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Interna
ISSN (O
www.ijr
Mod
Co
ABSTRA
Cymbal
transduce
modal un
stress lim
shows th
study, un
applicati
KEYWO
ELEMENT
Cym
bonding p
caps can
of high im
The vibr
analysis m
modal ch
sources o
dynamic
In this p
boundary
Cymbal t
Cym
epoxy res
2.1 Intr
As show
tional Journ
Online): 232
res.org Volu
del Anal
ollege of Urba
ACT : In ord
transducer. T
er can be app
nder the specif
mits are in th
at suitable fo
nder low frequ
ions.
ORDS CYMBA
T METHOD
mbal transduce
pressure of co
be low imped
mpedance, the
ration mode is
method which
haracteristics c
of the actual v
design and th
paper the Cym
y stress constr
transducer can
mbal transduce
sin and metal
oduction ab
wn in section
nal of Resea
20-9364, ISS
ume 3 Issue
ysis of C
an Railway Tr
der to study t
Through the u
plied on differ
ific natural fre
e security do
or large load
uency vibratio
AL TRANSDUCE
er is made up b
ombination wh
dance, high be
e path toward
s the inherent
h can figure o
can be predict
vibration respo
he fault diagno
mbal transduc
raints, the mo
n device of tra
er is a miniatu
end cap struc
Fig
bout the con
view 2, the
arch in Eng
SN (Print):
6 ǁ June 20
w
Cymbal G
C
Shi Yanc
ransportation
the influence f
use of ANSYS
rent constrain
equencies and
main, the mo
under low fre
on Cymbal tr
ER , MODEL A
I.
by two cymba
hich has small
ending axial de
the expansion
t and the ove
ut the structur
ted structure i
onse. Therefor
osis of the equ
cer can under
odal analysis u
ain vibration e
II. C
urized V crook
ture, the 3D e
gure 1. 3D ent
struction
Cymbal harv
gineering an
2320-9356
015 ǁ PP.05-
www.ijres.org
Generato
Condition
chao and Y
of Shanghai U
201620,China
for natural fr
S and SIMUL
nts and load c
d mode shape
odal analysis
equency vibra
ransducer can
ANALYSIS, INH
INTRODU
al shaped meta
l volume, ligh
eformation tra
n deformation
erall character
re in a suscep
in this frequen
re, the modal
uipment.
r the force co
using finite el
energy recover
CYMBAL TRA
ked device wh
entity model a
tity model of C
ester consists
nd Science (
6
12
g
or Unde
ns
Yang Jian
University of E
a
frequency und
LATION with
conditions, ca
s. Which in th
results of vib
ation of train
n provide sim
HERENT FREQU
CTION
al cap and pie
ht weight, can
ansformation
n[1]
.
ristic of the el
tible to freque
ncy band on e
analysis is the
onstraint cond
lement analys
ry provide stru
ANSDUCER
hich is compo
as shown in Fi
Cymbal transd
s of two piec
(IJRES)
r Differe
Engineering S
er different c
finite elemen
alculation and
he free and no
bration mode
vibration loa
ulation suppo
UENCY, MODE
zoelectric cer
bear large loa
for pressure e
lastic structur
ency range of
external or int
e important m
dition is analy
is software, c
uctural suppor
osed of a piezo
gure 1.
ducer
es of cymbal
ent Wor
Science,Shang
constraint con
nt method, th
d analysis to o
on free condit
and natural f
ad, the load in
ort for energy
E OF VIBRATIO
ramic sheet wi
ad. The cymba
electric cerami
re.. Through t
f each order of
ternal various
method for the
yzed. Accordi
comparative a
rt analysis.
oelectric ceram
l brass metal
5 | Page
king
ghai
nditions of
e Cymbal
obtain the
tions yield
frequency
n order to
y recovery
ON, FINITE
ith
al metal
ic wafer
the modal
f the main
s vibration
structural
ing to the
analysis of
mic sheet,
caps and
Model Analysis of Cymbal Generator Under Different Working Conditions
www.ijres.org 6 | Page
circular piezoelectric ceramic piece by epoxy resin adhesive. The thickness of metal cap is tm;The thickness of
Piezoelectric ceramic plate is tp;The Radius of Top circle of metal cap is R1;The Radius of Inner bottom
circle of metal cap is R2;The Radius of bottom circle of metal cap is R3;The height of Lumen height of metal
cap is h;
2.2 Power generation principle
When the metal cap is subjected to the external axial load, the movement displacement and the radial and
axial stretching of the piezoelectric ceramic piece have a certain functional relationship[2]
. When the external
axial vibration is Cymbal transducer to receiving device of metal end cap and a metal end cap to produce
bending vibration, due to the coupling between the metal end cap and a piezoelectric ceramic disk, external axial
load by metal end caps buffer and converted into electric vibrator radial compressive stress and the vibrator to
produce radial vibration, due to the pressure on the piezoelectric effect of piezoelectric ceramic, alternating
external vibration the cymbal transducer an alternating electric field is generated, which is to achieve the
transformation of the external source of vibration excitation energy[3]
.
Because of its special hollow metal cap structure, which applied in the metal cap on the top end of the axial
stress can conversion of piezoelectric ceramic sheet of radial pressure should force and axial stress, which
makes the d31 and d33 mode piezoelectric constant pressure are equivalent pressure constant play a role, the
effect of pressure dielectric constant is higher than that of single mode under the pressure of piezoelectric
ceramic d31 and d33, d31 radial vibration mode, thus increasing the mechanical and electrical conversion
efficiency[4]
.
III. CYMBAL TRANSDUCER MODALANALYSIS
According to the literatures of[5-6],Taking with structure parameters of piezoelectric constant high
equivalent of Cymbal transducer. Its parameters are as follows: Table 1.
The Metal cap’s material is brass. Piezoelectric ceramic pieces of material is PZT-5H. The Binder between them
is YH-896 which is applies to the bonding of metal and ceramic. It has the advantages of bonding strength,
impact resistance, high temperature resistance, wear resistance and the shock effect is ideal .
3.1 Selection of parameters for adhesive material
In the metal cap and the piezoelectric ceramic binder selection, according to the characteristics of the metal
and ceramic bond and the need of extra high bonding strength, impact resistance, high temperature resistance,
wear resistance, shockproof effect ideal binder. One of the suitable for this is the P-51, P-14, 7-2315 epoxy
adhesive, YH-896 and so on.YH-896 compared with several other binder, with moderate viscosity colloid,
strong tensile strength, shear strength. So choose YH-896 as bonded metal cap and the pressure piezoelectric
electric ceramic material. The material parameters of adhesive YH-896 are listed in Table 1.
2R2
h
2R3
tm
tp
Piezoelectric ceramic plate
Metal cap
Figure 2. Structure display of Cymbal
2R1
Model Analysis of Cymbal Generator Under Different Working Conditions
www.ijres.org 7 | Page
Table 1. Adhesive parameters
Item Parameter Unit
Type YH-896 /
Viscosity 10±5 /
Strength of extension ≥160±10 kg/cm2
Shear strength ≥150±10 kg/cm2
Shelf life 12 months /
Density 980 kg/m3
Curing speed 10-30s /
Modulus of elasticity 2.5 Gpa
Relative permittivity 3 /
Poisson ratio 0.36 /
Note: The above performance data is typical in laboratory environment temperature of 25 degree and the
humidity of 70% of the measured data, only use the customer reference does not guarantee is a particular
environment can reach all the data of the customer please when in use, to test data shall prevail.
For the piezoelectric ceramic transducer are PZT-5A, PZT-5H, PZT-4, PVDF and etc. The PZT-5H compared to
other materials with higher equivalent pressure constant, obtain good positive piezoelectric effect, can obtain
higher energy conversion rate, so in Cymbal transducer can structure select PZT-5H as the pressure of
piezoelectric materials.
3.2 Cymbal transducer material parameters
Phase compared to steel 45#, aluminum alloy, copper and other materials, brass with high stiffness and Young's
modulus, suitable for work in low frequency and high load conditions, and suitable for relatively high
conductivity. Here is a selection of brass as the material of the metal end caps.
By the literatures of [5-6],Under the train running condition of high and low frequency load environment, need
to design appropriate cymbal piezoelectric device structure, so Cymbal transducer can the material parameters
and structural parameters are listed in Table 2.
Table 2. Cymbal transducer parameters
Parameter Item Unit
Metal cap PZT-5H
Density ρ 8900 7500 Kg/m3
Poisson ratio μ 0.35 0.28 /
Modulus of elasticity 112 102 Gpa
Radius of bottom circle 15 15 mm
Radius of Top circle Top
circle diameter
4 / mm
Radius of Inner bottom circle 12 / mm
Height of Lumen 0.3 / mm
Thickness of Metal cap 0.4 / mm
thickness of PZT-5H / 1 mm
Thermal conductivity / 1.5 W/(m·k)
perm
const
flexible
Note: the
Mod
natural fr
and spect
Modal an
system’s
other dyn
and will b
ensure th
mode of p
4.1 The e
4.2 Defin
Accordin
of materi
number)
Item
Relative
mittivity matrix
0


 
  
 
Piezoelectric
tant matrix d
 
Piezoelectric
e constant mat
 s
e vacuum or st
dal analysis is
requencies an
trum analysis
nalysis is use
basic modes
namic analysis
be the first or
hat the energy
prisoners to th
establishmen
ne material p
ng to the priso
ial property p
value of 6. In
Model Ana
x 
c
d  
c
trix
tatic permittiv
IV. M
s used to ana
d vibration m
and the other
d to determin
and natural fr
s based. Will
rder mode and
harvesting de
he response ha
nt and calcula
Figure 3. Cy
roperties and
oners in front
parameters, se
n the mesh in t
alysis of Cym
w
Table 3. PZ
0
0
171




16.4
5.74 1
7.22 7
0
0
0



 





vity of 0 on t
MODALANA
lyze the vibra
modes of the st
dynamics ana
ne the natural
requencies is t
usually design
d other modes
evice for the s
as important i
ation of the fin
ymbal transduc
d set paramet
of the cymba
election of An
the properties
mbal Gener
www.ijres.org
ZT5-H piezoel
Paramete
1730 0
0 1730
0 0





0 0
0 0
171 374
5.74 7.22
16.4 7.22
7.22 18.8
0 0
0 0
0 0


the upper table
ALYSIS OF CY
ation characte
tructure, it is
alysis based.
frequency of
transient dyna
ners need to t
of vibration f
stability of the
influence.
nite element
cer sub entity
ters
al is the defini
nalysis Settin
grid settings f
rator Under
g
lectric parame
er
0
0 0
1730





0 584
584 0
0 0
0 0
0 0
0 0
47.5 0
0 47.5
0 0
e is vacuum. 
YMBAL TRAN
eristics of the
the harmonic
f the system a
amic analysis,
the vibration m
frequency inte
e structure, an
model of Cym
model and gr
ition of mater
ngs set Max m
for fine.
r Different W
eters
0
0
0





0
0
0
0
0
47.5









0 8.85 10 
 
NSDUCER
e structure, th
response anal
and correspon
, harmonic res
mode of the de
erval as far as
nd the resonan
mbal transdu
rid model diag
rial parameter
modes to find
Working Co
Un
/
10-12
10-12
12
/F m
hat is, to dete
alysis, dynami
nding mode sh
sponse analys
esign for the f
possible to in
nt frequency o
ucer
gram
rs, finite eleme
d (the maximu
onditions
8 | Page
nit
/
2
C/N
m/V
rmine the
c analysis
hapes, the
sis and the
first mode
ncrease, to
of the first
ent model
um modal
4.2.1 Nat
With the
with AN
and the f
reduce th
the vibra
shown in
Because
algorithm
results ar
Because
follows.
tural frequen
Cymbal trans
SYS and sim
finite element
he size of the n
ation energy o
n Figure 4 and
Order
1
2
3
4
5
6
of the differ
m, resulting in
re basically th
in practice, th
Model Ana
ncy of free sta
sducer under f
mulation by 10
t method is ca
natural freque
of Cymbal tra
d table 4.The m
-0.002
0.000
0.002
0.004
0.006
0.008
0.010
0.012
0.014
0.016
0.018
naturalfrequencies(Hz)
Fi
T
rence between
n these two sof
e same, in the
he reference v
alysis of Cym
w
ate
free state, wit
0 times analys
arried out vib
ency can effec
ansducer. The
mode state is s
1 2
SIMULA
ANSYS
igure 4. Resul
Table 4. Natur
SIMULATI
0
0
3.3539
0.002
0.003
0.003
n those two
ftware in anal
e realistic envi
value is more
mbal Gener
www.ijres.org
thout any cons
sis mean value
bration modal
ctively use the
e modal analy
shown in Figu
3 Orde
ATION
lts of modal an
ural frequenci
ION(Hz)
0
0
9e-009
23546
32262
32324
software of
lysis of natura
ironment of th
of the fourth
rator Under
g
straints, only
es obtained n
analysis, mo
e vertical reson
ysis of the firs
ure 5.
4 5er
nalysis in free
ies of a free
finite elemen
al frequency d
hird order freq
order, so only
r Different W
analysis of or
atural frequen
odal shape and
nance capture
st order to th
5 6
e state
state
AN
5
8.
nt calculation
ifferences, in
quency is more
y a fourth of t
Working Co
rder 6. After s
ncies of moda
d natural freq
e as much as p
he sixth order
NSYS(Hz)
0
5.8906e-003
.0661e-003
0.0134
0.0195
0.0209
n method of
the first three
e significance
the first four
onditions
9 | Page
simulation
al analysis
quency of,
possible to
modes is
immanent
e order the
e.
modes, as
In the fre
actual en
of non fre
4.2.2 Non
Practical
vibration
free state
belongs t
stacked g
Finite ele
stress yie
ee state, press
nvironment, pi
ee state constr
n free state
working env
n, therefore de
e, do not impo
to cap defined
gravity load.
ement calculat
eld limit and th
Model Ana
Figure 5. Vi
sure electric d
iezoelectric vi
raint modal an
vironment, pi
efined constrai
ose any constr
d as rigid conn
tions, as show
he stress in th
Figure 6. Mo
alysis of Cym
ww
ibration state o
dipole resonan
ibrator is in a
nalysis more r
iezoelectric s
ints is fixed u
aints, on the m
nection, the lo
wn in Figure 7
e safety range
ode shapes of t
mbal Gener
ww.ijres.org
of the first to
nce frequency
non free state
reference sign
streak in the
under the botto
metal cap, pre
oad was appli
and table 5. A
e of the brass.
the first to fou
rator Under
fourth mode u
y is low, four
e, exist a serie
nificance.
circular groo
om of the met
essure PZT-5H
ed on the met
According to t
urth mode und
r Different W
under free stat
steps were be
s of constrain
ove by vertic
tal cap constr
H piezoelectric
tal crown roun
the results of t
der non free st
Working Co
te
elow 100Hz,
nts. Therefore,
cal load, und
raints and othe
c ceramics and
nd face, load
the data in Fig
tate
onditions
10 | Page
but in the
the study
der forced
er parts in
d the gold
190N and
gure 6, the
Model Analysis of Cymbal Generator Under Different Working Conditions
www.ijres.org 11 | Page
1 2 3 4 5 6
0
2000
4000
6000
8000
10000
naturalfrequencies(Hz)
Order
SIMULATION
ANSYS
Figure 7. Results of modal analysis
Table 5. Results of modal analysis
Order SIMULATION(Hz) ANSYS(Hz)
1 1168.4 1629.7
2 1171.2 1645.5
3 2062 2716.2
4 7468.4 8955.6
5 8387.7 9293.4
6 8721.6 9296.6
In the ree state, two software simulation results have little difference. Between 7% - 12%, pressure of the first
order natural frequency of the electric dipole reached 1168.4Hz, and in the actual environment, environmental
vibration frequency multi around 100Hz and reduce harvesting is first-order natural frequency of the natural
frequency at or near ambient vibration frequency on the vibration of energy recovery has important significance.
V. CONCLUSION
The cymbal piezoelectric device as the rail vibration energy recovery technology as a new confession of
micro energy, will be able to train running environment of track vertical to the vibration energy conversion into
electrical energy, as some low power electronic components and sensor power supply, has important theoretical
significance and economic value in use. In this paper, an important unit of the Cymbal piezoelectric energy
recovery technology is a finite element study.
The finite element method and ANSYS workbench14.0 software, simulation software to analyze the design of
Cymbal transducer is, and analysis the first vibration modal and calculate the resonant frequency. Maximum
average displacement amplitude of the actual working condition of the first order vibration mode, with two
software calculation for resonant frequency compared, the relative deviation of less than 7. 00% its resonance
frequency 1168.4Hz, far higher than the actual environment vibration frequency. Experimental results show that
the engineering application significance to solve the Cymbal transducer. To get a good piezoelectric effect,
should be optimized in haversters results.
REFERENCE
[1] Wang Guangcan, Wang Likun, Li Guang, Luan Guidong, Zhang Fuxue. (2004) Study on Material Constants and
Electromechanical Characteristics of Cymbal Transducer [J]. Electronic Components & Materials, No.10,pp.33-35.
[2] Gao Quanqin. (2012) Analysis of Influencing Factors of Equivalent Piezoelectric Constant of Cymbal Piezoelectric Transducer [J].
Piezoelectrics & Acoustooptics,No.03,pp. 388-391.
[3] Lu Yigang,Yan Zhengfang. (2013) Finite element analysis on energy harvesting with cymbal transducer [J].Journal of Vibration
and Shock ,No.06,pp. 157-162.
[4] Ma Yongcheng,Li Denghua. (2006) Analysis of Cymbal Piezocomposite transduer’s effective Piezoelectric coefficients based on
ANSYS [J]. Chinese Journal of Scientific Instrument, No.S2,pp. 1313-1315.
[5] Yuan Jiangbo. (2011) Power Generation and Pivotal Technique of Discal Energy Harvester [D]. Harbin Institute of Technology.
Model Analysis of Cymbal Generator Under Different Working Conditions
www.ijres.org 12 | Page
[6] Guo Shuai. (2012) Analysis of Cymbal piezoelectric generator's effective piezoelectric strain constant [J]. Journal of Mechanical &
Electrical Engineering, No.04,pp. 443-446.
Authors
Corresponding author: Shi Yan-chao (1988-), male, master of vehicle engineering, research direction for Energy recovery of vertical
vibration of trains.E-mail: sandide2013@163.com
Acknowledgements
This work was supported by the Graduate student research innovation project of Shanghai University Of Engineering Science(E1-
0903-14-01176)and the Innovation Program of Shanghai Municipal Education Commission(14ZZ158).

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Model Analysis of Cymbal Generator Under Different Working Conditions

  • 1. Interna ISSN (O www.ijr Mod Co ABSTRA Cymbal transduce modal un stress lim shows th study, un applicati KEYWO ELEMENT Cym bonding p caps can of high im The vibr analysis m modal ch sources o dynamic In this p boundary Cymbal t Cym epoxy res 2.1 Intr As show tional Journ Online): 232 res.org Volu del Anal ollege of Urba ACT : In ord transducer. T er can be app nder the specif mits are in th at suitable fo nder low frequ ions. ORDS CYMBA T METHOD mbal transduce pressure of co be low imped mpedance, the ration mode is method which haracteristics c of the actual v design and th paper the Cym y stress constr transducer can mbal transduce sin and metal oduction ab wn in section nal of Resea 20-9364, ISS ume 3 Issue ysis of C an Railway Tr der to study t Through the u plied on differ ific natural fre e security do or large load uency vibratio AL TRANSDUCE er is made up b ombination wh dance, high be e path toward s the inherent h can figure o can be predict vibration respo he fault diagno mbal transduc raints, the mo n device of tra er is a miniatu end cap struc Fig bout the con view 2, the arch in Eng SN (Print): 6 ǁ June 20 w Cymbal G C Shi Yanc ransportation the influence f use of ANSYS rent constrain equencies and main, the mo under low fre on Cymbal tr ER , MODEL A I. by two cymba hich has small ending axial de the expansion t and the ove ut the structur ted structure i onse. Therefor osis of the equ cer can under odal analysis u ain vibration e II. C urized V crook ture, the 3D e gure 1. 3D ent struction Cymbal harv gineering an 2320-9356 015 ǁ PP.05- www.ijres.org Generato Condition chao and Y of Shanghai U 201620,China for natural fr S and SIMUL nts and load c d mode shape odal analysis equency vibra ransducer can ANALYSIS, INH INTRODU al shaped meta l volume, ligh eformation tra n deformation erall character re in a suscep in this frequen re, the modal uipment. r the force co using finite el energy recover CYMBAL TRA ked device wh entity model a tity model of C ester consists nd Science ( 6 12 g or Unde ns Yang Jian University of E a frequency und LATION with conditions, ca s. Which in th results of vib ation of train n provide sim HERENT FREQU CTION al cap and pie ht weight, can ansformation n[1] . ristic of the el tible to freque ncy band on e analysis is the onstraint cond lement analys ry provide stru ANSDUCER hich is compo as shown in Fi Cymbal transd s of two piec (IJRES) r Differe Engineering S er different c finite elemen alculation and he free and no bration mode vibration loa ulation suppo UENCY, MODE zoelectric cer bear large loa for pressure e lastic structur ency range of external or int e important m dition is analy is software, c uctural suppor osed of a piezo gure 1. ducer es of cymbal ent Wor Science,Shang constraint con nt method, th d analysis to o on free condit and natural f ad, the load in ort for energy E OF VIBRATIO ramic sheet wi ad. The cymba electric cerami re.. Through t f each order of ternal various method for the yzed. Accordi comparative a rt analysis. oelectric ceram l brass metal 5 | Page king ghai nditions of e Cymbal obtain the tions yield frequency n order to y recovery ON, FINITE ith al metal ic wafer the modal f the main s vibration structural ing to the analysis of mic sheet, caps and
  • 2. Model Analysis of Cymbal Generator Under Different Working Conditions www.ijres.org 6 | Page circular piezoelectric ceramic piece by epoxy resin adhesive. The thickness of metal cap is tm;The thickness of Piezoelectric ceramic plate is tp;The Radius of Top circle of metal cap is R1;The Radius of Inner bottom circle of metal cap is R2;The Radius of bottom circle of metal cap is R3;The height of Lumen height of metal cap is h; 2.2 Power generation principle When the metal cap is subjected to the external axial load, the movement displacement and the radial and axial stretching of the piezoelectric ceramic piece have a certain functional relationship[2] . When the external axial vibration is Cymbal transducer to receiving device of metal end cap and a metal end cap to produce bending vibration, due to the coupling between the metal end cap and a piezoelectric ceramic disk, external axial load by metal end caps buffer and converted into electric vibrator radial compressive stress and the vibrator to produce radial vibration, due to the pressure on the piezoelectric effect of piezoelectric ceramic, alternating external vibration the cymbal transducer an alternating electric field is generated, which is to achieve the transformation of the external source of vibration excitation energy[3] . Because of its special hollow metal cap structure, which applied in the metal cap on the top end of the axial stress can conversion of piezoelectric ceramic sheet of radial pressure should force and axial stress, which makes the d31 and d33 mode piezoelectric constant pressure are equivalent pressure constant play a role, the effect of pressure dielectric constant is higher than that of single mode under the pressure of piezoelectric ceramic d31 and d33, d31 radial vibration mode, thus increasing the mechanical and electrical conversion efficiency[4] . III. CYMBAL TRANSDUCER MODALANALYSIS According to the literatures of[5-6],Taking with structure parameters of piezoelectric constant high equivalent of Cymbal transducer. Its parameters are as follows: Table 1. The Metal cap’s material is brass. Piezoelectric ceramic pieces of material is PZT-5H. The Binder between them is YH-896 which is applies to the bonding of metal and ceramic. It has the advantages of bonding strength, impact resistance, high temperature resistance, wear resistance and the shock effect is ideal . 3.1 Selection of parameters for adhesive material In the metal cap and the piezoelectric ceramic binder selection, according to the characteristics of the metal and ceramic bond and the need of extra high bonding strength, impact resistance, high temperature resistance, wear resistance, shockproof effect ideal binder. One of the suitable for this is the P-51, P-14, 7-2315 epoxy adhesive, YH-896 and so on.YH-896 compared with several other binder, with moderate viscosity colloid, strong tensile strength, shear strength. So choose YH-896 as bonded metal cap and the pressure piezoelectric electric ceramic material. The material parameters of adhesive YH-896 are listed in Table 1. 2R2 h 2R3 tm tp Piezoelectric ceramic plate Metal cap Figure 2. Structure display of Cymbal 2R1
  • 3. Model Analysis of Cymbal Generator Under Different Working Conditions www.ijres.org 7 | Page Table 1. Adhesive parameters Item Parameter Unit Type YH-896 / Viscosity 10±5 / Strength of extension ≥160±10 kg/cm2 Shear strength ≥150±10 kg/cm2 Shelf life 12 months / Density 980 kg/m3 Curing speed 10-30s / Modulus of elasticity 2.5 Gpa Relative permittivity 3 / Poisson ratio 0.36 / Note: The above performance data is typical in laboratory environment temperature of 25 degree and the humidity of 70% of the measured data, only use the customer reference does not guarantee is a particular environment can reach all the data of the customer please when in use, to test data shall prevail. For the piezoelectric ceramic transducer are PZT-5A, PZT-5H, PZT-4, PVDF and etc. The PZT-5H compared to other materials with higher equivalent pressure constant, obtain good positive piezoelectric effect, can obtain higher energy conversion rate, so in Cymbal transducer can structure select PZT-5H as the pressure of piezoelectric materials. 3.2 Cymbal transducer material parameters Phase compared to steel 45#, aluminum alloy, copper and other materials, brass with high stiffness and Young's modulus, suitable for work in low frequency and high load conditions, and suitable for relatively high conductivity. Here is a selection of brass as the material of the metal end caps. By the literatures of [5-6],Under the train running condition of high and low frequency load environment, need to design appropriate cymbal piezoelectric device structure, so Cymbal transducer can the material parameters and structural parameters are listed in Table 2. Table 2. Cymbal transducer parameters Parameter Item Unit Metal cap PZT-5H Density ρ 8900 7500 Kg/m3 Poisson ratio μ 0.35 0.28 / Modulus of elasticity 112 102 Gpa Radius of bottom circle 15 15 mm Radius of Top circle Top circle diameter 4 / mm Radius of Inner bottom circle 12 / mm Height of Lumen 0.3 / mm Thickness of Metal cap 0.4 / mm thickness of PZT-5H / 1 mm Thermal conductivity / 1.5 W/(m·k)
  • 4. perm const flexible Note: the Mod natural fr and spect Modal an system’s other dyn and will b ensure th mode of p 4.1 The e 4.2 Defin Accordin of materi number) Item Relative mittivity matrix 0          Piezoelectric tant matrix d   Piezoelectric e constant mat  s e vacuum or st dal analysis is requencies an trum analysis nalysis is use basic modes namic analysis be the first or hat the energy prisoners to th establishmen ne material p ng to the priso ial property p value of 6. In Model Ana x  c d   c trix tatic permittiv IV. M s used to ana d vibration m and the other d to determin and natural fr s based. Will rder mode and harvesting de he response ha nt and calcula Figure 3. Cy roperties and oners in front parameters, se n the mesh in t alysis of Cym w Table 3. PZ 0 0 171     16.4 5.74 1 7.22 7 0 0 0           vity of 0 on t MODALANA lyze the vibra modes of the st dynamics ana ne the natural requencies is t usually design d other modes evice for the s as important i ation of the fin ymbal transduc d set paramet of the cymba election of An the properties mbal Gener www.ijres.org ZT5-H piezoel Paramete 1730 0 0 1730 0 0      0 0 0 0 171 374 5.74 7.22 16.4 7.22 7.22 18.8 0 0 0 0 0 0   the upper table ALYSIS OF CY ation characte tructure, it is alysis based. frequency of transient dyna ners need to t of vibration f stability of the influence. nite element cer sub entity ters al is the defini nalysis Settin grid settings f rator Under g lectric parame er 0 0 0 1730      0 584 584 0 0 0 0 0 0 0 0 0 47.5 0 0 47.5 0 0 e is vacuum.  YMBAL TRAN eristics of the the harmonic f the system a amic analysis, the vibration m frequency inte e structure, an model of Cym model and gr ition of mater ngs set Max m for fine. r Different W eters 0 0 0      0 0 0 0 0 47.5          0 8.85 10    NSDUCER e structure, th response anal and correspon , harmonic res mode of the de erval as far as nd the resonan mbal transdu rid model diag rial parameter modes to find Working Co Un / 10-12 10-12 12 /F m hat is, to dete alysis, dynami nding mode sh sponse analys esign for the f possible to in nt frequency o ucer gram rs, finite eleme d (the maximu onditions 8 | Page nit / 2 C/N m/V rmine the c analysis hapes, the sis and the first mode ncrease, to of the first ent model um modal
  • 5. 4.2.1 Nat With the with AN and the f reduce th the vibra shown in Because algorithm results ar Because follows. tural frequen Cymbal trans SYS and sim finite element he size of the n ation energy o n Figure 4 and Order 1 2 3 4 5 6 of the differ m, resulting in re basically th in practice, th Model Ana ncy of free sta sducer under f mulation by 10 t method is ca natural freque of Cymbal tra d table 4.The m -0.002 0.000 0.002 0.004 0.006 0.008 0.010 0.012 0.014 0.016 0.018 naturalfrequencies(Hz) Fi T rence between n these two sof e same, in the he reference v alysis of Cym w ate free state, wit 0 times analys arried out vib ency can effec ansducer. The mode state is s 1 2 SIMULA ANSYS igure 4. Resul Table 4. Natur SIMULATI 0 0 3.3539 0.002 0.003 0.003 n those two ftware in anal e realistic envi value is more mbal Gener www.ijres.org thout any cons sis mean value bration modal ctively use the e modal analy shown in Figu 3 Orde ATION lts of modal an ural frequenci ION(Hz) 0 0 9e-009 23546 32262 32324 software of lysis of natura ironment of th of the fourth rator Under g straints, only es obtained n analysis, mo e vertical reson ysis of the firs ure 5. 4 5er nalysis in free ies of a free finite elemen al frequency d hird order freq order, so only r Different W analysis of or atural frequen odal shape and nance capture st order to th 5 6 e state state AN 5 8. nt calculation ifferences, in quency is more y a fourth of t Working Co rder 6. After s ncies of moda d natural freq e as much as p he sixth order NSYS(Hz) 0 5.8906e-003 .0661e-003 0.0134 0.0195 0.0209 n method of the first three e significance the first four onditions 9 | Page simulation al analysis quency of, possible to modes is immanent e order the e. modes, as
  • 6. In the fre actual en of non fre 4.2.2 Non Practical vibration free state belongs t stacked g Finite ele stress yie ee state, press nvironment, pi ee state constr n free state working env n, therefore de e, do not impo to cap defined gravity load. ement calculat eld limit and th Model Ana Figure 5. Vi sure electric d iezoelectric vi raint modal an vironment, pi efined constrai ose any constr d as rigid conn tions, as show he stress in th Figure 6. Mo alysis of Cym ww ibration state o dipole resonan ibrator is in a nalysis more r iezoelectric s ints is fixed u aints, on the m nection, the lo wn in Figure 7 e safety range ode shapes of t mbal Gener ww.ijres.org of the first to nce frequency non free state reference sign streak in the under the botto metal cap, pre oad was appli and table 5. A e of the brass. the first to fou rator Under fourth mode u y is low, four e, exist a serie nificance. circular groo om of the met essure PZT-5H ed on the met According to t urth mode und r Different W under free stat steps were be s of constrain ove by vertic tal cap constr H piezoelectric tal crown roun the results of t der non free st Working Co te elow 100Hz, nts. Therefore, cal load, und raints and othe c ceramics and nd face, load the data in Fig tate onditions 10 | Page but in the the study der forced er parts in d the gold 190N and gure 6, the
  • 7. Model Analysis of Cymbal Generator Under Different Working Conditions www.ijres.org 11 | Page 1 2 3 4 5 6 0 2000 4000 6000 8000 10000 naturalfrequencies(Hz) Order SIMULATION ANSYS Figure 7. Results of modal analysis Table 5. Results of modal analysis Order SIMULATION(Hz) ANSYS(Hz) 1 1168.4 1629.7 2 1171.2 1645.5 3 2062 2716.2 4 7468.4 8955.6 5 8387.7 9293.4 6 8721.6 9296.6 In the ree state, two software simulation results have little difference. Between 7% - 12%, pressure of the first order natural frequency of the electric dipole reached 1168.4Hz, and in the actual environment, environmental vibration frequency multi around 100Hz and reduce harvesting is first-order natural frequency of the natural frequency at or near ambient vibration frequency on the vibration of energy recovery has important significance. V. CONCLUSION The cymbal piezoelectric device as the rail vibration energy recovery technology as a new confession of micro energy, will be able to train running environment of track vertical to the vibration energy conversion into electrical energy, as some low power electronic components and sensor power supply, has important theoretical significance and economic value in use. In this paper, an important unit of the Cymbal piezoelectric energy recovery technology is a finite element study. The finite element method and ANSYS workbench14.0 software, simulation software to analyze the design of Cymbal transducer is, and analysis the first vibration modal and calculate the resonant frequency. Maximum average displacement amplitude of the actual working condition of the first order vibration mode, with two software calculation for resonant frequency compared, the relative deviation of less than 7. 00% its resonance frequency 1168.4Hz, far higher than the actual environment vibration frequency. Experimental results show that the engineering application significance to solve the Cymbal transducer. To get a good piezoelectric effect, should be optimized in haversters results. REFERENCE [1] Wang Guangcan, Wang Likun, Li Guang, Luan Guidong, Zhang Fuxue. (2004) Study on Material Constants and Electromechanical Characteristics of Cymbal Transducer [J]. Electronic Components & Materials, No.10,pp.33-35. [2] Gao Quanqin. (2012) Analysis of Influencing Factors of Equivalent Piezoelectric Constant of Cymbal Piezoelectric Transducer [J]. Piezoelectrics & Acoustooptics,No.03,pp. 388-391. [3] Lu Yigang,Yan Zhengfang. (2013) Finite element analysis on energy harvesting with cymbal transducer [J].Journal of Vibration and Shock ,No.06,pp. 157-162. [4] Ma Yongcheng,Li Denghua. (2006) Analysis of Cymbal Piezocomposite transduer’s effective Piezoelectric coefficients based on ANSYS [J]. Chinese Journal of Scientific Instrument, No.S2,pp. 1313-1315. [5] Yuan Jiangbo. (2011) Power Generation and Pivotal Technique of Discal Energy Harvester [D]. Harbin Institute of Technology.
  • 8. Model Analysis of Cymbal Generator Under Different Working Conditions www.ijres.org 12 | Page [6] Guo Shuai. (2012) Analysis of Cymbal piezoelectric generator's effective piezoelectric strain constant [J]. Journal of Mechanical & Electrical Engineering, No.04,pp. 443-446. Authors Corresponding author: Shi Yan-chao (1988-), male, master of vehicle engineering, research direction for Energy recovery of vertical vibration of trains.E-mail: sandide2013@163.com Acknowledgements This work was supported by the Graduate student research innovation project of Shanghai University Of Engineering Science(E1- 0903-14-01176)and the Innovation Program of Shanghai Municipal Education Commission(14ZZ158).