IEEE TRANSACTIONS ON MAGNETICS, VOL. 44, NO. 12, DECEMBER 2008 4673
A New Pattern for Detecting Broken Rotor Bars in Induction Motors
During Start-Up
Jawad Faiz and Bashir-Mahdi Ebrahimi
Department of Electrical and Computer Engineering, School of Electrical and Computer Engineering, Center of Excellence on
Applied Electromagnetic Systems, University of Tehran, Tehran, Iran
This paper introduces a novel frequency pattern for diagnosis of broken rotor bars in induction motors during the start-up period.
This is important in the case of start-up of large induction motors with long starting time and also motors with frequent start-up. The
amplitude of the side-band components of the introduced frequency pattern is a suitable index for diagnosing the broken bars and de-
termining the number of faulty bars precisely during start-up. The paper investigates the performance of a faulty motor. Because the
number of broken rotor bars and the load are two major parameters affecting the performance of a faulty motor, the frequency spec-
trum of torque and speed in a motor with different numbers of broken rotor bars and different loads is analyzed. The time-stepping
finite-element method (TSFEM) is used to model the motor. This model takes into account the spatial distribution of the stator windings,
nonuniform magnetic permeance of the air gap, nonlinear characteristic of the cores, and continuous rotation of the rotor. The paper
compares simulation results in steady-state mode with experimental results and shows that the results agree well.
Index Terms—Broken rotor bars, induction motor fault diagnosis, starting transients, time-stepping-finite element method.
I. INTRODUCTION
S
QUIRREL-CAGE induction motors are widely used in
small and large industries, such as electric power stations,
oil refiners, and factories. Product lines will be stopped if
these motors fail to operate. In addition to the disturbance of
their operation, induction motor faults shorten their life-time.
Therefore, diagnosis of the faults is important from perfor-
mance improvement and longer life-time points of view. A
broken rotor bar is a common fault in induction motors. All
methods reported until 1987 have put limits on the type and
degree of fault, and there is no general and comprehensive
method for faults diagnosis (for different numbers of broken
bars and poles). Symmetrical components are among the first
applied methods for broken bar diagnosis [1]. In [2], the Norton
theorem has been used for analysis of broken rotor bars. It
shows that it is impossible to diagnose the disturbance due to
the fault in the rotor using torque-speed characteristic or stator
current. Therefore, a search coil has been suggested to do the
job. In [3], a double-cage induction motor has been analyzed
in steady-state mode for broken rotor bars assuming a current
passing the outer cage. However, there are considerable differ-
ences between the predicated and measured values which is due
to neglecting the saturation and inter-bar currents. Alternative
fault diagnosis methods are estimation and measurement of
the apparent resistance in broken rotor bars [4]; however, in
this method, variation of the rotor resistance with tempera-
ture must be taken into account. Variations of the rotor and
stator resistances have been taken into account offline, which
decreases the accuracy of the suggested method. In [5], the
presence of sidebands in specific harmonics on both sides of the
fundamental component of the flux in faulty machine has been
detected using a search coil. But this fault diagnosis method is
not usable for all types of machines with different structures.
Digital Object Identifier 10.1109/TMAG.2008.2002903
Color versions of one or more of the figures in this paper are available online
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Also, location of the detecting coil has a considerable effect
on the fault diagnosis. The relation between the magnetomotive
force (MMF) distribution of an induction motor and varieties
of broken rotor bars has been discussed in [6], but saturation
and influence of the spatial harmonics have not been taken into
account.
Magnetic field distribution in a healthy machine and a ma-
chine with five broken bars have been obtained by using the fi-
nite-element method (FEM), and a few search coils have been
then fixed inside and outside of the machine in order to diagnose
the broken rotor bars [7]. However, the broken bars current have
been assumed equal to zero, due to the presence of the inter-bar
currents which is not quite true.
It is shown in [8] and [9] that both the level of load and the
fault influence the stator current spectrum. If the stator current
is visualized in the synchronous reference frame, an existing
magnetic asymmetry influences both and components of
the current, while the load fluctuation affects only the com-
ponent. In [10], a simulation method has been presented based
on the rotating field theory for an induction motor with nonsinu-
soidal air gap flux distribution, in the presence of different load
types. However, this method is useful only for a particular type
of fault and nonideal operating conditions. In [11]–[13], appli-
cation of intelligent techniques has been proposed for diagnosis
of broken rotor bars. In [14] and [15], it has been assumed that
there are three symmetrical windings on the stator and loops
on the rotor, and with equation , steady-state analysis of
the motor has been carried out, and the presence of
components in the stator current and components in the
torque and speed have been shown. In [16], and compo-
nents have been calculated using Park’s transformation, and the
attempt has been made to diagnose the fault by comparing the
Park’s current patterns in the healthy and faulty motor. In [17],
the winding function method has been used to model the faulty
induction motor under broken rotor bars.
In Section II of the paper, the fault diagnosis algorithm is
introduced and its different parts are discussed. In Section III,
modeling of the motor with broken rotor bars using time-step-
ping finite-element method (TSFEM) is presented. The experi-
mental setup is described in Section IV and the basic principles
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