Motor Protection
Niwat Sriklam
Introduction
Many differential application
Differential motor characteristics
Difficult to standardise protection
Protection applied range from
FUSE ÎÎ RELAYS
Introduction
COST & EXTENT = POTENTIAL
OF PROTECTION HAZARDS
SIZE OF MOTOR,
TYPE & IMPORTANCE
OF THE LOAD
Motor Protection
System Motor Circuit Load
-Voltage dips -Insulation failure -Overload
-Voltage Unbalance -Open circuits -Locked rotor
-Loss of Supply -Short circuit -Coupling faults
-Overheating -Bearing faults
~
Motor Protection Application
Switching
Voltage Rating Protection
Device
< 600V < 11kW Contractor i) Fuses
ii) Fuses + Direct acting
Thermal O/L + U/V
releases
< 600V 11-300kW Contractor Fuses + Electronic O/L +
Time Delay Earth Fault
3.3 kV 100kW-1.5MW Contractor Options :- Stalling Under
Current
6.6 kV 1MW-3MW Contractor
6.6 kV >1MW Circuit Breaker As above
+ Instantaneous O/C
11 kV >1MW Circuit Breaker + Differential
Introduction
Protection must be able to :-
Operate for abnormal conditions
Protection must not :-
Affect normal motor operation
Consideration :-
Starting current
Starting time
Full load current
Stall withstand time (hot & cold)
Thermal withstand
Motor Currents
Induction Motor
Station field f
fr
Define slip, S, as the PER UNIT difference in speed between
the Stator and Rotor field
Slip ‘S’ = (f - fr)/f
Speed of stator field relative to rotor
(f - fr) = sf
Motor Currents
Induction motor
Magnitude of induced voltage : Proportional to sf
Frequency of Induction rotor current : Equal to sf
R2
X2 = 2¶fL
kVs (Stand Still)
Rotor Equivalent Circuit
Standstill :
R2
kVs X2 = 2¶fL = rotor reactance at (Stand Still)
Running :
R2 Rotor Current = skVs
skVs 2¶fL = sX2
[ R22 + S2X22]½
Rotor Current = kVs
[ R22 + X22]½
S2
R2/s
kVs X2
Motor Starting Characteristic
Rotor Current = skVs time
[ R22 + S2X22]½
Rotor Current = kVs
[ R22 + X22]½
S2
X2 >> R2
Therefore R2 >> X2
When S is small
Start
Time
Full load Current
Current
Mechanical Overload
Overload
Heating
Insulation
Deterioration
Over Load Protection
FUSES Thermal Replica
Motor Heating
HEAT STORED
Î INCREASE
THE MOTOR TEMPERATURE
HEAT DEVELOPED AT
A CONSTANT RATED
DUE TO CURRENT FLOW
HEAT DISPLATED AT
A RATED PROPOTIONAL
TO MOTOR TEMPERATURE
Motor Heating
Motor Temperature
T = Tmax (1-e-t/ζ)
Tmax
Time
Rate of rise depend on motor thermal time constant ζ
or as temp rise α (Current)2
T = KI2max (1-e-t/ζ)
Motor Heating
I2
I22 T2
I12 T1
IR2 Tmax
Time
t2 t1
Motor Heating
Time
t1
Thermal Withstand
t2
Current
IR I1 I2
Motor Heating
Current2
Ieq2
Iθ2
I m2
Time
tTRIP
Iθ2- Im2= ( Ieq2- Im2)(1- e-t/ζ) Or alternatively
Rearrange this express in term of Time t = ζ ℓn {(K2 - a2)/(K2 - l2)}
t = ζ ℓn {(Ieq2 - Im2)/(Ieq2 - Iθ2)}
Motor Cooling
Cooling Equation :
Current2
Im I2m’ = I2me-t/ζr
Im’
Time
t
After time ‘t’ equivalent motor current is reduced from Im to Im’
Motor Heating
Temp
TRIP
Tmax
Time
t1 t2
t1 = Motor restart not possible
t2 = Motor restart possible
Cooling Time Constant ζr
Start/Stall Protection
Niwat Sriklam
Stalling Protection
Required for :-
Starting on start-up (Lock Rotor cold stall)
Stall during running (Hot stall)
With normal 3Ø supply :-
Istall = I locked Rotor ~ Istart
Cannot disthinguish between ‘STALL’ and ‘START’ by
current alone
Most case : tstart < t stall withstand
Sometimes : tstart > t stall withstand
Stall during Running Condition
Increase Load
Voltage drop or Dip
Lock Rotor Protection
Start Time < Stall Withstand Time
Where Staring Time is than Stall Withstand Time :
Use Thermal Protection Characteristic
Use Dedicated Locked rotor Protection
Stall Protection
T start < t stall : Use of Thermal Characteristic
Time
Insufficient margin between T start and T stall
Thermal Cold
Curve Cold Use of definite time Overcurrent relay :
Stall
Withstand Time
Start
Time + -
Thermal Hot O/C
Curve TD
Start TD
TD
Time 86
Full load Current
Current
TRIP
Full load I O/C Current
Current
Stall Protection
T start > t stall : Use of Tachoswitch and definite overcurrent relay time
Time
+ -
TACHO O/C
TD
Start
TD
Time 86
TD
TRIP
Full load I O/C Current
Current
Stall Protection
T start < t stall : Use of motor start contact and 2 stage definite overcurrent relay
Time
+ -
Cold Stall MSD
TD1+TD2 TD1
Start TD1 Hot Stall TD1 O/C
Time TD2
TD2
86
TD2
Full load I O/C Current
Current TRIP
MSD=Motor switching device
Motor Currents
Negative Sequence Current
Station field f
fr
Relative Frequency of stator field = f + fr
But fr = (1 - s)f
Therefore
(f + fr) = (2-s) f
Motor Positive and Negative
Sequence Impedances
Positive ½
(R1+ R’2 )2+j(X 1+X’2)2
R1 R’2
S j(X1+X’2) S ½
(R1+ R’2)2+j(X1+X’2)2
At standstill
Negative ½
(R1+ R’2 )2+j(X 1+X’2)2
R1 R’2
2-S j(X1+X’2) 2-S ½
2
(R1+ R’2) +j(X1+X’2)2
2 At normal
running
speed
Operation On Supply Unbalance
At normal running speed
Positive SEQ IMP ~ Starting Current .
Negative SEQ IMP Normal Running Current
Negative Sequence Impedance is much less than Positive
Sequence Impedance
Small unbalance = Relatively Large Negative Sequence current
Heating effect of Negative Sequence is greater than equivalent
Positive Sequence Current because they are Higher Frequency
Equivalent Motor Current
Heating from Negative Sequence Current Greater than Positive
Take this into account in thermal calculation
Ieq = (I12 + n I22)½
Where : n = Pos Seq Imp : Neg Seq Imp, [ 6 ]
Small amount of I2 gives large increase in
Ieq and hence calculated motor Thermal
state
Loss of 1 Phase while Starting
Star Normal Starting Current
IA = VAN/ Z
With 1 Phase open
I’A = VAB/ 2Z = √3 VAN/ 2Z
A = 0.866 x IA
SYMMETRICAL COMPONENT
Z I1 = ⅓( I’A + aI’B)
I1 = ⅓( 1 - a) I’B
Z |I1 | = ½ IA
I2 = ⅓( I’A + a2I’B)
Z
B I2 = ⅓( 1 - a2) I’A
C |I2 | = ½ IA
Loss of 1 Phase while Starting
Delta Normal
IA = √3 VAB/ Z
1 Phase open
I’A = VAB 3/2Z
A = 0.866 x Normal
Z Z
Z
C
B
1 Winding carries twice the current in the other 2
Single Phase Stalling Protection
Loss of phase on starting motor remains Stationary
Start current = 0.866 normal start I
Negative seq component = 0.5 normal start I
Clear condition using Negative Sequence Element.
Typical Setting = ⅓ I2
i.e. 1/6 Normal Starting current
Reverse Phase Sequence Starting
Protection required for LIFT motors , Conveyers
Instantaneous I2 unit
Time delayed thermal trip
Separate phase sequence detector for low load current
machines
Undervoltage Protection
Cause Low output torque
Machine cannot reach rated speed draws high stator current
Use time delayed undervoltage protection
Undervoltage Consideration
Reduced Torque
Increase Starting current
Reduced Speed
Failure To run-up
Form Of Undervoltage Condition
Slight but Prolonged (regulation)
Large transient Dip (Fault Clearance)
Undervoltage Protection
Disconnects motor from failure supply
Disconnects motor after Dip long enough to prevent successful
re-acceleration
Undervoltage Tripping
Mean of undervoltage tripping
AC holding coil for Fuse Contractor
Undervoltage release
Undervoltage relay for shunt trip
DEFINITE TIMP
INVERSE TIME
Consideration
U/V tripping should be delayed for essential motors so that
they may be given a chance to re-accelerate following a
short voltage dip (<0.5 s)
Delayed drop-out of fused contractor could be arranged by
using a capacitor in parallel with AC holding coil
Insulation Failure
Result of Prolonged or Cyclic Overheating
Instantaneous Earth Fault Protection
Instantaneous Overcurrent Protection
Differential Protection on some Large Machines
Stator Earth Fault Protection
R-stability
50
50
MOTOR MOTOR
a) Residually Connected CT’s b) Core Balance (Toroidal) CT
Short Circuit Protection
Due to the machine construction internal phase-phase faults are
almost impossible
Most phase-phase faults occur at the machine terminals or
occasionally in the cabling
Ideally the S/C protection should be set just above the max Istart
(I>> 1.25 Istart), however, there is an initial start current of up to
2.5 Istart which rapidly reduces over 3 cycles
Increase I>> or delay t>> in small increments according to
start conditions
Use special I>> characteristic
Instantaneous Earth Fault or Negative Seq.
Tripping is not permitted with Contactors
Fuse
50/51/49
MPR = Motor Protection
MPR
Ts
M 50/51G
Is Icon
Ts > Tfuse at Icont.
High Impedance Winding
Differential Protection
R Stabilizing
87 87 87 Relay
High Impedance Scheme
Note : Protection must be stable with starting current
Self Balance Winding Differential
Protection
A
87
87
87
Bearing Failure
Electrical Interferance
Induce voltage
Results in circulating currents
May fuse the bearing
Remember to take precaution – earting
Mechanical failure
Increase Friction
Loss of Lubrication
heating
Use of RTD
RTD sensors as known Stator Hotspotes
Absolute temperature measurements to bias the relay thermal
characteristics
Monitoring of Motor / Load baring temperatures
Ambient air temperature measurement
Synchronous Motors
Out of step protection
Inadequate field or excessive load can cause the machine to
fall out of step. This subjects the machine to overcurrent and
pulsating torque leading to stalling
Field current method
Detect AC current induced in field circuit.
Power factor method
Detect heavy current at low power factor
Loss of supply
On loss of supply motor should be disconnected if supply
could be restored automatically
Overvoltage & Under-frequency
Under-power & Reverse power
Power Factor Method
I
I’
Stator Current on
Loss Synchronism