then the acceleration times for the individual zones plus
the average acceleration torques which take effect in the segment are computed
and added for the individual speed segments (for example, 20% speed increase
per segment).
Motors
4.10
0.2 0.4 1 2 4 10 20 40 100 200
StartingTime(s)
Rated Operating Power kW
10
4
2
1
0.4
0.2
0.1
0.04
0.02

4.4 Calculation using change-over frequency
Frequent starting of motors is called switching mode and the maximum change-
over frequency per hour must be checked. The manufacturer's data usually show
the allowable no-load switching per hour, i.e., the number of change-overs at
which the motor reaches its maximum temperature without load and without an
additional flywheel moment during idle operation. The frequency of change-
over plays an important role in operating mode S4.
The allowable frequency of change-over of a motor is determined by its temper-
ature limit. It is derived from the square mean value of current from the cycle
characteristic. This mean value may not exceed the rated current of the
machine.
Figure 4.11.1 Acceleration torque for computing the acceleration time when
the motor torque MM and the load torque ML are not constant
and exhibit a dramatically different behavior.
4.11
Motors
Acceleration time for non-constant torques
tA = starting time in s
tA = J' = moment of inertia reduced to the motor shaft
in kgm2
∆n = speed difference in rpm
MB = acceleration torque in Nm
∑J' · ∆n
9.55 · MB
rpm

Excessive change-overs which cause a response of protective devices or even
destruction of the motor often occur during the commissioning phase, adjust-
ments, and jogging.
Often an additional inertia mass causes a load condition. In this case the num-
ber of allowable switchings zz per hour can be computed based on the switching
mode energy principle:
In switched duty with an existing load moment ML the number of allowable
switchings zL per hour is determined as follows:
In practice there are usually a load flywheel Jz and an additional load torque
ML. Thus the following applies to the number zZul of allowable switchings per
hour:
zZul = zz · = z0 · and converted:
Motors
4.12
Allowable switching operations with additional mass
zz = allowable switching operations per hour with
additional mass
zz = z0 = allowable no-load switching operations per hour
JM= Massenträgheitsmoment des Motors in kgm2
Jz= reduced additional mass moment of inertia in kgm2
z0 · JM
JM + Jz
Allowable switchings with load torque
zL =
zL = allowable switchings per hour with load torque
z0 = allowable no-load switching operations per hour
MM = mean motor torque during acceleration in Nm
ML = mean load torque during acceleration in Nm
z0 · (MM - ML)
MM
zL
z0
JM · (MM - ML)
(JZ + JM) · MM

Motors
Table 4.13.1 Typical no-load change-over frequency z0 per hour
4.5 Choosing with the use of catalog data
Using the mean values for power Pmi, torque Mmi and current Imi that were
computed for less demanding conditions a motor can be chosen using catalog
data, whereby the corresponding catalog data may not be less than the computed
averages:
Pmi ≤ Pn, Mmi ≤ Mn, Imi ≤ In
Most motor applications can be assigned to the 9 duty types S1 through S9. In
more complex situations, where a definite selection is not possible, a similar
duty type can be defined and then converted to S1. This method, however,
requires detailed knowledge with respect to thermal time constants and cooling
conditions. The motor manufacturer can supply these data.
4.13
Allowable switchings with additional load and flywheel moment
zL = z0 ·
zL = allowable switching operations per hour with load flywheel and
load torque
z0 = allowable no-load switchings
MMmi = mean motor torque during acceleration in Nm
MLmi = mean load torque during acceleration in Nm
Jz = reduced additional mass moment of inertia in kgm2
JM = mass moment of inertia of the motor in kgm2
1 - MLmi / MMmi
1 + Jz / JM
Pn Rated power 2-pole 4-pole 6-pole 8-pole
kW
0.guatda.com/cmx.p09...1.5 1500...4000 2500...8500 5500...8000 7000...11000
2.guatda.com/cmx.p2...18.5 400...1000 800...4000 1500...5000 2000...10000
22 200 600 800 1200
30...55 50...150 200...400 300...600 500...900
75...160 30...40 90...130 170...260 270...400

Motors
4.14
5 Equation Symbols
Symbol Meaning Unit Remark
f frequency s-1 line frequency
FI factor of inertia
h ratio of ventilated/
unventilated heat release
I current A supply line current
Imi mean current (Ieff) A effective value
In rated current A maximum continuous
current
J' moment of inertia
reduced to the motor shaft kgm2
Jext load moment of inertia in
reference to the motor
shaft kgm2
JM moment of inertia of motor kgm2
Jmot motor moment of inertia kgm2
JZ reduced additional mass
moment of inertia kgm2
Jzus additional moment of
inertia kgm2
k0 ratio of equivalent
load/no-load losses
kg counter-torque factor Nm
kL load factor Nm
M torque Nm
MA breakaway torque Nm
MB acceleration torque Nm
MK pull-out torque Nm
ML load torque Nm
MLmi mean load torque
during acceleration Nm
MM motor torque Nm
MMmi mean motor torque
during acceleration Nm
Mmi mean torque Nm
Mn rated torque Nm
MS pull-up torque Nm

4.15
Motors
n speed rpm
n operating speed rpm
n0 no-load speed rpm
nn rated speed rpm
ns synchronous speed rpm
p pole pair number
(pole number/2)
P power kW
P2 output power kW
P1 input power kW
PCu load loss kW
PCuR ohmic loss in rotor kW square function
of current
PCuS ohmic loss in stator kW square function of
current
PFe core loss in stator kW roughly constant in
operation
PLa bearing friction loss kW roughly constant in
operation
PLu windage loss kW roughly constant in
operation
Pmech motor mech. limit rating kW
Pmi average power kW
Pn rated power kW
Pth thermal limit rating kW
Pv losses kW
PVR loss in rotor kW
Pzus stray loss kW roughly constant in
operation
s slip kW
S1 continuous duty
S2 temporary duty
S3 intermittent periodic duty-type ...without starting
S4 intermittent periodic duty ...with starting
S5 intermittent periodic duty ...with starting and
electrical braking

Motors
4.16
Table of symbols and units
S6 continuous-operation duty type ... with interucittent
periodic load
S7 continuous-operation duty ... with starting and
electrical braking
S8 continuous-operation ... with related load
periodic duty /speed changes
S9 duty with non-periodic load
and speed variations
t time s, min, h
T thermal time constant min
tA starting time s, min
tB load time, operating time s, min
tB operating time s, min
tBr braking time s, min
tL no-load time s, min, h
tr relative duty cycle %
tS cycle duration s, min, h
tSt stopping time s, min, h
U voltage V
z0 no-load change-over
frequency h-1 (per hour)
zA no-load starting
frequency h-1
zL allowable switching operations
per hour with load torque and
possible additional mass h-1
zz allowable switching operations
per hour with additional mass h-1
zzul allowable change-over
frequency h-1
η efficiency %
ϑ temperature °C
ϑmax maximum temperature °C
∆n speed differential rpm
cosϕ power factor

Publication WP-Motors, Nov. 96 Printed in Switzerland
Power equipment Power contactors and motor starters
Motor protection
Motor control centers
Power monitoring
Control and load switches
Relays
Sensor technology Limit, photoelectric and proximity switches
Pressure and temperature sensors
Identification systems (HF)
Bar code reader systems
Encoders
Image processing systems
Controllers Control devices and signalling units
Text and LCD displays
Control consoles
Industrial computers
Visualization software
Drive engineering Soft starters
Frequency converters
AC and DC drives
Axis controls and servo drives
CNC controls
Automation Programmable controls
Digital and analog I/O
Intelligent peripheral modules
Communications Networks and field bus systems
Open communications networks (MAP)
System solutions Custom developments
Process/batch controls
Burner controls
Die-casting and press controls
SCADA
Quality assurance Statistic data acquisition and analysis
Service Worldwide service and support
Customer training
Repair and spare parts service
Technical consultation
More than 350,000 possibilities for improving your automation system
Germany
Rockwell Automation GmbH
Zweigniederlassung der
Rockwell International GmbH
Düsselberger Straße 15
D-42781 Haan
Telephone 02104-960-0
Fax 02104-960-121
Austria
Rockwell Automation GmbH
Bäckermühlweg 1
A-4030 Linz
Telephone 07-38909
Fax 07-385 651 61
Switzerland
Rockwell Automation AG
Verkaufszentrum Gewerbepark
Postfach 64
CH-5506 Mägenwil
Telephone 062 889 77 77
Fax 062 889 77 66

Application basics of operation

More Related Content

What's hot (20)

Similar to Application basics of operation (20)

More from Ahmed Mohammed Alhntoshi (19)

Recently uploaded (20)

Application basics of operation