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Pannkaaj More, D.H. Burande / International Journal of Engineering Research and
Applications (IJERA) ISSN: 2248-9622 www.ijera.com
Vol. 3, Issue 4, Jul-Aug 2013, pp. 442-446
442 | P a g e
Vibration Performance Evaluation of Collecting plates of
Electrostatic Precipitators Using FEAApproach
Pannkaaj More1
, D.H. Burande2
1
(Thermax Ltd. Enviro Division, Pune, Maharashtra, India)
2
(Department of Mechanical Engineering, Sinhgad College of Engineering, Pune, Maharashtra, India)
ABSTRACT
Electrostatic Precipitators is the device
used for removal of dust from boiler process
gases. Various factors affect the effectiveness of
this device. One of them is regular cleaning of the
collecting electrodes. The dust removal takes
place due to vibrations of collecting electrodes.
Further, in time bound project
development, it becomes very difficult to test at
every stage of design improvements which also
affect the project cost. In such cases, more
practical approach is to make design
improvements through simulations followed by
validation through physical measurements.
This paper presents FEA approach for
modeling and analysis of collecting electrodes in
an electrostatic precipitator using Implicit
transient dynamic analysis approach.
Experimental testing is done for validation of
results. The results of FEA approach and testing
are discussed.
Keywords - Collecting electrodes, Electrostatic
Precipitator, Experimental testing, FEA, Vibration
analysis
I. INTRODUCTION
Dust particles contained in various process
gases is one of the major industrial air pollution
problem that must be controlled. Electrostatic
Precipitator (ESP) is one of the more frequently used
device to remove the dust from process gas. The
effective work of an electrostatic precipitator
depends on the conditions of gas flow, the generated
electric field and the geometric parameters of the
electrostatic precipitator (ESP).
The efficiency of ESP also depends on the efficiency
of the periodic cleaning of the collecting electrodes
[1]. The collecting electrodes are provided with a
dust removal system, which removes dust that has
gathered on the electrodes. Dust is removed by
inducing vibrations at accelerations, which will
effectively detach dust that has collected on
electrode surfaces [2].
The vibrations generated at the assembly
plays vital role in improving ESP performance.
These vibrations are created by gravity operated
rapping system, in which plunger is made to fall on
rod. Due to these
vibrations dust deposited on collecting electrodes
falls in hoppers.
Thus effective working of rapping system
plays important role in dust removal process.
Different accelerations are developed are at different
locations of the system. Accelerations are mainly
depends on both energy of the rapper at the moment
of impact and the way in which the force is
transferred to the collecting electrodes and also
Geometrical features of the electrodes (shape,
length, thickness) .Impact force generated by the
rapper have an essential influence on tangent and
normal accelerations at different points of the plates,
and thus on the effectiveness of the dust removal
process [3].
Various experimental studies were done by
researchers to ensure effective removal of dust from
collecting electrodes.
This experimental approach has major drawbacks of
higher time lines and cost involved in physical
testing. Need is felt to develop a quick and reliable
method to evaluate the vibration performance of
ESP. CAE simulations are often used to for
evaluating different designs.
This paper describes simulation procedure of
evaluating ESP.
II. DETAILS OF ESP SYSTEM
Typical ESP System consists of rows of
collecting electrodes mounted parallaly and hanging
between top and bottom hangers. Top hangers are
mounted on support channel, which are hanging
through roof bolts. Anvil is mounted on top hangers
on which rapper rod is placed. Electromagnetically
operated plunger is placed on top of rapper rod
which lifts and falls on it periodically. Due to this
impact collecting electrode gets vibrated. These
periodic vibrations are responsible for removal of
dust from collecting electrodes.
Fig.1 shows typical assembly of collecting
electrodes and rapping system of ESP.
Pannkaaj More, D.H. Burande / International Journal of Engineering Research and
Applications (IJERA) ISSN: 2248-9622 www.ijera.com
Vol. 3, Issue 4, Jul-Aug 2013, pp. 442-446
443 | P a g e
Fig.1 Typ assembly of collecting electrodes of ESP
III. DETAILS OF FE MODEL
Due to complicated geometry and large size
of dimensions use of FEA method for modelling and
analysis of vibrations of collecting electrodes is
much suitable option. For finite element analysis
subassembly of two parallel collecting plates is
considered as shown in fig.2. The commercial
software packages are used for modelling, meshing
and analysis of the system. In this collecting plates
and top & bottom hangers are modelled using
shell63 element. Discretisation of the solid
components like rapper rod, anvil & bolt is done
using solid45 element. Collecting plate to hanger
bolt connection is modelled using rigid element.
Connections of top hanger to support channel and
rapper rod to anvil plate are considered as fixed
connections as shown in fig.3. Analysis is done by
using ANSYS package.
Fig.2 Subassembly of ESP collecting plates
Fig.3 FE Model details of ESP subsystem
IV. ANALYSIS METHODOLOGY
Following analysis are done for evaluation of
ESP subsystem.
Modal analysis:
It is done to study of the dynamic character
of a system. These characteristics can be defined
independently from the loads applied to the system
and the response of the system. It is a technique used
to determine a structure’s vibration characteristics:
like, Natural frequencies, Mode shapes, Mode
participation factors (how much a given mode
participates in a given direction). Refer fig.4 for FE
model boundary conditions used for modal analysis.
Fig.4 FE model for modal analysis
Pannkaaj More, D.H. Burande / International Journal of Engineering Research and
Applications (IJERA) ISSN: 2248-9622 www.ijera.com
Vol. 3, Issue 4, Jul-Aug 2013, pp. 442-446
444 | P a g e
This also helps to predict resonant
frequencies. Refer fig.5 for first 10 modes of ESP
subsystem. Significance of modal analysis also helps
to set plunger hitting frequency outside the range of
natural frequencies of subsystem.
SET FREQ (Hz)
1 0.15397
2 1.0328
3 1.0855
4 1.1381
5 1.2978
6 1.2984
7 1.4502
8 1.7436
9 1.7495
10 1.7519
Fig.5 Natural frequencies calculated from modal
analysis
Transient analysis:
Plunger hitting operation is the transient
event which depends on the time taken to complete
one hitting cycle. This type of event cannot be
simulated using conventional static analysis
approach. Transient analysis is the most appropriate
approach in order to simulate such events.
Transient analysis approach helps to study response
of a system for particular time intervals. Output such
as amplitude w.r.t time can be captured accurately at
various locations.
In present exercise, transient analysis is
carried out to measure plate displacement when
plunger hits rapper rod. System response is
measured for 3.5sec from the moment of impact. To
determine the expected impact force, pulse width of
expected time force curve is required to be
estimated. Impact acceleration is calculated from the
change in velocity during the pulse width time. The
highest peak impact forces occur when there is a
steel-on-steel impact. The initial and final velocities
of impact are depends on structure stiffness. The
resulting peak acceleration is calculated from below
equation [9],
𝑎 =
𝑑𝑣
𝑑𝑡
=
𝑑𝑣
𝑡 𝑝𝑢𝑙𝑠𝑒
=
𝑉 𝐼𝑛𝑖𝑡𝑖𝑎𝑙 − 𝑉 𝐹𝑖𝑛𝑎𝑙
𝑡 𝑝𝑢𝑙𝑠𝑒
= 2x
2𝑔ℎ
𝑡 𝑝𝑢𝑙𝑠𝑒
(1)
The impact force is then calculated from Newton’s
2nd law equation,
F = ma ... (2)
Calculated impact force is applied at top of
rapper rod. Refer fig.6 for boundary conditions of
the transient analysis of ESP system. From Transient
analysis, displacements at various locations of plates
are measured. Higher the displacements better the
cleaning efficiency. The displacements targets are
decided based on design space constraint and
electrical components clearances available.
Fig.6 Model for Transient Analysis
V. ANALYSIS RESULTS
Refer fig.7 for details of locations where
displacements are measured in analysis.
Fig.7 Measurement locations (A,B,C)
The result of FEA method performed using
ANSYS package founds good agreement with
testing data. Result data is mainly governed by
model geometry and accurate estimation of impact
force. Fig.8 shows displacement vs time plot.
Maximum displacement is occurring within first 0.5
sec time after impact. And within next 1 to 1.5 sec it
is almost getting damped.
Pannkaaj More, D.H. Burande / International Journal of Engineering Research and
Applications (IJERA) ISSN: 2248-9622 www.ijera.com
Vol. 3, Issue 4, Jul-Aug 2013, pp. 442-446
445 | P a g e
Fig.8 Displacement vs time plots measured at, (A)
At Middle of plate, (B) At 1m from top, (C) At 1m
from plate bottom
VI. VALIDATION OF RESULTS
Validation is done by comparing the results
of FEA method with measurements performed on
physical model. Testing is done on actual onsite
equipment of Electrostatic Precipitator as shown in
Fig.10,11.
The instrument Vibration Analyzer is used
for the measurement of vibrations. As electrode
vibrations occurred by rapping system is random
process and due to critical geometry and parameters
occurring errors in measurement various set of trials
are required to be taken during measurement. Fig.10
shows actual picture of collecting plate assembly.
The analysis output i.e. displacements are compared
with the physical testing measurements, refer Fig.9.
Measurement Locations A B C
Displacement
(mm)
FEA method 7.1 5.1 3
Testing data 6.5 4.6 2.8
Fig.9 Table of displacement values measured
Fig.10 Onsite Equipment of ESP
Fig.11 Collecting plate subassembly of Testing
Equipment
VII. CONCLUSION
The vibration excitation of collecting
electrodes mainly depends upon impact force and
system geometry. Maximum displacement is
occurring at middle of the collecting electrode and
minimum at the bottom. The result of validation
gives good agreement between FEA method and
testing data. With this respect FEA method
presented in this paper can be useful for predicting
the vibration behavior of the system during its
design stage. It enables us to assess the effect of
different geometrical parameters such as collecting
Pannkaaj More, D.H. Burande / International Journal of Engineering Research and
Applications (IJERA) ISSN: 2248-9622 www.ijera.com
Vol. 3, Issue 4, Jul-Aug 2013, pp. 442-446
446 | P a g e
plate profile, plate thickness and rapping location of
the system on its vibrations. This method is much
simpler, cost effective and time saving as compared
to actual physical testing of the system.
VIII. ACKNOWLEDGEMENTS
We would like to thank Mr. P.G.Soman
(Design-Head) and Mr. Pradeep Deore (Design-
Manager) for giving the opportunity to work on this
challenging project and to present this paper.
Also we would like to thank Mr.Prashant
Chavan and AMCON Consultech for providing
guidance in CAE simulation. And Mr.Sandeep
Kadam, Mr.Ganesh Chavan, Mr.Nandkishor Yadav
and Dr.S.V. Deshpande involved in the physical
testing and measurement.
REFERENCES
[1] Andrzej Nowak, Vibration of collecting
electrodes in electrostatic precipitators -
Modelling, measurements and simulation
tests, Journal of Electrostatics 70 (2012)
327e332
[2] Nowak Andrzej, Wojciech Stanisław,
Optimisation and experimental verification of
a dust-removal beater for the electrodes of
electrostatic precipitators, Computers and
Structures 82 (2004) 1785–1792.
[3] Iwona Adamiec-Wojcik, Nowak Andrzej,
Wojciech Stanisław , Comparison of methods
for vibration analysis of electrostatic
precipitators,Acta Mech Sin DOI
10.1007/s10409-011-0415-2
[4] Michael Neundorfer, Electrode cleaning
system : Optimizing rapping energy and
rapping control, Environment International,
Vol.6.pp.279-287,1981
[5] HU Manyin, LIU Yujing, YIN Qi, LIU
Zhong, GAO Xianglin, Research on
Vibration Period Optimization of
Electrostatic Precipitator, 11th International
Conference on Electrostatic Precipitation.
[6] S.H. Kim, K.W. Lee, Experimental study of
electrostatic precipitator performance and
comparison with existing theoretical
prediction models, Journal of Electrostatics
48 (1999) 3}25
[7] A.P. Nowak, Measurement verification of the
hybrid finite element method, ECCM2010
[8] Iwona Adamiec-Wójcik, Modelling of systems
of collecting electrodes of electrostatic
precipitators by means of the rigid finite
element method, The archive of mechanical
engineering2010, 10.2478/v10180-011-0002-x
[9] Robert Metz, PCB Piezotronics, Impact and
Drop Testing with ICP Force Sensors,
SOUND AND VIBRATION/FEBRUARY

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  • 1. Pannkaaj More, D.H. Burande / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 4, Jul-Aug 2013, pp. 442-446 442 | P a g e Vibration Performance Evaluation of Collecting plates of Electrostatic Precipitators Using FEAApproach Pannkaaj More1 , D.H. Burande2 1 (Thermax Ltd. Enviro Division, Pune, Maharashtra, India) 2 (Department of Mechanical Engineering, Sinhgad College of Engineering, Pune, Maharashtra, India) ABSTRACT Electrostatic Precipitators is the device used for removal of dust from boiler process gases. Various factors affect the effectiveness of this device. One of them is regular cleaning of the collecting electrodes. The dust removal takes place due to vibrations of collecting electrodes. Further, in time bound project development, it becomes very difficult to test at every stage of design improvements which also affect the project cost. In such cases, more practical approach is to make design improvements through simulations followed by validation through physical measurements. This paper presents FEA approach for modeling and analysis of collecting electrodes in an electrostatic precipitator using Implicit transient dynamic analysis approach. Experimental testing is done for validation of results. The results of FEA approach and testing are discussed. Keywords - Collecting electrodes, Electrostatic Precipitator, Experimental testing, FEA, Vibration analysis I. INTRODUCTION Dust particles contained in various process gases is one of the major industrial air pollution problem that must be controlled. Electrostatic Precipitator (ESP) is one of the more frequently used device to remove the dust from process gas. The effective work of an electrostatic precipitator depends on the conditions of gas flow, the generated electric field and the geometric parameters of the electrostatic precipitator (ESP). The efficiency of ESP also depends on the efficiency of the periodic cleaning of the collecting electrodes [1]. The collecting electrodes are provided with a dust removal system, which removes dust that has gathered on the electrodes. Dust is removed by inducing vibrations at accelerations, which will effectively detach dust that has collected on electrode surfaces [2]. The vibrations generated at the assembly plays vital role in improving ESP performance. These vibrations are created by gravity operated rapping system, in which plunger is made to fall on rod. Due to these vibrations dust deposited on collecting electrodes falls in hoppers. Thus effective working of rapping system plays important role in dust removal process. Different accelerations are developed are at different locations of the system. Accelerations are mainly depends on both energy of the rapper at the moment of impact and the way in which the force is transferred to the collecting electrodes and also Geometrical features of the electrodes (shape, length, thickness) .Impact force generated by the rapper have an essential influence on tangent and normal accelerations at different points of the plates, and thus on the effectiveness of the dust removal process [3]. Various experimental studies were done by researchers to ensure effective removal of dust from collecting electrodes. This experimental approach has major drawbacks of higher time lines and cost involved in physical testing. Need is felt to develop a quick and reliable method to evaluate the vibration performance of ESP. CAE simulations are often used to for evaluating different designs. This paper describes simulation procedure of evaluating ESP. II. DETAILS OF ESP SYSTEM Typical ESP System consists of rows of collecting electrodes mounted parallaly and hanging between top and bottom hangers. Top hangers are mounted on support channel, which are hanging through roof bolts. Anvil is mounted on top hangers on which rapper rod is placed. Electromagnetically operated plunger is placed on top of rapper rod which lifts and falls on it periodically. Due to this impact collecting electrode gets vibrated. These periodic vibrations are responsible for removal of dust from collecting electrodes. Fig.1 shows typical assembly of collecting electrodes and rapping system of ESP.
  • 2. Pannkaaj More, D.H. Burande / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 4, Jul-Aug 2013, pp. 442-446 443 | P a g e Fig.1 Typ assembly of collecting electrodes of ESP III. DETAILS OF FE MODEL Due to complicated geometry and large size of dimensions use of FEA method for modelling and analysis of vibrations of collecting electrodes is much suitable option. For finite element analysis subassembly of two parallel collecting plates is considered as shown in fig.2. The commercial software packages are used for modelling, meshing and analysis of the system. In this collecting plates and top & bottom hangers are modelled using shell63 element. Discretisation of the solid components like rapper rod, anvil & bolt is done using solid45 element. Collecting plate to hanger bolt connection is modelled using rigid element. Connections of top hanger to support channel and rapper rod to anvil plate are considered as fixed connections as shown in fig.3. Analysis is done by using ANSYS package. Fig.2 Subassembly of ESP collecting plates Fig.3 FE Model details of ESP subsystem IV. ANALYSIS METHODOLOGY Following analysis are done for evaluation of ESP subsystem. Modal analysis: It is done to study of the dynamic character of a system. These characteristics can be defined independently from the loads applied to the system and the response of the system. It is a technique used to determine a structure’s vibration characteristics: like, Natural frequencies, Mode shapes, Mode participation factors (how much a given mode participates in a given direction). Refer fig.4 for FE model boundary conditions used for modal analysis. Fig.4 FE model for modal analysis
  • 3. Pannkaaj More, D.H. Burande / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 4, Jul-Aug 2013, pp. 442-446 444 | P a g e This also helps to predict resonant frequencies. Refer fig.5 for first 10 modes of ESP subsystem. Significance of modal analysis also helps to set plunger hitting frequency outside the range of natural frequencies of subsystem. SET FREQ (Hz) 1 0.15397 2 1.0328 3 1.0855 4 1.1381 5 1.2978 6 1.2984 7 1.4502 8 1.7436 9 1.7495 10 1.7519 Fig.5 Natural frequencies calculated from modal analysis Transient analysis: Plunger hitting operation is the transient event which depends on the time taken to complete one hitting cycle. This type of event cannot be simulated using conventional static analysis approach. Transient analysis is the most appropriate approach in order to simulate such events. Transient analysis approach helps to study response of a system for particular time intervals. Output such as amplitude w.r.t time can be captured accurately at various locations. In present exercise, transient analysis is carried out to measure plate displacement when plunger hits rapper rod. System response is measured for 3.5sec from the moment of impact. To determine the expected impact force, pulse width of expected time force curve is required to be estimated. Impact acceleration is calculated from the change in velocity during the pulse width time. The highest peak impact forces occur when there is a steel-on-steel impact. The initial and final velocities of impact are depends on structure stiffness. The resulting peak acceleration is calculated from below equation [9], 𝑎 = 𝑑𝑣 𝑑𝑡 = 𝑑𝑣 𝑡 𝑝𝑢𝑙𝑠𝑒 = 𝑉 𝐼𝑛𝑖𝑡𝑖𝑎𝑙 − 𝑉 𝐹𝑖𝑛𝑎𝑙 𝑡 𝑝𝑢𝑙𝑠𝑒 = 2x 2𝑔ℎ 𝑡 𝑝𝑢𝑙𝑠𝑒 (1) The impact force is then calculated from Newton’s 2nd law equation, F = ma ... (2) Calculated impact force is applied at top of rapper rod. Refer fig.6 for boundary conditions of the transient analysis of ESP system. From Transient analysis, displacements at various locations of plates are measured. Higher the displacements better the cleaning efficiency. The displacements targets are decided based on design space constraint and electrical components clearances available. Fig.6 Model for Transient Analysis V. ANALYSIS RESULTS Refer fig.7 for details of locations where displacements are measured in analysis. Fig.7 Measurement locations (A,B,C) The result of FEA method performed using ANSYS package founds good agreement with testing data. Result data is mainly governed by model geometry and accurate estimation of impact force. Fig.8 shows displacement vs time plot. Maximum displacement is occurring within first 0.5 sec time after impact. And within next 1 to 1.5 sec it is almost getting damped.
  • 4. Pannkaaj More, D.H. Burande / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 4, Jul-Aug 2013, pp. 442-446 445 | P a g e Fig.8 Displacement vs time plots measured at, (A) At Middle of plate, (B) At 1m from top, (C) At 1m from plate bottom VI. VALIDATION OF RESULTS Validation is done by comparing the results of FEA method with measurements performed on physical model. Testing is done on actual onsite equipment of Electrostatic Precipitator as shown in Fig.10,11. The instrument Vibration Analyzer is used for the measurement of vibrations. As electrode vibrations occurred by rapping system is random process and due to critical geometry and parameters occurring errors in measurement various set of trials are required to be taken during measurement. Fig.10 shows actual picture of collecting plate assembly. The analysis output i.e. displacements are compared with the physical testing measurements, refer Fig.9. Measurement Locations A B C Displacement (mm) FEA method 7.1 5.1 3 Testing data 6.5 4.6 2.8 Fig.9 Table of displacement values measured Fig.10 Onsite Equipment of ESP Fig.11 Collecting plate subassembly of Testing Equipment VII. CONCLUSION The vibration excitation of collecting electrodes mainly depends upon impact force and system geometry. Maximum displacement is occurring at middle of the collecting electrode and minimum at the bottom. The result of validation gives good agreement between FEA method and testing data. With this respect FEA method presented in this paper can be useful for predicting the vibration behavior of the system during its design stage. It enables us to assess the effect of different geometrical parameters such as collecting
  • 5. Pannkaaj More, D.H. Burande / International Journal of Engineering Research and Applications (IJERA) ISSN: 2248-9622 www.ijera.com Vol. 3, Issue 4, Jul-Aug 2013, pp. 442-446 446 | P a g e plate profile, plate thickness and rapping location of the system on its vibrations. This method is much simpler, cost effective and time saving as compared to actual physical testing of the system. VIII. ACKNOWLEDGEMENTS We would like to thank Mr. P.G.Soman (Design-Head) and Mr. Pradeep Deore (Design- Manager) for giving the opportunity to work on this challenging project and to present this paper. Also we would like to thank Mr.Prashant Chavan and AMCON Consultech for providing guidance in CAE simulation. And Mr.Sandeep Kadam, Mr.Ganesh Chavan, Mr.Nandkishor Yadav and Dr.S.V. Deshpande involved in the physical testing and measurement. REFERENCES [1] Andrzej Nowak, Vibration of collecting electrodes in electrostatic precipitators - Modelling, measurements and simulation tests, Journal of Electrostatics 70 (2012) 327e332 [2] Nowak Andrzej, Wojciech Stanisław, Optimisation and experimental verification of a dust-removal beater for the electrodes of electrostatic precipitators, Computers and Structures 82 (2004) 1785–1792. [3] Iwona Adamiec-Wojcik, Nowak Andrzej, Wojciech Stanisław , Comparison of methods for vibration analysis of electrostatic precipitators,Acta Mech Sin DOI 10.1007/s10409-011-0415-2 [4] Michael Neundorfer, Electrode cleaning system : Optimizing rapping energy and rapping control, Environment International, Vol.6.pp.279-287,1981 [5] HU Manyin, LIU Yujing, YIN Qi, LIU Zhong, GAO Xianglin, Research on Vibration Period Optimization of Electrostatic Precipitator, 11th International Conference on Electrostatic Precipitation. [6] S.H. Kim, K.W. Lee, Experimental study of electrostatic precipitator performance and comparison with existing theoretical prediction models, Journal of Electrostatics 48 (1999) 3}25 [7] A.P. Nowak, Measurement verification of the hybrid finite element method, ECCM2010 [8] Iwona Adamiec-Wójcik, Modelling of systems of collecting electrodes of electrostatic precipitators by means of the rigid finite element method, The archive of mechanical engineering2010, 10.2478/v10180-011-0002-x [9] Robert Metz, PCB Piezotronics, Impact and Drop Testing with ICP Force Sensors, SOUND AND VIBRATION/FEBRUARY