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A R T Ū R A S T A D Ž I J E V A S
S U M M A R Y O F D O C T O R A L D I S S E R T A T I O N
K a u n a s2 0 1 5
D Y N A M I C S A N D D I A G N O S T I C S O F
V E R T I C A L R O T O R S W I T H N O N L I N E A R
S U P P O R T S S T I F F N E S S
T E C H N O L O G I C A L S C I E N C E S , M E C H A N I C A L
E N G I N E E R I N G ( 0 9 T )
KAUNAS UNIVERSITY OF TECHNOLOGY
ARTŪRAS TADŽIJEVAS
DYNAMICS AND DIAGNOSTICS OF
VERTICAL ROTORS WITH NONLINEAR
SUPPORTS STIFFNESS
Summary of Doctoral Dissertation
Technological Sciences, Mechanical Engineering (09T)
2015, Kaunas
The doctoral dissertation was prepared in 2010-2014 at Kaunas University of
Technology, Faculty of Mechanical Engineering and Design, Department of
Mechanic Engineering. Research was supported by Research Council of
Lithuania.
Scientific supervisor:
Prof. Dr. Habil. Vytautas BARZDAITIS (Kaunas University of Technology,
Technological Sciences, Mechanical Engineering – 09T).
Dissertation Defence Board of Mechanical Engineering Science Field:
Prof. Dr. Rimvydas GAIDYS (Kaunas University of Technology,
Technological Sciences, Mechanical Engineering – 09T) – chairman;
Assoc. Prof. Dr. Giedrius JANUŠAS (Kaunas University of Technology,
Technological Sciences, Mechanical Engineering – 09T);
Assoc. Prof. Dr. Vytautas JŪRĖNAS (Kaunas University of Technology,
Technological Sciences, Mechanical Engineering – 09T)
Prof. Dr. Habil. Rimantas KAČIANAUSKAS (Vilnius Gediminas Technical
University, Technological Sciences, Mechanical Engineering – 09T);
Prof. Dr. Juozas PADGURSKAS (Aleksandras Stulginskis University,
Technological Sciences, Mechanical Engineering – 09T).
The official presentation of the dissertation will be held at 11 a.m. on June
19, 2015 at the public meeting of the Board of Mechanical Engineering
Science field in the Dissertation Defence Hall at the Central Building of
Kaunas University of Technology.
Address: K. Donelaičio st. 73 – 403, LT – 44029 Kaunas, Lithuania.
Phone: (370) 37 300042, fax. (370) 37 324144, e-mail: [email protected]
The Summary of Dissertation was sent on the 19th
of May, 2015.
The dissertation is available on the internet (http://ktu.edu) and at the library
of Kaunas University of Technology
(K. Donelaičio g. 20, Kaunas).
KAUNO TECHNOLOGIJOS UNIVERSITETAS
ARTŪRAS TADŽIJEVAS
VERTIKALIŲ ROTORIŲ, SU NETIESINIO
STANDŽIO ATRAMOMIS, DINAMIKA IR
DIAGNOSTIKA
Daktaro disertacija
Technologijos mokslai, mechanikos inžinerija (09T)
2015, Kaunas
Disertacija rengta 2010 – 2014 metais Kauno technologijos universitete,
Mechanikos inžinerijos ir dizaino fakultete, Mechanikos inžinerijos
katedroje. Moksinius tyrimu rėmė Lietuvos mokslo taryba.
Mokslinis vadovas:
prof. habil. dr. Vytautas BARZDAITIS (Kauno technologijos universitetas,
technologijos mokslai, mechanikos inžinerija – 09T).
Mechanikos inžinerijos mokslo krypties taryba:
Prof. dr. Rimvydas GAIDYS (Kauno technologijos universitetas,
technologijos mokslai, mechanikos inžinerija – 09T) - pirmininkas;
Doc, dr. Giedrius JANUŠAS (Kauno technologijos universitetas,
technologijos mokslai, mechanikos inžinerija – 09T);
Doc. dr.. Vytautas JŪRĖNAS (Kaunas University of Technology,
Technological Sciences, Mechanical Engineering – 09T);
Prof. habil. dr. Rimantas KAČIANAUSKAS (Vilniaus Gedimino technikos
universitetas, technologijos mokslai, mechanikos inžinerija – 09T);
Prof. Dr. Juozas PADGURSKAS (Aleksandro Stulginskio universitetas,
technologijos mokslai, mechanikos inžinerija – 09T).
Disertacija bus ginama viešame mechanikos inžinerijos mokslo krypties
tarybos posėdyje 2015 m. birželio 19 d. 11 val. Kauno technologijos
universiteto, centrinių rūmų, disertacijų gynimo salėje.
Adresas: K. Donelaičio g. 73 – 403, LT – 44029 Kaunas, Lietuva.
Tel. (370) 37 300042, faksas (370) 37 324144, el. paštas:
Disertacijos santrauka išsiųsta 2015 m. gegužės 19 d.
Disertaciją galima peržiūrėti internete (http://ktu.edu) ir Kauno technologijos
universiteto bibliotekoje
(K. Donelaičio g. 20, Kaunas).
INTRODUCTION
With the rapid development of technologies, new technological
processes are being created and old processes are being improved.
Rotating machinery plays a very important part in this. Most of the
technological processes, such as mechanical separation, grinding,
hydro energy production, are exclusively gravity-based technological
processes. Therefore, vertical rotor machinery is inevitably used in
industry, hydro power plants and maritime. When assessing the spread
of vertical vs. horizontal machinery among low to medium power
rotary equipment, horizontal rotor machinery makes up a significantly
larger proportion among the overall rotary machinery. However,
vertical rotor machinery is much more widely spread in industrial
areas, or in navigation, where technological processes are gravity-
based. Regulatory documentation, in relation to the rotor system
operation and diagnostics, mainly focuses on the horizontal rotors.
Vertical rotors in such documents are distinguished only in normative
documentation related to the large hydro turbines. In the material,
provided by the review of scientific publications, one can find
instances of scientists conducting research with vertical rotors, when
there is a need to avoid gravitation effects on the rotary system in
radial direction, for instance, when the object of study is the influence
of support anisotropy on the dynamics of the rotor system. In other
instances, research is conducted with horizontal rotor systems.
In analyzing the most common rotor system faults, according to
their frequency, one can distinguish that the most prevalent fault of
rotor systems is the imbalance, followed by the coupled rotor shaft
axis misalignment. The third most common fault is the rotor support
bearing defect. Shaft axis misalignment is found more frequently in
horizontal rotor systems, because the rotor drive unit and the work
unit may be mounted on different foundations and, eventually, the
weight of the system may deform the foundation. Vertical rotors have
common foundations and axis misalignment is a less prevalent defect
6
of the vertical rotor system, therefore, in this study, it has not been
analyzed in greater detail.
Topicality of the problem
In everyday life, people are surrounded by a number of
household appliances, many of which work based on some kind of
rotating parts. It is easy to notice that most of the household
appliances and devices used domestically, function on some part with
the help of some kind of mechanism with horizontal axis rotor.
However, even domestically, there are numerous areas, where it is
necessary that the rotor of the household appliance be vertically
oriented, otherwise, we could not be capable of performing certain
processes. These are particular technological processes that are
gravity-based. There are many household appliances that cannot
function without the help of the gravity, although, without going into
much detail, one would not say,that they would have to be particularly
with vertical rotors. Examples of such appliances would be:
separators, various household cutting equipment, grinders (household
grater), whisks, mixing equipment, juice extractors etc. Much of the
above mentioned household equipment would not operate with
horizontally oriented rotation axis, however, when using them, we do
not realize, that these processes are influenced by gravity.
In industry, maritime and energetic, as well as in households,
equipment with horizontally oriented rotation axis is more
widespread. Much of the fundamental scientific research, as well as
regulatory documentation for evaluation of technical condition and
monitoring are dedicated to this kind of machinery. Although, there
are many areas, where systems with vertically oriented rotation axis
must be used. Otherwise, technological processes, production of
energy or technological supply are impossible. Such equipment has
some certain specific features that are not fully described nor in
scientific works, nor in regulatory documentation. Devices of this kind
differ from the horizontally oriented ones in that their rotors are not
stabilized by the gravity (the weight of the rotor in radial direction).
Therefore, they are much more sensitive to radial loads in dynamic
stability sense. In addition, their foundation has significantly lower
stiffness in the upper part of the rotor, because they are not mounted
on some massive base, but rather attached to some certain prepared
construction, the stiffness of which, as compared to the stiffness of the
system mounted on the massive base, is significantly lower. These
factors complicate the assessment and monitoring of such equipment
conditions therefore, service personnel with huge experience in
technical condition assessment of such rotor machinery are required.
The major differences between the vertical and horizontal rotor
systems can be found out through examining the dynamic forces
acting on rotor supports in greater detail. If analyzing horizontal rotary
systems, a plane perpendicular to the axis of rotation of the rotor is
sufficient to define the operation of forces acting on the support, then,
assessing forces, acting on the vertical rotor supports, it is necessary to
define spatial forces, because as the rotation speed of the rotor
changes, so does the radial component of the overall dynamic force.
When speaking of support-mounted roller bearing defects, we
have to signify that the great majority of the defects in horizontal rotor
systems form at the most loaded part of the bearing. Meanwhile in
vertical rotor systems with changing operating mode, it is very
difficult to distinguish, which part of the rotor system is going to be
loaded most, i.e., whether the radial forces outweigh the gravity, and
how the load direction changes etc.
The objective of this work is to quantifiably assess and find
similarities and differences in the evaluation of technical conditions of
vertical and horizontal rotor systems and to present it in quantitative
manner, easily perceivable to the experts of this field.
Aim and tasks for the thesis
The aim of this work was to investigate and quantifiably assess
the dynamics of vertical rotor, rotating in the non-linear stiffness
supports and establish its correlation to diagnostic of defects of
vertical rotor elements.
8
These tasks were formed in order to achieve the objective of
this work:
1. To analyze scientific works published in periodic scientific
journals and international standards where the rotor dynamics are
examined in practice and theory, also to examine scientific works
published in periodic scientific journals, elaborating on the existing
and novel methods of defect diagnostic research for rotors with roller
bearings.
2. To conclude an analytical model to calculate forces, acting on
vertical rotor supports, as well as to calculate the forces acting on the
radial axial load of the vertical rotor.
3. To develop a generalized vertical rotor model, that can evaluate the
effect of the gyroscope, gravity and its spatial direction and which
could allow to theoretically determine the radial – axial forces acting
on the vertical rotor support as well as to research the rotor dynamics
phenomena.
4. To perform the comparative diagnostic research on the defects of
vertical and horizontal rotor roller bearings and quantifiably assessing
the differences in diagnostic research on defects among the two
systems.
5. To perform the diagnostic investigation of vertical rotor system
with inner rolling bearing ring race defect at different rotor imbalance
excitation force and inner ring defect angular positions.
6. To perform diagnostic research on vertical rotors with outer rolling
bearing ring race defect, while changing the tilt angle of the rotor
rotation axis from the vertical, also to determine how the dynamics of
the rotor shifts with the change of the tilt angle, to examine, how it
affects the results of the diagnostic.
Scientific novelty
Analytical model has been constructed, allowing assessing
forces acting on radial-axial supports of the vertical rotors.
A generalized theoretical model of the vertical rotor has been
designed, capable of evaluating the effect of the gyroscope, gravity
and its spatial direction, the non-linearity of the rotor supports as well
as the radial and axial gaps in the supports.
The major differences in vertical and horizontal rotor
diagnostics have been determined and quantifiably evaluated through
scientific research.
With the help of a generalized theoretical model of vertical
rotor, it has been determined, how the dynamics of the vertical rotor
shifts, when rotor sways from the vertical at an angle of up to 15˚.
Experimental studies have shown how this affects the results of the
rotor’s diagnostic research.
Practical value
The results of the research have been applied in conducting
diagnostic studies of vertical rotor equipment at „DFDS Seaways“
ferries “Vilnius Seaways“, „Optima Seaways“, „Victoria Seaways“
and „Athena Seaways“. The results of these studies have been
approbated at such industrial enterprises as PLLC “„Lifosa“, PLLC
„Nordic Sugar“, “JSC „Arvi fertis“ and others. PLLC “Lifosa” has
been advised on the renewal and the selection of new vertical pumps
for the sulfuric acid.
A universal model of the vertical rotor has been created, with
the consideration on the gravity and its spatial direction. Because of its
versatility, this rotor system model can be applied for the research on
the dynamics of both vertical and horizontal rotors.
Statements for defense
1. The analytical model of radial - axial forces acting on rotor
supports, allows for determining the magnitude and the spatial
position of overall forces F acting on radial - axial supports of the
vertical rotor.
2. In order to examine the dynamics of rotor systems, a generalized
model of the vertical rotor system, capable of evaluating the gravity
and its spatial direction, could be applied both to vertical as well as
horizontal rotor systems with nonlinear stiffness of supports.
10
3. A new created relative parameter – Defect Visibility Ratio (DVR)
allows to quantifiably assessing and compare the diagnostic research
features both for the horizontal as well as vertical rotors. It also
facilitates for the machine technical condition monitoring as well as
defect diagnostic research in situ.
The work approbation
6 (six) scientific articles were published on this topic (4 ISI
Web of Science with a citation index, and 2 other peer - reviewed
scientific journals) as well as presentations at in 9th scientific
conferences:
1. „MSM 2011“, topic of presentation: „Modeling and diagnostic of
rotary system powered by multi gear“.
2. „Mechanics 2012“, topic of presentation: „Comparison of Vertical
and Horizontal Rotor System Models and Simulation Results".
3. „Vibroengineering 2012“, topic of presentation: „Features of
Vertical Axis Rotor with Rolling Bearings Diagnostics".
4. „Scientific work on technology in western Lithuania 2012“, topic
of presentation: „Research on vertical rotor dynamics“.
5. „Mechanics 2013“, topic of presentation: "Vertical Versus
Horizontal Rotors Vibration and Diagnostics"
6. „ICOVP-2013“, Lisbon, topic of presentation: "Vertical Versus
Horizontal Rotors Dynamics and Diagnostics"
7. „Vibroengineering 2013“, topic of presentation “Influence of
imbalance phase angle to vertical and horizontal rotors bearings
diagnostics“.
8. „Mechanics 2014“, topic of presentation: „New deep groove ball
bearings high frequencies vibration testing“.
9. „Marine science and technology 2014“, topic of presentation:
„The specifics of vertical rotor machinery testing in marine
technology“
The structure of the work
Doctoral thesis consists of an introduction, four chapters,
general conclusions, references, list of author publications and
appendixes. The total scope of the dissertation of 142 pages, they
contain 107 pictures, 91 bibliographic references are used.
1 ROTOR DYNAMICS AND DIAGNOSTICS
1.1 REVIEW OF ROTOR DYNAMICS
The dynamics of rotors, as a science, started from W.J.M. Rankine
and his mathematical model of rotor that he published in 1869 year.
This model was dedicated to calculate the first critical rotational speed
of rotor. To determine the critical rotational speed of rotor, he choose
a model with two degrees of freedom, that consists of point mass that
is fixed onto stiffness element and another end of stiffness element is
fixed. All mentioned components rotate about fixed node of stiffness
element. In 1883 engineer from Sweden K.G.P. de Laval created the
first impulse turbine, which reached rotational speed of 40 000 RPM.
He derived a relationship, through which it was possible to determine
the centrifugal forces, which affect whirling motion of shaft, he also
found the self-centering phenomenon of rotors. The first
comprehensive model of rotor was created by a professor of Munich
University, August Föppl in 1885 year. A. Föppl was the first to
explain the self-centering phenomenon, investigated by de Leval, in
detail [1]. Theoretical model of A. Föppl has allowed establishing a
stable supercritical rotational speed and theoretically opened a rotor
work opportunity at supercritical rotational speed. This model has
been ignored by investigators, because in practice, it seldom allowed
to get a stable supercritical rotation speed [2]. Later, in 1919, the
Royal Society of London, commissioned an independent research of
the Irish Royal College professor Henry Jeffcott to improve a model
of August Föppl and solve the disagreements between theoretical
model and experiments. The subsequent, very important step in the
history of rotor dynamics was made in 1924 by A.Stodola. A.Stodola
12
proved in his works, that there is a second (not only one) critical speed
of rotors. During analysis of gas and steam turbines, A.Stodola
noticed, that the disc, mounted on the rotating shaft, changes the
dynamics of rotor. And that depends on the inertia moment of disk,
mounted on the rotor. This way, the damping component of
gyroscopic effect appears in mathematical expressions of rotor
dynamics. In 1924 A.Stodola published a book, in which the
phenomenon of second resonance has been described in detail. In this
book he also describes a static rotor balancing methods, approximate
calculation of critical speeds (eigenvalues) of stepped rotors and etc.
in detail. The fundamentals published in Föppl, Jeffcott and Rankine
works are also relevant today. They placed grounds of rotor dynamics
which was the basis for Campbell’s diagram of rotor critical speeds
diagram, which is often referred as the rotor critical speeds map [3].
The Vertical rotors are particularly suitable for investigations of
nonlinearity of supports. There is a couple of works where the
nonlinearity of supports investigated by analyzing a whirling motion
of rotors with different non-linearity of rotor supports. These studies
are described in works of worldwide recognized investigators of the
rotor dynamics [4]. Some authors uses the vertical rotors to create new
or to develop existing models to better describe the kinematic
movement of shaft neck in supports, but those models rarely takes a
greater theoretical or practical value, as they often are very
complicated or needs a complex mathematical ability or describe the
motion of rotor accurately only under certain conditions consolidation
[5]. During the analysis of scientific periodical publications we can
observe a one or other work that are dedicated to investigate the
dynamics of vertical rotors using finite element method. Some authors
investigated the dynamics of vertically oriented rotating discs [6].
Other authors use the vertical rotors to investigate an accuracy of
finite element solvers by comparing the results of eigenvalues of
vertical rotor to experimental results [7]. By increasing the popularity
of FEM (that are induced by development of semiconductor
technologies and FEM software development) investigations and
capabilities of complex multi stage gas turbines can be examined.
There is a few works published in this field of investigations [8]. In
periodic scientific publications, we can find authors that investigates
the multi rotational rotors of jet engines by using FEM software
ANSYS. The multi rotational speeds rotors of jet engines consists of
two gas turbines, the first and main rotor rotates fixed in supports of
motor second rotor rotates mounted using the hydrodynamic bearings
on first rotor shaft [9]. We also can find a recently defended PhD
thesis dedicated to investigate the dynamics of vertical rotors. Some
works are dedicated to parametric optimization of large rotors work
conditions to prevent an undesirable working mode of rotor [10].
Other works dedicated to theoretical investigations of rotors using
FEM [11].
1.2 REVIEW OF DIAGNOSTICS OF ROTORS
The diagnostics of rotor systems is an integral part of modern
rotor systems commissioning process. Therefore, it is necessary to
mention the possible rotor diagnostic techniques and explore some of
the reasons for their popularity and development trends in
contemporary science works. The vibration diagnostics of rotor
systems is one of several stages of technical condition assessment,
which is primarily used for, the evaluation of technical condition of
rotating machinery. The main aspects of the use of this method are
described in detail in the international standard ISO 13373-1: 2002
Condition monitoring and diagnostics of machines - Vibration
condition monitoring - Part 1: General Procedures" [12], processing
and analysis of measured vibration data are described in detail in
international standards ISO 13373-2: 2005 "Condition monitoring and
diagnostics of machines - Vibration condition monitoring - Part 2:
Processing, analysis and presentation of vibration data" [14] and ISO
13379: 2003, "Condition monitoring and diagnostics of machines -
General Guidelines on Interpretation date and diagnostics techniques
[13]. The main requirements of vibration measurement and
monitoring equipment are described in detail in the international
14
standard ISO 2954: 2012 "Mechanical vibration of rotating and
reciprocating machinery - Requirements for instruments for measuring
vibration severity" [15]. The relative vibration measurement,
evaluation of the rotor shaft neck vibrations in supports, described in
relation to an international standard, which consists of 5 - the essential
parts of this [16 – 20]. The standard describes in detail the vibration
measurements and interpretation of measurement data by measuring
the vibrations of rotor systems on non-rotating parts, consists of six
parts [21 – 26].
The traditional rotor diagnostic methods are in detail described
in practical tutorials and international standards. We should try to
identify some of them: the vibration signal spectral analysis method;
whirling motion analysis method; vibration shape factor method,
envelope method; acoustic emission method; shock pulse method and
etc. All of those methods are used in rotor vibration monitoring and
diagnostics for more then 10 - 20 years. But there is no relation
between those methods and influence of rotor dynamics to diagnostics
using mentioned traditional methods. This work is an attempt to find
trends of vertical axis rotor dynamics and it’s relation to diagnostics of
those rotors.
Among the developed new diagnostic research methods are
increasingly visible a diagnostic methods based on artificial neural
networks and the use of a hybrid, combining several diagnostic
methods together to increase the precision [27 – 28]. During the
analysis of scientific publications we can find the research works that
are dedicated to develop of a new analysis methods for spectrum or
spectrum cascades [29, 30]. The significant steps to rolling bearings
diagnostics with all kinds of defects were made by R.B. Randall with
colleagues and other well known researchers [31, 32], but all of these
works are concentrated to identify a bearing element fault indications
in different formats of data, but not related with the rotor dynamics.
We also can find some scientific publications dedicated to investigate
rolling bearings wearing problems, one of the most frequent topics -
growth of a radial fault of bearing [33, 34]. Among the new,
developed methods of rotor diagnostic, many of them based on the
new signal processing capabilities. Many of them showing good
results during investigations on testing rigs in laboratories but in
practice are hardly applicable. Many of them have a limited usage and
need of expensive research equipment.
2 THEORETICAL INVESTIGATION OF GENERALIZED
VERTICAL ROTOR MODEL
2.1 FORCES ACTING IN ROTOR SYSTEM
Mechanical vibrations are an integral environment of dynamic
systems, which, often, interpreting vibration data in a right way can
provide a lot of information about the observed system. In order to
properly assess technical monitoring of the condition of the rotor
system, it is necessary to know that some of the effects of rotor
dynamics help in stabilizing the system, but there are cases, where
summative these effects can get the opposite phenomenon -
spontaneous destabilization. In order to analyze forces acting at
supports of rotors in deep, we need to examine the main components
of summary dynamic forces in detail. There are two cases of analysis.
The first one is to analyze the acting forces in orthogonal system; a
second is to analyze acting forces in spatial system. We can see that
when we are talking about a horizontally oriented rotor, the planar
formulation of acting dynamic forces is sufficient. However, when we
talk about vertically oriented rotor system, a spatial formulation of
task is necessary, because the force of rotor weight acts in axial
direction of rotor, while the dynamic force of imbalance, which
depends from rotational speed, acts in direction that is perpendicular
to axis of rotation. It was accepted, that two acting forces exist in
orthogonal planes in vertical axis rotors: eccentric inertia force,
induced by imbalance u, acting perpendicular to rotation axis and
second – axial force as gravity force Fmg of rotor‘s mass m acting
parallel to vertical axis. In Fig.1 we see, that the total dynamic force Fs
depends on centrifugal dynamic force of imbalance and when the
16
rotational force increases, not only the magnitude of total force is
changing, the angle between rotation axis and total force also change
Fig. 1 Scheme of the forces acting in the vertical rotating rotors with
imbalance
The magnitude of total force can be calculated using mathematical
expression (2.1.).
22
cmgs FFF (2.1.)
Where: Fs – total dynamic force, N; Fmg – gravity force, N; Fc –
dynamic force of imbalance, N.
The angle between rotation axis of rotor and total dynamic force
can be calculated using mathematical expression (2.2.)
;c
mg
F
Farctg (2.2.)
We see, that if the position of rolling bearing fault is placed in
the wrong direction on the bearing ring race (the dynamic force acting
a fault indirectly), we could not see the indications of fault during the
diagnostics of such rotor. There is a lot of vertical axis equipment in
ships and diagnostics of such equipment in this environment plays an
important role. During movement, the ship makes a pitching (we
didn't analyze pitching motion types; there is six basic pitching motion
types). If the ship makes pitching, the axis of equipment with vertical
axis of rotation is tilted from vertical position; there is no data about
diagnostics of vertical rotors that are tilted from vertical. We need to
analyze how the dynamic forces affect supports (in what direction and
how it affects the magnitude), when the rotor is tilted from vertical. In
Fig.2, the forces, acting supports, when the axis of rotation of rotor is
tilted from vertical, is presented. In fig. 2 we see that the total force Fs
is not of the same direction and magnitude in different sides of rotor
support. If we have an oscillating total force, we know that it affects
and axial force.
Fig. 2 Scheme of the forces acting vertical rotors with imbalance,
when the rotation axis tilted from vertical
The total force in the side where rotor is tilted can be calculated
using (2.3.) mathematical expression. In the opposite side, it can be
calculated using (2.4.).
sin222
1 mgcmgcs FFFFF (2.3.)
sin222
2 mgcmgcs FFFFF (2.4.)
18
Then the amplitude of total force can be calculated using (2.5.).
sin
2
sin2sin2 2222
mgc
mgcmgcmgcmgc
s
FF
FFFFFFFFF
(2.5.)
And the amplitude of axial force is given in (2.6.) mathematical
expression.
cosmgmgas FFF (2.6.)
The amplitude of centrifugal force given in mathematical
expression (2.7.).
2sin)sin()sin( mgmgcmgcc FFFFFF (2.7.)
These varied axial and radial forces make rotor‘s and bearings
condition monitoring and failure diagnostic procedure complicated.
Modeling of vertical axis rotors and simulating forces acting on
bearings makes failure diagnostics procedure more adaptive for
practical usage.
2.2 FE MODEL OF VERTICAL AXIS ROTOR
Modeling and simulation of vertical axis rotor provided with
FEM and ANSYS software [35]. The designed physical model of
vertical rotor is shown in Fig. 3. and model designed with FEM in Fig.
4. The rotor total mass 2,80 kg, shaft length is 0,6 m, diameter 0,02 m,
wheel diameter 0,15 m with radius ru=0,06 m for the fixing imbalance
masses, two stiffness elements in radial direction of 1st (upper)
bearing and three stiffness elements - two in radial direction and one
in axial direction - of the 2nd
(lower) bearing.
Fig. 3 Physical model of vertical rotor elements
The FEM beam type BEAM188 10 elements used for modeling
shaft of the rotor. The beam type BEAM188 3 elements used for the
wheel with unbalance mass modeling by element MASS21. For
nonlinear bearings stiffness elements the COMBIN39 element and for
stiffness-damping linear bearing elements the COMBIN14 element
was used. The image of elements of FE model given in Fig.4.
Fig. 4 Visualized elements of FE model
The bearings nonlinear stiffness elements Kxi, Kyi and Kz2
parameters for COMBIN39 elements experimentally measured with
testing machine Zwick/Roell Z100 (Germany) in axial and radial
directions. Simulations of FEM model were provided in series: with
20
static analysis evaluating constant forces; frequency analysis for
determining resonance frequencies; harmonic analysis and transient
dynamics analysis axis symmetrical problem and axis asymmetrical
problem solving. There were used such mathematical models: Static
analysis model (2.8.).
}{}{ FuK (2.8.)
Modal analysis is using such mathematical expression for
determination of eigenvalues of rotor (2.9.).
0}]{[ 2 uMK (2.9.)
Harmonic response analysis can be implemented using (2.10.)
mathematical expression.
},,{}{}{}{ tuuFuKuCCuM gyr (2.10.)
Where the real and imaginary parts of centrifugal force can be
defined in such way (2.11., 2.12.).
tj
ccx eFtFF cos (2.11.)
tj
cccy ejFtFtFF )2/cos(sin (2.12.)
2.3 THE RESULTS OF THEORETICAL INVESTIGATIONS
In this part of this work attention is focused to the unique
features of diagnostics of vertical rotor with rolling bearings.
Therefore, the simulation is performed using the experimental tests
measured stiffness values, which measured in radial and axial
directions on rolling bearing and the experimentally measured radial
and axial gaps of rolling bearings. The simulation results presented in
Fig. 5 and Fig. 6 as vertical axis tilt angle γ influences on dynamics of
Fs and position angle φ. The simulation provided when variable
vertical axis tilt angle γ values change in discreet steps 5º, 10 º, 13,5º
degrees. The absolute value of Fs varies in wide range from 168 N up
to 203 N with increasing tilt angle γ, Fig. 5 and inflated with
increasing rotor’s imbalance. According to simulation results the
absolute value of dynamic force Fs and angular position of force φ
increases nonlinearly with increasing rotational speed n, imbalance u
and rotors axis tilting angle γ.
Fig. 5 The 2nd bearing’s dynamic forces Fs (n, γ) plots versus rotor’s
rotational speed and tilt angle γ with imbalance of 120 gmm
Fig. 6 The 2
nd bearing’s dynamic forces Fs position angles φ plots versus
rotational velocity of rotor and tilt angle γ (5º, 10 º and 13,5 º) with imbalance
of 120 gmm
It happens, that up to first resonance frequency ωR = 204 1/s the
dynamic force Fs position angle φ decreases and becomes φ = 0º
22
value, Fig. 5 and Fig. 6. Further increasing the angular velocity from
ωR=204 1/s, the Fs position angle φ increases nonlinearly. For
example, when ω = 314 1/s, imbalance uL=80,4 gmm the simulated
position angle is φ = 22º and when angular velocity is high ω = 559
1/s imbalance uL=80,4 gmm the position angle increased up to φ=77º.
At resonance at angular speed of ωR= 204 1/s kinetic orbit drastically
changes in magnitude and angle in comparison with ωL= 100 1/s and
ωH= 314 1/s angular velocities, Fig.7. These results indicated that
failures diagnostics indications of vertical axis rotors are too different
in comparison with the horizontal axis rotors. ωL= 100 1/s and ωH=
314 1/s angular velocities, Fig.7. These results indicated that failures
diagnostics indications of vertical axis rotors are too different in
comparison with the horizontal axis rotors.
a) b)
c)
Fig. 7 Kinetic orbits of vertical rotor shaft neck when rotor tilted
13,5˚ from vertical: a) n = 1000 RPM; b) nc = 1950 RPM; c) n = 2
850 RPM;
3 EXPERIMENTAL INVESTIGATIONS
3.1 COMPARATIVE INVESTIGATION BETWEEN VERTICAL AND
HORIZONTAL ROTOR DIAGNOSTICS
In this section of the work, author's research using original
testing stand is presented. This subpart is dedicated to compare the
indications of diagnostics of same rolling bearings with same faults of
vertically and horizontally oriented rotor. The objective of this section
is to identify the essential differences of the horizontal vs. vertical
rotary system fault indications, during diagnostic tests, to determine
the quantitative and qualitative differences between them. To establish
quantitative relationships as vertical rotary equipment defects
diagnostic tests and correlate with the results of rotor parameters
describing the dynamics of systems. The experimental test stand,
shown in Fig. 8 has been set up in order to investigate differences of
diagnostic features during tests with damaged 6004 single row deep
groove ball and new bearings in horizontal and vertical axis rotors.
The rotor is driven by a variable - speed AC motor controlled by
frequency inverter. Rotational speed during, measurement has been
ramped up from 100 to 3050 RPM.
Fig. 8 Rotor researches stand. 1 – AC motor; 2 – Coupling; 3 –
20 mm diameter shaft; 4 – Supports with rolling bearings.
The rotor bearing supports 1 and 2 were (Fig. 9) positioned in a
= 50 mm, a + b = 550 mm distances from flywheel disc. During a tests
24
rotation axis of the rotor has been switched from horizontal to vertical
position. At first, the brand new 2nd
ball bearing was examined, then,
it has been replaced with the faulted bearing.
Fig. 9 Orientation of rotational axis and positions of
accelerometers
Separate tests were provided: the first one with artificial defect
on the inner ring race and second - with artificial defect on the outer
ring race, as shown in Fig.10.
a) b)
Fig. 10 Defects of the deep groove ball bearing 6204: a - inner
ring race fault; b - outer ring race fault;
Tests were carried out with imbalance of 80 gmm (maximum
permissible imbalance according to ISO 1940-1 is 125 gmm) and with
determined residual imbalance of 240 gmm as found in balancing
quality grade G6.3 (ISO 1940-1). The balancing mass was attached to
the rotor flywheel disc at radius ru. The absolute vibration velocity of
bearing supports has been measured with four accelerometers 1x, 1y
and 2x, 2y mounted in two perpendicular directions at each bearing
support. Experimental data has been processed using multi-channel
vibration signal analyzer "OROS".
The order of test, during the experimental investigations, given
in Table 1.
Table 1. The vibration measurements order
No. Orientation of
rotor axis Imbalance
Rolling bearing
defects
1. Horizontal 80 g∙mm Without
Vertical
2. Horizontal 240 g∙mm Without
Vertical
3. Horizontal 80 g∙mm Inner ring race defect
Vertical
4. Horizontal 240 g∙mm Inner ring race defect
Vertical
5. Horizontal 80 g∙mm Outer ring race defect
Vertical
6. Horizontal 240 g∙mm Outer ring race defect
Vertical
Initial condition of bearing fault position, fixing in supports, given in
Fig. 11.
a) b)
Fig. 11 Initial conditions of measurements: a) position of inner
ring race defect; b) position of outer ring race defect
26
The absolute vibration data of the rotor bearing supports was
evaluated as root mean square values vRMS and vibration velocity
spectrum and cascade diagrams. The 2nd
bearing was under
investigation. The first test was performed with the brand new 2nd
bearing and another, second and third test has been carried out with
the faulty 2nd
bearing. The 1st bearing was brand new throughout the
entire experiment.
The 2nd
bearing support vibration measurement data plotted in
vibration velocity spectral cascade diagrams (Fig. 12 and Fig. 13)
shows that the 1X frequency vibration magnitudes dominated in
horizontal axis rotor at run up mode at wide rotational speed range
(1000-3050 r/min).
a) b)
Fig. 12 Vibration velocity vRMS cascade plots of 2nd
new 6004
bearing, measured with 2ya accelerometer, at run up mode of the rotor
240 gmm unbalance: a – horizontal axis rotor; b – vertical axis rotor.
The vertical axis of rotor with the new bearing generates 1X, 2X,
3X harmonics at wide rotational speed range and indicated existence
of radial gaps as nonlinearities (Fig. 12 b). Therefore, it is difficult to
diagnose imbalance in this systems. The vertical rotor with faulty
bearing generates 1X, 2X,…, 7X frequencies vibration harmonics
from 1500 RPM (Fig. 13 b). It shows us that it is difficult to diagnose
the imbalance in the rotor with significant defect in bearing. The
nonlinearities of radial gaps in the bearings dominated without acting
gravity force as shock form.
a) b)
Fig. 13 Vibration velocity vRMS cascade plots of 2nd
faulty bearing
6204 with outer ring race fault, measured with 2ya accelerometer, at
run up mode of the rotor with 240 g·mm imbalance: a – horizontal axis
rotor, b – vertical axis rotor
The physical effect stated that the rotor’s gravity force augments
vibrations velocity vRMS values in horizontally oriented rotor, although
the anisotropy of supports is significantly noticeable and stiffness of
supports in y - direction is higher than in x – direction. “Defect
visibility ratio (DVR)” parameter was designed for the quantitative
evaluation of the dynamics features of the vertical and horizontal
rotors with deep grove ball bearings.
XRMS
DEFRMS
v
vDVR
1
._ (3.1)
Where: ._ DEFRMSv – dominant defect nX harmonic vibration
velocity vRMS value, mm/s;
XRMSv1
– 1X frequency vibration velocity vRMS value,
mm/s;
As shown in table 2, the damaged bearings with defects of inner
and outer rings races, kinematic vibration frequencies were simulated.
Constant rotational speed of inner ring ni = 3050 RPM and outer ring
was fixed: ball diameter dr = 6,35 mm, number of balls 9.
The statistical data of dominating faulty bearing vibration velocity
vRMS level value divided by 1X (synchronous frequency) harmonic
vibration velocity vRMS level values was presented in Fig.14, Fig.15
DVR diagrams. The graphs shows that, in some cases, when the rotor
oriented vertically the bearing fault frequency vibration velocity vRMS
28
level is very low compared with 1X harmonic vibration velocity vRMS
level. It's very complicates such rotors bearing diagnostics.
Table 2. Kinematic vibration frequencies with stationary outer ring for the
bearing 6004
Constant rotation speed of inner ring, ni=3050 RPM=
=50,83 Hz and outer ring ne= 0 RPM
Typical
vibration
frequencies,
Hz
Rotational frequency of rolling element cage, fc 20,2
Vibration caused by radial fault of the rolling
element, with consideration to its impacts only
against the inner or only against the outer ring, fr1
[Hz]
119
The passage of rolling elements over defect in the
rotating inner ring, fip 276
The passage of rolling elements over defect in the
stationary outer ring, fep 182
Vibration caused by radial fault of the rolling
element, with consideration to its impacts against the
inner and outer rings, frp [Hz]
238
Fig. 14 Horizontally and vertically oriented rotors “Defect
Visibility Ratio” calculated form 2x accelerometer measurements data
The vibration velocity vRMS cascades, which presented in Fig. 12,
Fig.13 shows that in some cases measured vibrations of the vertical
rotor vRMS level has a lot of vibrations “noise” around the bearing
defect frequency. It very complicates such rotor bearing diagnostics,
because those vibrations can be awaking by work chain rubbing, shaft
alignment, coupling defect and etc.
Fig. 15 Horizontally and vertically oriented rotors “Defect
Visibility Ratio” calculated form 2y accelerometer measurements data
The measuring data of vibration velocities vRMS of the first
support (the second plane data) allows as only a partial determination
of a second support bearing fault. When rolling bearing with inner
ring race fault where mounted on 2nd
support, in second plane (1st
support plane) kinematic bearing fault frequency harmonics cannot be
detected. However when bearing with outer ring race fault where
mounted on 2nd
support, the accelerometers mounted on 1st support
(second plane accelerometers) captures relatively high level of the
outer ring race defect frequency 2x and 3x harmonics.
Conclusions of subchapter:
1. Vibration velocity spectrums of the vertical rotor are rich of
higher level vibrations in higher frequencies in comparison with
horizontal axis rotors. This can able to happen due to the chaotic
vertical rotor movement kinematics in radial bearing clearance.
2. Vibration intensity of horizontal axis rotor is higher in
comparison with vertical axis rotor in y-direction. Due to gravitational
influence to horizontal rotor in radial y-direction. Horizontal rotation
axis rotor is more sensitive to imbalance that generates high level 1X
30
frequency vibration amplitudes in comparison with vertical axis rotors
that is more sensitive to the values of radial gaps in the bearings.
3. The designed DVR values provide quantitative evaluation of
horizontal and vertical rotors vibration ratio levels which enables
determination how many times the defect frequency band vibration
level is less than the first harmonic vibration level. It quantifies the
complexity of the defect diagnosis.
3.2 INFLUENCE OF DYNAMIC FORCE ANGULAR POSITION TO
VERTICAL AND HORIZONTAL ROTORS ROLLING
BEARINGS FAULTS DIAGNOSTICS
Instead of using the traditional periodic planned assessment of
technical condition, monitoring systems, based on acceleration
transducers to measure and supervise mechanical vibrations often has
been used for diagnostics of modern technological machinery.
Although, sometimes it is difficult to identify rolling bearing faults,
even if constantly monitoring and analyzing the machinery vibration
acceleration or vibration velocity FFT spectra or their cascades. We
usually run into such problems when analyzing gravity based
technological processes (separators, diffusion machinery) in vertical
machinery observations. This is because the angular position of
imbalance mass varies often in this type of machinery, which causes
the inner ring race fault in the bearing. This subchapter of this work is
a comparative experimental research data between the vertical and
horizontal axis rotors. The test stand consists of the disk mounted onto
the end of the shaft; the deep groove rolling bearing 6004/C3 with
inner ring race defect is mounted behind the support. Throughout the
investigation tests, the angular position of dynamic force of imbalance
mass and inner ring race local fault is switched from 0° to 360
°, using
a 450 angular step value. The experimental studies are carried out both
with rotor axis oriented vertically and horizontally. In order to
simplify the data being analyzed and to quantifiably assess the
diagnostic experiments of vertical and horizontal rotor defects,
statistical processing parameter called “Defect Visibility Ratio”
(DVR) has being designed. Through the use of this statistical
parameter, the defect-identification capabilities of rotor with bearing
with inner ring race fault can be determined quantifiably.
Fig. 16 The experimental test stand. 1 – AC motor; 2 –
Coupling; 3 – Supports with rolling bearings; 4 – 20 mm diameter
shaft; 5 – Flywheel disc.
The experimental test stand, shown in Fig. 16, consists of rigid
frame and fixing plate on which the rotor system is mounted. The
rotor system consist of: asynchronous electric motor with current
frequency inverter 1, elastic aluminum coupling 2, 20 mm diameter
and 600 mm length shaft 4, two supports with 6004 deep groove ball
bearings 3 and flywheel disc 5, with holes, bored using 45° angular
step, for imbalance excitation mass fixing. The signal from
acceleration transducers were recorded with multi-channel vibration
signal analyzer OROS Mobi-pack OR-36. The data were analyzed
using vibration signal processing and analysis software OROS
32
NVGate V8.00. The experimental tests were carried out using deep
groove ball bearing, with inner ring race artificially designed fault as
shown in Fig. 17a. This Bearing was mounted in 2nd
support of test rig
located near the flywheel disk 5. During experimentation, the angle β,
between the bearing’s inner ring fault position and the imbalance force
vector Fu angular position, was changed from 0° to 360
° using 45
°
angular steps. The scheme of the angle ß evaluation is shown in Fig.
17 b. The experimentation was carried out using three values of
imbalance on flywheel: 72 g·mm, 120 g·mm and 156 g·mm. The
maximum allowable imbalance, according to ISO 1940-1, for
machines of such type is 125 g·mm (grade G 6.3).
a) b)
Fig. 17 Photography of the inner ring race artificial defect (a) and
explanation scheme of the angular position of imbalance force vector
Fu relative to inner ring race fault location
Dimensions of 6004/C3 rolling bearing: n = 9, number of balls;
fr = 50 Hz rotation frequency shaft with inner ring; BD = 7,8mm ball
diameter; PD = 31 mm, pitch diameter; α = 0° contact angle.
Fig. 18 The vibration velocity spectrum of vertical rotor, with 72
g·mm imbalance value and β = 0° phase angle
Synchronous frequencies 50 Hz vibration velocities dominant in
FFT spectra of vertical rotor, with 100 gmm imbalance and angle β =
0° of imbalance force vector Fu as shown in Fig. 18. Vibration
amplitudes of frequencies of 1 x BPFI, 2 x BPFI, 3 x BPFI and 4 x
BPFI are visible in the FFT vibration velocity spectrum. The 1 x =
50 Hz synchronous frequency vibration velocity amplitude is
dominant in the spectra. Higher harmonics as 2 x= 100 Hz and 3 x=
150 Hz of rotation speed vibration velocity amplitudes indicated
chaotic kinematic motion of the vertical rotor with smaller imbalance
and due to higher radial clearance in C3 class rolling bearing.
Fig. 19 The vibration velocity spectrum of vertical rotor, with 100
g·mm imbalance and β =90° phase angle
34
Comparing the vibration velocity spectra in Fig.18 and Fig. 19,
we observe that changes in angular position of imbalance force Fu
vector changed vibration velocity magnitudes of BPFI frequencies
vibration velocities amplitudes. Vibration velocity root mean square
values vRMS significantly decreased however the vRMS magnitudes of
rotor’s synchronous rotation frequency provide little changes.
In order, to simplify the processing procedure of bearing defect
diagnostics using vibration measurements experimental data and to
make data practically quantifiable and useful, we have designed the
statistical parameter "Defect visibility ratio" (DVR). The defect
visibility ratio DVR is calculated as the vibration parameter velocity
(or acceleration) of dominant bearing defect frequency value vRMS (or
aRMS) dividing by rotors synchronous rotation frequency 1x vibration
vRMS value (or aRMS) according equation (3.1).
The DVR plots versus imbalance values and positions of
imbalance force vector phase angle β of experimental tests processed
by 2x and 2y acceleration transducers signals are shown in Fig. 20 and
Fig. 21. Vertical axis rotors provide higher DVR values independent
of the imbalance values and phase angles in comparison with
horizontal axis rotors. Vertical axis rotor with damaged inner ring of
bearing is more sensitive to imbalance and has higher DVR values.
Rotor generates higher vibration velocities amplitudes of dominant
bearing inner race fault frequency vRMS values, because dynamic
stiffness of vertical rotor is less in comparison with horizontal axis
rotor.
Fig. 20 The DVR plots versus imbalance values and positions of
imbalance force vector phase angles β processed by 2x acceleration
transducer
Fig. 21 The DVR plots versus imbalance values and positions of
imbalance force vector phase angles β of experimental tests processed
by 2y acceleration transducer
Conclusions of subchapter:
1. The vertical axis rotors are more sensitive to imbalance values
in comparison with horizontal axis rotors.
36
2. The identification of bearings inner ring defect using BPFI
frequency in practical diagnostics is more informative in vertical axis
rotors.
3. The bearing’s defect identification in horizontal rotor with
acceleration transducer measuring absolute vibration in direction of
gravity force is not informative.
4. The DVR of vertical axis rotor decreases valuable by
magnifying imbalance force and bearing defect diagnostics of vertical
rotor is more applicable in practice because the DVR is greater in
comparison with horizontal axis rotors.
3.3 INFLUENCE OF MAGNITUDE AND SPATIAL DIRECTION OF
TOTAL DYNAMIC FORCE Fs AND THE BEARING FAULT
SIZE ON DYNAMICS AND DIAGNOSTICS OF VERTICAL
ROTOR
This subpart presents experimental research results of a variable
tilting of axis of vertical rotor with imbalance and artificially damaged
deep groove ball bearings 6004/C3. The imbalance has been varied in
order to determine how the magnitude of imbalance contributes to the
bearing‘s outer ring raceway spalls masking defect. The general
dynamic force acting in variable vertical rotational axis rotors
composed of rotor mass gravity force and unbalance generated force.
In order to increase rotor‘s defects diagnostic procedure accuracy and
identification of technical condition of rotor‘s with bearings housings
vibration measurement data the statistical parameter DVR (Defect
Visibility Ratio) was designed and implemented in practice.
a) b)
Fig. 22 Vertical axis rotor testing stand a) scheme of angle γ tilting
and positions of bearings b) photo of the testing stand. 1 – Tilting part
of foundation; 2 – Guiding rails; 3 – Foundation part that are fixed to
rigid wall; 4 – Rolling axis of foundation tilting mechanism; 5 – 20
mm diameter shaft; 6 – AC motor; 7 – Supports with rolling bearings;
8 - Flywheel disc.
The experimental test stand in Fig. 22a comprises of rigid frame
on which the rotor system is mounted. The system powered with
370 W asynchronous electric motor with current frequency inverter
(SSD Drives, model 650V/003/230F) control, elastic coupling, 20 mm
diameter and 600 mm length shaft, two bearing’s housings with
6004/C3 deep groove ball bearings 1, 2 and flywheel disc with holes
for imbalance masses fixation at radius ru = 60 mm. The artificially
damaged 2nd
bearing outer raceways fixed in the housing.
Each tested bearing 6004/C3 has artificially manufactured outer
ring raceway spalls: first tested has a 1,4 mm and second 3,0 mm
diameter spall, Fig. 23.
38
a) b)
Fig. 23 Artificially manufactured rolling bearings faults a) 1,4 mm
diameter outer ring spall b) 3,0 mm diameter outer ring spall
The bearings outer raceway defect in the housing has been
located in the y transducer position as shown in Fig.24. The
experiment has been carried out with increasing rotor‘s rotational
speed up to 3000 RPM, constant running at 3000 RPM and decreasing
to stand stop.
Fig. 24 Position of bearings outer raceway fault in housing
The 6004/C3 bearing’s with outer ring raceway one spall ball
pass frequency (BPFO) theoretically calculated at nominal rotational
speed 3000 RPM is fBPFO = 168,4 Hz. Imbalance has been changed
Position of outer
raceway fault
from low value uL = 80 g mm, permissible value umax_per = 125 g mm
for G6,3 balancing quality grade (ISO 1940-1), to high value uH =
156 g mm. The imbalances were variable in order to determine how
the magnitude of imbalance contributes to the bearing‘s outer raceway
failures masking effect. Angular position of vertical axis rotor has
been changed as tilting angle γ varies from 0º to 13,5 º. Vibration of
bearings housings measured using the Wilcoxon Research transducers
model 793 (sensitivity 100mV/g) and processed with signal analyzer
OROS Mobi-Pack OR-36, software OROS NVGate V8.00 and OROS
ORBIGate V4.00 and oscilloscope Scopi XII OX7104 (Metrix).
The 2nd
bearing vibration velocity (measured with 2y transducer)
spectrum in cascade format is presented in Fig.25. The vibration
measured with 2x and 2y transducers and plotted in cascade format
has limited information for vibration sources identification in bearings
failures diagnostics. The BPFO and harmonics vibration velocity
amplitudes are too low and not significant for bearing outer raceway
failure diagnostics procedure. The imbalance generated vibration
velocities amplitudes of 1x frequency synchronized with increasing
rotational speed up to n = 3000 RPM dominated in the spectrum and
BPFO frequency fBPFO = 168,4 Hz and harmonics (nX def.) vibration
velocity amplitudes values are too low.
Fig. 25 The 2
nd bearing vibration velocity spectrum in cascade format
plot during acceleration up to 3000 RPM measured by 2y transducer;
nX - synchronous rotational speeds frequencies, nX-def. BPFO
40
vibration velocity amplitudes, tilt angle γ = 13,5º, spall diameter
3,0 mm, imbalance u = 120 g mm
In order to make the procedure of bearings defect diagnostics
practically quantifiable and efficient in technical condition evaluation,
the statistical parameter "Defect Visibility Ratio" (DVR) has been
designed (described in 3.1 chapter). In the case of vertical rotor axis γ
= 0º bearing small spall diameter (1,4 mm) DVR increases with
increasing rotor’s imbalances and slightly dependent of transducers 2x
and 2y locations shown in diagram given in Fig.26. However when
the outer raceway spall diameter is more than two times larger (3,0
mm) the DVR decreases with increasing imbalances because the
bearing’s balls rotate through outer ring spall in enlarge contact area.
The spall damping effect increases and BPFO vibration velocity
values decreases Fig.26.
With increasing rotor’s vertical axis tilting angle γ the DVR
value decreases and slightly depends on rotor’s imbalance (Shown in
Fig. 27) and transducers locations 2x or 2y.
Fig. 26 The DVR versus dynamic force Fs plots
This factor indicates that DVR can be adopted to evaluate rotors
vertical angle position in the cases of installation of new machines not
only for evaluation of technical condition of vertical rotors axis
position and damaged bearings.
Fig. 27 The DVR versus axis tilt angles γ
Conclusions of subchapter
Theoretically simulated vertical axis rotor dynamic force Fs
position angle φ can be used for evaluations not only for degradations
of technical condition of bearings or bearings housing, but for control
of the vertical axis position reference to ideal vertical axis position; it
is important when angular velocities of rotors in technological
machines varies at run up and coast down including resonance
rotational speeds.
In the condition of small tilting angle (e.g. γ < 5º) the
vibration velocity values measured with x and y transducers are the
same order. However as tilting angle increased (e.g. γ > 5 º, as
characterized for sea ships machines) up to γ =13,5 º, the acting forces
on bearings are different and vibration velocities values differs about
20% when measured with x and y transducers.
In the case of outer raceway small spall (1,4 mm as the initial
defect in first phase of degrading bearing) with increasing dynamic
force Fs, the ball contact area with spall increases, and damaged
bearings indications parameter DVR increases, but in the case of large
spall (3,0 mm) the DVR values decreases, because the damping effect
during ball contact with enlarged spall increases.
The DVR parameter useful not only for vertical axis rotors
with antifriction bearing diagnostics, but for rotors with hydrodynamic
bearings technical condition monitoring, technological process control
42
in food and chemical industries (sulfuric acid pumps, sugar production
centrifuges, etc.).
4. EXPERIMENTAL VERIFICATION OF THEORETICAL MODEL
This section of work is devoted to verify a generalized
theoretical model of the vertical rotor. In second chapter of this work
the methodology of calculation of forces acting a vertical rotor
supports were provided. In second chapter of this work also presented
a generalized model of vertical rotor using finite elements. The
generalized rotor model can evaluate the gravity direction and
supports nonlinearity as well as radial gap of bearings.
The experimental research setup presented in Fig. 28, it consist
of AC motor driven by frequency inverter, labeled 1 in figure, elastic
coupling labeled 2, two supports with sliding bearings 3, dv = 20 mm
diameter shaft 4, flywheel disk 5 on which the unbalance mass can be
fixed, optical transducer for the rotational speed measurement 6. On
each of the rotor supports two displacement sensors EPRO PR6423
were mounted.
Fig. 28 Experimental investigation setup for theoretical model
verification
During experimental studies in the first support of rotor the
rolling bearing 6004/ C3 were mounted, in the second support of rotor
(located next to the disk) friction bearings with different radial gaps
were used, the material of friction bearings were PET HD 500. The
frictional bearings used in tests shown in Fig.29. The smallest used
radial gap of frictional bearing was 0,23 mm and the largest was 0,53
mm.
Fig. 29 The frictional bearings used for investigation
During the experimentation, three masses of imbalance where
used, lowest imbalance of 10 gmm, 85 gmm imbalance and 145 gmm
imbalance. In order to compare experimental results with theoretical
model calculations the radial stiffness of frictional bearings was
measured according to methodology described in second chapter. The
comparison of experimentally measured and calculated using FEM
model peak - peak values of shaft center, during first resonance of
rotor system presented in Fig. 30.
The comparison of experimentally measured and calculated
using FEM model rotational speed of first rotor resonance versus
radial gap in 2nd bearing of rotor shown in Fig. 31.
44
Fig. 30 Peak – peak values of shaft center during first resonance,
experimental and calculated results
Fig. 31 First resonance rotational speed of rotor versus radial gap in
2nd
frictional bearing, experimental and calculated results
Conclusions of subchapter
In order to assess the accuracy of the theoretical model,
additional experiments were carried out, when in the second support
of rotor radial sliding bearings with different radial gaps were
mounted. The radial stiffness curve of sliding bearings, for theoretical
model calculations, was measured experimentally.
A comparison of theoretical and experimental results of first
critical rotational speed nk values were used. It was found that at 0,39
mm radial sliding bearings gap, values between the theoretical model
and experimental data showed the highest relative error of 2,94%.
Relative error values indicate that the theoretical generalized vertical
rotor model, quite high accuracy and can be used to investigate the
behavior of the rotor.
MAIN CONCLUSIONS
1. Literature analysis of rotor dynamics fundamentals covered
stages of developments, analysis and review of modern methods and
tools applied to rotor dynamics research field. It was found that the
rotors with a vertical axis of rotation, as a research object, are usually
examined in order to analyze the influence of variable rotor properties
(mass, moment of inertia, nonlinear stiffness, variable damping, rotor
design) precession motion or in order to analyze the influence of
different non-linearity’s of supports stiffness to precession motion.
The material presented in the scientific literature has been analyzed,
focusing on the traditional, newly designed research methods for rotor
systems and their elements faults diagnostic and technical condition
monitoring. It was found that identification of technical condition of
rotor systems and diagnostics of defects are extremely relevant to the
creation of modern rotortronic systems and to renewal of long time
operated ones. Due to this fact, experimental research are being
developed continuously improving traditional diagnostic testing
methods and tools to create automatic failure prevention and forecast
methods. It was found that the diagnostic research methods, newly
developed under laboratory conditions, showed positive results of
rotor defects identification, but practical application becomes limited
when testing in Situ. Applying newly developed diagnostic methods in
practice, usually rotor dynamics is not proper taken into account. Thus
application of such methods becomes limited or difficult and expected
output is not reached. Literature analysis has showed that there is no
46
any detailed study which quantifiably aims to link vertical rotors
dynamics and defects diagnostics methods and their industrial
application.
2. Methodology for calculation of forces, acting to vertical rotors
supports, was developed. In accordance with methodology radial axial
loads of vertical rotors were calculated. It was established, that at rotor
speed of n = 3000 RPM the double increment of laboratory stand
imbalance mass (from 80 gmm to 154 gmm) results increasing by only
5 N of total force Fs, acting to rotor support next to the disk, while the
angle φ of both rotor rotation axis and the total force Fs increases by
17˚. It was found that due to the imbalance increased radial force
acting to rotor support significantly effects direction of the total rotor
support force Fs while magnitude is affected insignificantly.
Calculations were carried out not considering the rotor dynamics, gyro
effect, so this finding is theoretical.
3. In this work generalized vertical rotor model, which allows
estimating the effect of gyro and gravity, was developed. Using this
numerical model reaction forces at rotor supports were calculated,
capturing influence of imbalance. From constructed Campbell chart
critical angular velocity map ωk = 559 rad/s of the system being
analyzed was defined. It was found that even a small deviation of the
rotor rotation axis from the vertical, leads to appearance of subcritical
rotational speed. It is caused by bearing radial gap at the second
support. This gap also defines the system dynamic stiffness. It was
estimated that assessment of the effects of rotor dynamics affecting
the rotor system at rotational speed of the rotor n = 3000 RPM, double
increase of imbalance (from 80 gmm to 153 gmm) leads to increase of
the total force Fs next to the disk only slightly (only 6 N, from 31 N to
37 N). Total force Fs, angle φ, which it forms with the axis of rotation,
increases significantly by 15,5 degrees. At the critical rotational speed
ωk = 559 rad/s of the rotor the total force Fs acting to the second
support of rotor increases to 123 N, while the angle φ between the
total force and the rotor axis of rotation increases insignificantly by 6
degrees only.
4. After the comparative study of diagnostic tests of defects in
vertical and horizontal rotor rolling bearings, a new relative parameter
- Defect Visibility Ratio (DVR) was derived. DVR allows the quantity
assessment of differences among rotor defects diagnostic results.
Studies of rotor systems with differently oriented axis of rotation have
showed that defect indications of horizontal rotor system in many
cases are clearer. It allows for the researcher to identify the rolling
bearing defects in the early stages of their initiation. It was found that
defect on the rolling surface of bearing outer ring in horizontal rotor is
more precisely identified at horizontal plane which is perpendicular to
the defect. However, for vertical rotor bearings in both radial
directions defect is identified with no difference in accuracy.
5. After dynamics and diagnostic tests of the rotor with defect on
the inner surface of bearing ring under conditions of mismatch
between dynamic imbalance force and the phase angle of defect on
inner surface of bearing ring, it was found that the vertical rotors are
significantly more sensitive to the effects of imbalance, their defect
indications brightness, depends more on the magnitude of dynamic
imbalance force Fc. It was also found that the identification of defects
on inner surface of rolling bearing ring in horizontal rotors along the
direction of gravity force is uninformative. Defect indication does not
change even changing the dynamic imbalance force Fc.
6. During diagnostic investigation test of rolling bearings of
vertical rotor, which axis of rotation was tilted from the vertical the
following was found: when tilting of rotor system from the vertical is
up to 5˚ results measured in x and y directions are similar. The
difference is caused by the defect position in support (defect was
oriented in the y direction). At higher vertical rotor axis deviation
from the vertical (angle γ = 10˚ - 13,5˚), rotor dynamics makes more
influence to data measured in different radial directions. This
phenomenon is caused by variable dynamic stiffness of support during
test. It can be highlighted that under condition of larger (3,0 mm)
defect spall at surface of rolling bearing, outer ring angle β doesn’t
affect fault indication. It is caused by rolling elements which roll
48
through the defect and result increase in total dynamic force Fs.
Thus, defect indication decreases and also the parameter DVR
decreases.
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with normal operating speeds of 1 500 r/min, 1 800 r/min, 3 000
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machine vibration by measurements on non-rotating parts –
Part 3: Industrial machines with nominal power above 15 kW and
nominal speeds between 120 r/min and 15 000 r/min when
measured in situ“. 2009.
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vibration by measurements on non-rotating parts - Part 4: Gas
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LIST OF AUTHOUR’S SCIENTIFIC PUBLICATIONS
Articles in the Journals from the list of Institute of Scientific Information
(ISI)
1. Barzdaitis, Vytautas; Tadžijevas, Artūras; Mažeika, Pranas;
Grigonienė, Jurga; Modeling and diagnostics of vertical axis
rotary system powered by multi gear drive // Journal of
Vibroengineering. Kaunas: Vibrotechnika. ISSN 1392 – 8716.
2012, vol. 14, iss. 1, p. 171-178. [ISI Web of Science; INSPEC].
2. Artūras Tadžijevas, Vytautas Barzdaitis, Marius Vasylius, Pranas
Mažeika; The Comparison of Diagnostic Features between the
Vertical and Horizontal Axis Rotors // Journal of
Vibroengineering. Kaunas: Vibrotechnika. ISSN 1392 – 8716.
2013, vol. 16,[ISI Web of Science; INSPEC].
3. Artūras Tadžijevas, Vytautas Barzdaitis, Pranas Mažeika, Marius
Vasylius; Influence of Imbalance Force Angular Position to
Vertical and Horizontal Rotors Rolling Bearings Defects
Diagnostics // Journal of Vibroengineering. Kaunas:
Vibrotechnika. ISSN 1392 – 8716. 2014, vol. 16, iss. 3. [ISI Web
of Science; INSPEC].
52
4. Barzdaitis, Vytautas; Barzdaitis, Vytautas V.; Maskvytis,
Robertas; Tadžijevas, Artūras; Vasylius, Marius. "New deep
groove ball bearings high frequencies vibration testing" // ISSN
1392-1207. Mechanika. 2014 Volume 20(3), p. 287-293.
INFORMATION ABOUT AUTHOR
Artūras Tadžijevas was born in Klaipeda on November 12th,
1982. In 2001, he graduated from Klaipeda “Vetrunge” gymnasium.
During 2001-2005, he studied at Klaipeda University, Faculty of
Marine Engineering and in 2005 was awarded with a Bachelor’s
degree in mechanical engineering. During 2005-2007, he studied at
Klaipeda University, Faculty of Marine Engineering and in 2007 was
awarded with a Master’s qualification degree in mechanical
engineering. In 2010, started and in 2012 completed his doctoral
studies in a field of mechanical engineering at Kaunas University of
Technologies.
E-mail: [email protected]
REZIUMĖ
Daktaro disertaciją sudaro įvadas, keturi skyriai, išvados ir cituotų
šaltinių sąrašas bei priedai. Bendra disertacijos apimtis142 puslapiai,
107 paveikslai ir 91 bibliografinė nuoroda.
Pirmajame daktaro disertacijos skyriuje analizuojama mokslinėje
periodikoje bei tarptautiniuose standartuose publikuotų rotorių
dinamikos ir jos sąryšis su rotorių elementų diagnostika. Skyriaus
pabaigoje pateikiamos skyriaus išvados.
Antrasis daktaro disertacijos skyrius dedikuotas analitinio
vertikalių rotorių bei baigtinių elementų modelio veikimui aprašyti.
Skyriuje taip pat pateikti skaičiavimų rezultatai. Skyriaus pabaigoje
pateikiamos skyriaus išvados.
Trečiajame skyriuje pateikiami trys nepriklausomi
eksperimentiniai tyrimai. Pirmasis tyrimas pateiktas pirmajame šio
skyriaus poskyryje ir yra skirtas ištirti ir palyginti vertikalių ir
horizontalių rotorių dinamikos įtaką šių rotorių riedėjimo guolių
diagnostikai. Skyriuje pateikiamas naujas, sukurtas statistinis
parametras, kurio dėka galime palyginti rotorių diagnostikos
ypatumus. Artajame šio skyriaus poskyryje pateiktas vertikalių ir
horizontalių rotorių eksperimentinis tyrimas su vidinio riedėjimo
guolio žiedo defektu, kai vidinio žiedo defekto ir dinaminės
disbalanso jėgos fazės kampas nesutampa. Trečiajame šio skyriaus
poskyryje pateiktas vertikalių rotorių pasvirusių nuo vertikalės,
dinamikos ir diagnostikos tyrimas. Poskyrio tikslas nusakyti, kaip
suminės dinaminės disbalanso jėgos bei ašinės jėgos dydis ir kampas
įtakoja vertikalių rotorių elementų gedimų diagnostiką. Skyriaus
pabaigoje pateikiamos išvados.
Ketvirtajame šio darbo skyriuje pateikiamas apibendrinto
vertikalių rotorių baigtinių elementų modelio verifikavimas. Skyriuje
aprašomas eksperimentinis tyrimas, kuris atliktas su skirtingą radialūjį
tarpą turinčiais slydimo guoliais, rezultatai lyginami su skaičiavimo
rezultatais. Skyriaus pabaigoje pateikiamos išvados.
Darbo pabaigoje pateikiamos bendrosios išvados, bibliografinių
nuorodų sąrašas, publikuotų, su šio darbo tematika susijusių, autoriaus
mokslinių darbų sąrašas, priedai.
INFORMACIJA APIE AUTORIŲ
Artūras Tadžijevas gimė 1982 metų lapkričio 12 dieną, Klaipėdoje.
2001 metais baigė „Vėtrungės“ gimnaziją Klaipėdoje. 2001 – 2005
metais studijavo Klaipėdos universitete, Jūrų technikos fakultete, įgijo
mechanikos inžinerijos bakalauro kvalifikacinį laipsnį. 2005 – 2007
metais studijavo Klaipėdos universitete, Jūrų technikos fakultete, įgijo
mechanikos inžinerijos magistro kvalifikacinį laipsnį. 2010 metais
pradėjo ir 2014 metais baigė Kauno technologijos universiteto
mechanikos inžinerijos mokslo krypties doktorantūros studijas.
El. paštas: [email protected]
54
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