T60004-L2130-W587 [ETC]
NaNOcRysTallINE VITROPERM;型号: | T60004-L2130-W587 |
厂家: | ETC |
描述: | NaNOcRysTallINE VITROPERM |
文件: | 总16页 (文件大小:4474K) |
中文: | 中文翻译 | 下载: | 下载PDF数据表文档文件 |
NaNOcRysTallINE
VITROPERM
EMc PROducTs
adVaNcEd MaTERIals – THE KEy TO PROGREss
NaNOcRysTallINE
VITROPERM
EMc PROducTs
VacuuMscHMElZE GmbH & co. KG (Vac)
iꢀ ꢁ ꢂeꢁꢃing gꢂobꢁꢂ mꢁnꢄfꢁꢅtꢄrer of moꢃern
mꢁgnetiꢅ ꢁꢂꢂoꢆꢀ, ꢅoreꢀ ꢁnꢃ inꢃꢄꢅtive ꢅompo-
nentꢀ. Vac hꢁꢀ ꢀꢄppꢂieꢃ innovꢁtive ꢀoꢂꢄtionꢀ
for eꢂeꢅtromꢁgnetiꢅ ꢅompꢁtibiꢂitꢆ (EMc) pro-
teꢅtion for more thꢁn 30 ꢆeꢁrꢀ.
2
NaNOcRysTallINE VITROPERM / EMc PROducTs
VITROPERM :
extending the possibilities of iron
Nꢁnoꢅrꢆꢀtꢁꢂꢂine VITROPERM ꢁꢂꢂoꢆꢀ ꢁre bꢁꢀeꢃ on Fe with si ꢁnꢃ B with Nb ꢁnꢃ cꢄ ꢁꢃꢃi-
tiveꢀ. Vac pioneereꢃ the ꢃeveꢂopment of rꢁpiꢃ ꢀoꢂiꢃifiꢅꢁtion teꢅhnoꢂogꢆ reꢀꢄꢂting in the
proꢃꢄꢅtion of thin tꢁpeꢀ or ribbonꢀ ꢁpproximꢁteꢂꢆ 20 μm thiꢅk. speꢅiꢁꢂ ꢀꢂitting ꢁnꢃ ꢅore
winꢃing mꢁꢅhineꢀ proꢃꢄꢅe tꢁpe-woꢄnꢃ ꢅoreꢀ with externꢁꢂ ꢃiꢁmeterꢀ rꢁnging from 2
mm to 600 mm. a ꢀꢄbꢀeqꢄent heꢁt treꢁtment ꢁt ꢁroꢄnꢃ 500 – 600 °c trꢁnꢀformꢀ the ini-
tiꢁꢂꢂꢆ ꢁmorphoꢄꢀ miꢅroꢀtrꢄꢅtꢄre of the tꢁpe into the ꢃeꢀireꢃ nꢁnoꢅrꢆꢀtꢁꢂꢂine ꢀtꢁte. Thiꢀ
being ꢁ two-phꢁꢀe ꢀtrꢄꢅtꢄre with fine ꢅrꢆꢀtꢁꢂꢂine grꢁinꢀ (ꢁverꢁge grꢁin ꢃiꢁmeter of 10-40
nm) embeꢃꢃeꢃ in ꢁn ꢁmorphoꢄꢀ reꢀiꢃꢄꢁꢂ phꢁꢀe.
VITROPERM nanocrystalline alloys are optimized to
combine highest permeability and lowest coercive
field strength. The combination of very thin tapes and
the relatively high electrical resistance (1.1 – 1.2
μΩm) ensure minimal eddy current losses and an
outstanding frequency vs. permeability behaviour.
Along with saturation flux density of 1.2 T and wide
operational temperature range, these features com-
bine to make VITROPERM a universal solution for
most common EMC problems and vastly superior in
many aspects to commonly used ferrite and amor-
phous iron materials.
Fig.1:Rapidsolidificationtechnologyisusedtoproducethinmetaltapeswithanamorphousstructure(metallicglass).
Fig2:Crystallinestructure,amorphousstructure,nanocrystallinemicrostructure
NaNOcRysTallINE VITROPERM / EMc PROducTs
3
cꢀmmꢀꢁ mꢀꢂꢃ
cꢄꢀkꢃꢅ &
tape-wound ꢆores
Nꢁnoꢅrꢆꢀtꢁꢂꢂine ꢅoreꢀ ꢁre wiꢃeꢂꢆ ꢄꢀeꢃ in ꢅommon moꢃe ꢅhoke (cMc) ꢁppꢂiꢅꢁtionꢀ ꢃꢄe to their ꢄniqꢄe
ꢅombinꢁtion of propertieꢀ. Bꢆ ꢄtiꢂiꢀing ꢂow-ꢅoꢀt rꢁw mꢁteriꢁꢂꢀ (Fe-bꢁꢀeꢃ) ꢁnꢃ moꢃern, ꢂꢁrge-ꢀꢅꢁꢂe pro-
ꢃꢄꢅtion, VITROPERM iꢀ ꢁ verꢆ ꢅompetitive ꢀoꢂꢄtion for ꢁ wiꢃe rꢁnge of ꢁppꢂiꢅꢁtionꢀ. Keꢆ ꢁreꢁꢀ of ꢁppꢂi-
ꢅꢁtion ꢁre:
• switꢅheꢃ-moꢃe
power ꢀꢄppꢂieꢀ (sMPs)
Our CMCs feature high attenuation which is
maintained across a wide frequency range offe-
• soꢂꢁr inverterꢀ
ring extremely broadband attenuation. In many
cases, this characteristic can allow a reduction
• Freqꢄenꢅꢆ ꢅonverterꢀ
of the number of filter stages in multistage EMC
filter configurations to reduce complexity, cost
• EMc fiꢂterꢀ
and filter volume. Ohmic (copper) losses are
also reduced increasing the efficiency and lowe-
• Weꢂꢃing eqꢄipment
ring component temperature.
• Winꢃ generꢁtorꢀ
stꢁnꢃꢁrꢃ 2-ꢀtꢁge EMI-Fiꢂter Optimizeꢃ 1-ꢀtꢁge EMc-Fiꢂ-
ter with VITROPERM
• Inꢃꢄꢅtion hobꢀ
• aꢄtomotive ꢁppꢂiꢅꢁtionꢀ
• uninterrꢄptꢁbꢂe
power ꢀꢄppꢂieꢀ (uPs)
NF stꢁge
HF stꢁge
Fig.3:Nanocrystallinechokesallowareductionoffilterstages
50
40
30
20
10
0
VACUUMSCHMELZE has extensive practical and theo-
retical expertise in the design of CMCs and filter confi-
guration using nanocrystalline cores and components.
At higher frequencies, the winding configuration has a
major effect on the parameters of winding capacitance
and leakage inductance and is therefore carefully con-
sidered in our choke designs. Figure 4 shows a compa-
rison of insertion loss for two chokes which differ only
in their winding configuration (core material, number of
turns and wire thickness are identical in both cases).
This illustrates how our design expertise can improve
filter efficiency, maximize reliability and reduce costs.
1-phase CMC
Core: VITROPERM 500F
25 x 20 x 10mm
N = 2 x 28 turns
(0.71mm / AWG 21)
separator: 5 mm
HF optimized winding
design, Cw = 4pF
16dB
simple winding
design, CW=21pF
0.001
0.01
0.1
1
10
frequency [MHz]
Fig. 4:Optimizedchokedesign:improvedattenuationofupto16dB(ormore)at4MHz.
4
NaNOcRysTallINE VITROPERM / EMc PROducTs
Features & benefits
of VITRꢀPꢃRm
nanoꢆrystalline ꢆhoꢇes
High μ, high B
• smꢁꢂꢂ ꢀize
s
High μ, high B , suitable core geometries
s
• sꢄitꢁbꢂe for high ꢅꢄrrentꢀ
ꢁnꢃ/or high voꢂtꢁgeꢀ
Extremely broadband attenuation behaviour,
high permeability, low-capacitance design,
moderate reduction of μ up to high frequen-
cies, low Q-factor in 150 kHz range
• singꢂe ꢀtꢁge fiꢂter ꢃeꢀignꢀ poꢀꢀibꢂe
Low number of turns required for high L,
reduction of filter stages
• High effiꢅienꢅꢆ, ꢂow power ꢂoꢀꢀ
• "Green“, environmentꢁꢂꢂꢆ frienꢃꢂꢆ
Low power loss, reduced use of material
High Curie temperature, material properties
(μ, Bs, λs) nearly independent of temperature
• sꢄitꢁbꢂe for high ꢁnꢃ ꢂow ꢁmbient
temperꢁtꢄreꢀ ꢁnꢃ high operꢁting
temperꢁtꢄreꢀ
Material properties (μ, B , λ) nearly indepen-
• “Eꢁꢀꢆ fiꢂter ꢃeꢀign”
s s
dent of temperature, linear magnetization curve
delivers stable impedance across a broad
range of common mode currents – VAC choke
design software available
• ul-ꢅompꢂiꢁnt ꢃeꢀignꢀ
Suitable plastic materials meet UL1446 insula-
tion requirements
• Optimizeꢃ ꢀoꢂꢄtionꢀ for ꢁ vꢁrietꢆ
of ꢃifferent ꢁppꢂiꢅꢁtionꢀ
A range of μ levels and VITROPERM alloys
available
• No operꢁting noiꢀe
Material is practically magnetostriction-free
• Beꢀt ꢀꢄiteꢃ for winꢃing of thiꢅk wireꢀ
Material is practically magnetostriction-free,
coatings/casings are resistant against mecha-
nical stress
NaNOcRysTallINE VITROPERM / EMc PROducTs
5
VITROPERM
vs. ferrite
dꢄe to the optimizeꢃ high-freqꢄenꢅꢆ propertieꢀ the inꢀertion ꢂoꢀꢀ of oꢄr
nꢁnoꢅrꢆꢀtꢁꢂꢂine ꢅommon moꢃe ꢅhokeꢀ iꢀ ꢀꢄperior ꢅompꢁreꢃ to thꢁt of
ꢁ tꢆpiꢅꢁꢂ ferrite ꢅhoke in the reꢂevꢁnt freqꢄenꢅꢆ rꢁnge.
50
1- phase CMC, core:
25 x 20 x 10 mm (VITROPERM)
25 x 15 x 10 mm (ferrite)
VITROPERM CMC
40
30
20
The properties of VITROPERM are very much diffe-
rent from conventional ferrites. This has to be consi-
dered in the filter design for optimal solutions. The
main physical and magnetic characteristics are illus-
trated in the following diagrams.
10
typical ferrite CMC
0
0.001
0.01
0.1
1
10
frequency [MHz]
Fig.5:ComparisonofinsertionlossofVITROPERMandferrite
permeꢁbiꢂitꢆ
100,000
VITROPERM 500F
The permeability of VITROPERM 500F is signifi-
cantly higher than ferrite in the low frequency range.
At higher frequencies the μ of both nanocrystalline
materials remains above that of ferrites. A high
choke impedance is preferred for a high attenuation.
This can be achieved more effectively by using high
permeability core materials than by increasing the
number of turns, as a lower number of turns results
in lower winding capacitance and hence improved
HF properties.
10,000
1,000
100
VITROPERM 250F
typical Mn-Zn ferrite
10
0.001
0.01
0.1
1
10
100
frequency [MHz]
Fig. 6: Frequency response of the permeability of VITROPERM 500F (μ=40 000) and VITROPERM 250F
(μ=5000)incomparisontoatypicalMnZnferrite(μ=5000).
6
NaNOcRysTallINE VITROPERM / EMc PROducTs
Permeꢁbiꢂitꢆ
& ꢈagnetization ꢆurve
100,000
10,000
1,000
100
VITROPERM 500F, !=100 000
The frequency dependence of the permeability, μ(f)
of VITROPERM 500F and ferrites differ fundamen-
tally. μ(f) of μ=5 000 ferrites offer a flat and linear
characteristic up to approximately 1 MHz (ferrites
with μ=10 000 range up to approximately 200 kHz).
In this flat range, the attenuation properties are de-
termined by μ’ and the impedance |Z| is dominated
by the inductance L. If the self resonance of the
choke is within this frequency range, the attenuation
curve is narrow-band and attenuation is primarily
caused by reflection of the interference signal.
Above 1 MHz (or 200 kHz) Re(Z) takes the major
share of attenuation and μ’’ becomes the dominant
factor. If the self resonance of the choke is in this fre-
quency range the attenuation characteristic beco-
mes increasingly broadband.
|!|
!''
|!|
typical ferrite, !=5500
!''
!'
!'
0.001
0.01
0.1
1
10
frequency [MHz]
Fig.7:Differencesinthebalancebetweenμ’andμ’’forVITROPERMandferriteleadtodifferent
attenuationmechanisms
mꢁgnetizꢁtion ꢅꢄrve
1.5
VITROPERM is basically similar in this respect. The
flat sector of μ(f) of VITROPERM 500F ranges (de-
pending on the initial permeability level) to frequen-
cies of several 10 kHz (20 kHz in this example), only.
Consequently, attenuation (or |Z|) is already domi-
nated by Re(Z) and is always broadband in the
whole EMC-relevant range above 150 kHz. In-
ductance plays a minor role and describes the atte-
nuation only partially. The determining factor is the
total impedance. The approximation |Z|=ωL is valid
for ferrite chokes. For VITROPERM chokes |Z|>>ωL
applies. Attenuation primarily does not result from a
reflection of the interference signal, but from its ab-
sorption.
VITROPERM 500F
! = 80 000
1.0
! = 30 000
! = 20 000
VITROPERM 250F
! = 5000
0.5
0.0
typical ferrite
-0.5
-1.0
-1.5
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
2.0
2.5
H [A/cm]
Fig.8a:HysteresisloopsforvarioustypesofVITROPERMandtypicalMnZnferrite.
1.5
VITROPERM 500F
! = 80 000
! = 30 000
VITROPERM 250F
It is only when these different characteristics are
taken into consideration that the design of optimized,
compact and low-cost nanocrystalline chokes is pos-
sible. However, VITROPERM 250F is an exception,
because the flat μ(f) sector range is similar to
μ=5 000 ferrites to frequencies of up to 1 MHz and
the attenuation is primarily inductive.
1.0
0.5
0.0
! = 5000
! = 20 000
typical
ferrite
0.0
0.5
1.0
1.5
2.0
2.5
H [A/cm]
Fig.8b:MagnetizationcurveofVITROPERM500FandVITROPERM250Fincomparisonto
typicalMnZnferrite,showingnoticeabledifferencesinpermeability
(slopeofthecurve)andsaturationfluxdensity(B )
s
NaNOcRysTallINE VITROPERM / EMc PROducTs
7
Thermꢁꢂ
properties
1.4
1.2
1
nanocrystalline
VITROPERM®
The saturation flux density of VITROPERM changes
by only a few percent in the operating temperature
range of up to 150 °C, while MnZn ferrites decline
up to 40 % at temperatures above 100 °C. The high
Curie temperature of VITROPERM alloys (above
600 °C), allows short term maximum operating tem-
peratures as high as 180 – 200 °C 1).
0.8
0.6
0.4
0.2
0
typical
Mn-Zn ferrite
1)Maximumcontinuoustemperaturedependsonthecasing/coatingmaterialsused.Please
0
100
200
300
Temperature [ °C ]
400
500
600
contactVACformoredetailedinformation.
Fig.9:Temperaturedependenceofsaturationfluxdensity B (T)
s
80%
60%
typical MnZn ferrites
! = 5000 … 10 000
40%
20%
0%
The permeability of VITROPERM typically changes
by less than 10 % in the temperature range
from -40 °C to 120 °C, while the permeability of
MnZn ferrites can drift in a range of ± 40 – 60 %
around the room temperature value.
nanocrystalline
VITROPERM®
! = 30 000
nanocrystalline
VITROPERM®
! = 80 000
-20%
-40%
-40
-20
0
20
40
60
80
100
120
Temperature [°C]
Fig.10:RelativechangeofμT)atf=100kHz,normalizedforroomtemperature
Insertion loss (and impedance) of a CMC made of VITROPERM 500F is almost temperature-independent in the tempe-
rature range of – 40 °C to above 150 °C. In contrast, ferrite chokes feature a significant drop of insertion loss with increa-
sing temperature.
40
30
20
10
0
30
VITROPERM
CMC
VITROPERM
CMC
20
10
0
+120°C
+150°C
- 40°C
+ 25°C
+120°C
+150°C
+160°C
- 40°C
+ 20°C
+100°C
+120°C
+160°C
+120°C
+100°C
- 40°C
typical ferrite
CMC (high TC)
typical ferrite
CMC
+ 20°C
+ 20°C
- 40°C
0.01
0.1
1
10
100
0.001
0.01
0.1
1
10
frequency [MHz]
frequency [MHz]
Fig.11a:Comparisonoftemperaturedependenceofinsertionlossofa
VITROPERMCMCandachokewithstandardMnZnferritecore
Fig.11b:Comparisonoftemperaturedependenceofinsertionlossupto160°Cofa
VITROPERMCMCandaMnZnchokeusingahighCurietemperatureferritematerial
8
NaNOcRysTallINE VITROPERM / EMc PROducTs
sꢁtꢄrꢁtion behꢁvioꢄr
Highpermeabilitynanocrystallinecoresenableveryhighin-
Fig. 12b shows permeability characteristics under DC bias
fieldforaVITROPERM500Fcore(μ=20000)and2typical
MnZn ferrites (μ=5 000 and μ=8 000, respectively). The
diagram shows the significantly higher permeability and a
ductancelevelsinextremelycompactcoreorchokedimen-
sions.However,asaconsequenceanincreasedsensitivity
to asymmetric magnetization conditions caused by com-
monmode,unbalancedorleakagecurrentshastobecon-
sidered. These currents may occur as low-frequency
leakage currents (50 Hz) or as medium or high-frequency
interference currents. These are caused for example by
longmotorcableswithdifferentcapacitanceoftheindividual
conductors to earth, or by resonances which occur (com-
monly due to bearing currents) in such cables leading to
short, extremely high and rapidly declining current peaks
squareμ(H )characteristicofthenanocrystallinematerial
DC
in comparison to the rounded properties of the two ferrite
cores. This behaviour complies to the linear magnetization
curve of VITROPERM (Figs. 8a / 8b) and leads to nearly
constantinductanceoverawiderangeoftheDCbiasfields.
VITROPERM 250F is always used where highly satura-
tion-resistantsolutionsarerequiredforapplicationswithvery
high common mode or unbalanced currents. However, it
cannot equal the high attenuation of VITROPERM 500F.
withamplitudesofuptoseveral10A
peak
andpulsewidths
in the nanosecond range (1 … several 100 ns). If these
common mode currents exceed the saturation level of the
choke or core, the attenuation of the choke breaks down
and the choke becomes less effective.
100
10
1
The saturation behaviour of ferrite is less sensitive due to
itslowerpermeability.Forapplicationswithhigherimbalance
currents, the advantages of VITROPERM with 1.2Tsatu-
ration flux density (approximately 3 times higher than ferri-
tes) can still be realised since VITROPERM is available in
arangeofpermeabilitylevelsbetween4000and150000.
In these cases, a lower μ level may have to be selected in
order to find the optimum saturation-resistant solution. Fig.
12ashowsacomparisonofsaturationcurrentsfordifferent
VITROPERM designs with a typical ferrite core of similar
dimensions. Itcanbeseenthatthesaturationbehaviourof
the MnZn ferrite (μ=6 000) is comparable with that of
VITROPERM500F(μ=17000)uptofrequenciesofappro-
ximately 50 kHz. At higher frequencies, however, the
VITROPERM design is becoming more advantageous.
VITROPERM 250F, 40 x 25 x 15 mm
!i=4 500, AL(100kHz)=4.6!H
VITROPERM 500F, 40 x 25 x 15 mm
!i=17 000, AL(100kHz)=14!H
MnZn ferrite, 40 x 24 x 16 mm
!i=6000, AL(100kHz)=9.5!H
VITROPERM 500F, 40 x 25 x 15 mm
!i=110 000, AL(100kHz)=24!H
0.1
0.001
0.01
0.1
1
10
frequency [MHz]
Fig.12a:ComparisonofsaturationbehaviourofVITROPERM500F,VITROPERM250FandMnZnferrite
The VITROPERM solution offers a 50 % higher A value
L
at 100 kHz and a significantly higher impedance (note that
the impedance of VITROPERM is determined to a small
partbyinductanceLinthisfrequencyrange).Highpermea-
bilityVITROPERM500Fcoresarecharacterizedbyanex-
tremely high attenuation or impedance at low frequencies,
andtheyareclearlysuperioragainstferritesathighfrequen-
cies. However, the price of this superior performance is a
moresensitivesaturationbehaviour,whichisimprovingwith
increasingfrequencybutstillmorecriticalthanthatofother
core materials. It should be noted that Fig. 12a shows the
saturationcurrentsofthecoreswithoutwinding.Depending
20000
VITROPERM 500F, !=20000
15000
10000
typical MnZn ferrite, !=8000
5000
typical MnZn ferrite, !=5000
onthenumberofturns,theI valuesofchokesaresome
cm
10 mA to several 100 mA, only (see tables of standard
series).
0
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
DC bias HDC [A/cm
Fig.12b:ComparisonofpermeabilitycharacteristicsunderDCbiasfieldsforVITROPERM500F
andtwotypicalMnZnferrites.
NaNOcRysTallINE VITROPERM / EMc PROducTs
9
deꢀign ꢁꢃvꢁntꢁgeꢀ
with VITROPERM
The superior material properties of nanocrystalline
VITROPERM enable common mode chokes with
high inductance/impedance with a small number of
turns, resulting in reduced copper losses, low win-
ding capacitance and excellent HF performance.
Due to the high initial permeability, low winding ca-
pacitance and a low Q-factor (above 100 kHz)
VITROPERM CMCs offer a broadband insertion loss
curve ranging from 10 kHz up to several MHz and
improved attenuation behaviour at both low and high
frequencies in comparison to conventional ferrite
chokes with similar core dimensions and identical
windings (see Fig. 13).
Better attenuation properties and an extended ope-
rating temperature range allow a reduction of the
component volume by a factor of up to 3 or more
under similar conditions. Note that the insertion loss
curve of the small VITROPERM choke in Fig. 14 is
similar to that of ferrite materials at frequencies of
about 600 kHz – 1 MHz and is superior below 500
kHz and above 1 MHz.
Fig.13:ComparisonofinsertionlosscurveofaVITROPERM500FCMC(redcurve)andferriteCMC
(bluecurve)ofsimilarsizeandwiththesamenumberofturns.
The excellent attenuation of VITROPERM CMCs
simplifies the filter design in a wide frequency range.
For laboratory tests, VAC offers different sample kits
with selected standard cores and chokes.
Fig.14:ComparisonofthedimensionsofaVITROPERM500FCMC(redcurve)andferriteCMC
(bluecurve)withsimilarattenuationpropertiesinthe1MHzrange
VITROPERM – tꢆpiꢅꢁꢂ ꢃꢁtꢁ
Max. operational temperature
Continuous-epoxy
Continuous-plastic casing
short-term
Permeability
T
=
max
Saturation flux density
Coercivity (static)
Saturation magnetostriction
VITROPERM 500F
VITROPERM 250F
B = 1.2 T
s
c
120 °C 1)
H < 3 A/m
130/155 °C 1)
180 °C 1)
μ =
λ=
s
10-8....10-6
≈ 8 x 10-6
i
VITROPERM 500F
VITROPERM 250F
Core losses (100 kHz, 0.3 T)
15 000...150 000
4 000... 6 000
PFe = 80 W/kg (typ.)
Specific electrical resistance
Curie temperature
≈115 μ⏲cm
T > 600 °C
c
1) PleasecontactVACformoredetailedinformationaboutthetemperaturelimitsofourcasingandcoatingmaterials.
10
NaNOcRysTallINE VITROPERM / EMc PROducTs
ꢅTꢉꢁꢂꢉRꢂ ꢅꢃRIꢃꢅ
ꢀF VITRꢀPꢃRm cꢀRꢃꢅ
Oꢄr VITROPERM ꢅoreꢀ ꢁre ꢁvꢁiꢂꢁbꢂe with ꢃifferent a -ꢂeveꢂꢀ for mꢁnꢆ ꢅore
ꢀizeꢀ. Thꢄꢀ, ꢀꢁtꢄrꢁtion-reꢀiꢀtꢁnt ꢀoꢂꢄtionꢀ ꢁre ꢁvꢁiꢂꢁbꢂe for vꢁrioꢄꢀ fieꢂꢃꢀ
l
of ꢁppꢂiꢅꢁtionꢀ. common moꢃe ꢅꢄrrentꢀ mꢁꢆ oꢅꢅꢄr ꢁꢀ interferenꢅe ꢅꢄr-
rentꢀ, biꢁꢀ ꢅꢄrrentꢀ or, primꢁriꢂꢆ, ꢄnbꢁꢂꢁnꢅeꢃ ꢅꢄrrentꢀ. If the ꢅommon
moꢃe ꢅꢄrrentꢀ exꢅeeꢃ the ꢀꢁtꢄrꢁtion ꢅꢄrrentꢀ (I ) of the ꢅoreꢀ or ꢅhokeꢀ,
ꢅm
ꢅoreꢀ with higher ꢀꢁtꢄrꢁtion reꢀiꢀtꢁnꢅe mꢄꢀt be ꢄꢀeꢃ. High a vꢁꢂꢄeꢀ
l
(high μ) ꢁre more ꢀꢄitꢁbꢂe for tꢆpiꢅꢁꢂ ꢀingꢂe-phꢁꢀe ꢁppꢂiꢅꢁtionꢀ with ꢂow
ꢄnbꢁꢂꢁnꢅeꢃ ꢅꢄrrent (e.g. ꢀwitꢅheꢃ-moꢃe power ꢀꢄppꢂieꢀ), whiꢂe ꢅoreꢀ with
ꢂower a vꢁꢂꢄeꢀ ꢁre often ꢄꢀeꢃ in 3-phꢁꢀe ꢁppꢂiꢅꢁtionꢀ with high ꢄnbꢁꢂꢁn-
l
AFe
ꢅeꢃ ꢅꢄrrentꢀ (e.g. freqꢄenꢅꢆ ꢅonverterꢀ with ꢂong motor ꢅꢁbꢂeꢀ).
OD
Nꢁnoꢅrꢆꢀtꢁꢂꢂine VITROPERM ꢅoreꢀ
with epoxꢆ reꢀin ꢅoꢁting
da
di
ID
Although the epoxy resin coating is suitable for direct winding, we recommend additional insula-
tion between core and winding for enhanced insulation requirements. The epoxy resin is suitable
for continuous operational temperatures of up to 120 °C and complies with the UL94-V0 standard
(UL file number: E214934), class A (105 °C).
h
H
*
AL
nominal core
dimensions
limiting dimensions
(incl. coating)
iron cross
section
mean path
length
weight
saturation current
Icm**, typical
10 kHz
100 kHz
OD
ID
H
nominal
µH
10 kHz
100 kHz
part number
da x di x h
AFe
cm2
0,08
lFe
mFe
g
mm x mm x mm
16 x 12.5 x 6
22 x 17 x 6
25 x 20 x 10
mm
mm
mm
cm
A
2,6
2,6
15,0
4,8
3,9
0,5
1,1
0,8
1,7
T60004-L2016-W620
T60004-L2016-W619
17,8
24,0
27,3
10,7
15,2
17,5
8
4,5
6,1
7,1
6,0
8,0
12,3
0,12
0,19
5,4
16,4
4,3
0,6
1,2
T60004-L2022-W867
9,9
9,9
22,5
9,0
7,2
5,8
0,7
1,7
1,4
2,7
T60004-L2025-W622
T60004-L2025-W621
30 x 25 x 15
30 x 20 x 10
32,3
32,5
22,7
17,8
17,5
12,5
0,27
0,40
8,6
7,9
17,4
23,1
26,5
56,0
8,5
0,9
0,6
1,7
1,2
T60004-L2030-W676
T60004-L2030-W911
13,4
36
36
32,5
13,0
10,3
8,4
1,1
2,8
2,2
4,3
T60004-L2040-W624
T60004-L2040-W623
40 x 32 x 15
45 x 32 x 15
50 x 40 x 20
42,3
47,3
52,3
29,1
29,8
37,1
17,8
17,8
22,8
0,44
0,71
0,73
11,3
12,1
14,1
63,3
19,7
12,8
3,0
4,6
T60004-L2045-W886
76
76
43,0
17,0
13,8
11,2
1,4
3,6
2,7
5,4
T60004-L2050-W626
T60004-L2050-W625
124
124
18,0
11,5
11,6
10,4
4,4
6,9
6,7
8,7
T60004-L2063-W627
T60004-L2063-W721
63 x 50 x 20
80 x 63 x 20
100 x 80 x 20
65,5
83
46,6
59,5
75
22,8
22,8
23
0,95
1,24
1,46
17,8
22,5
28,3
205
205
18,5
11,9
12,0
10,7
5,6
8,7
8,5
11,0
T60004-L2080-W628
T60004-L2080-W722
303
303
17,3
11,2
11,2
10,0
7,1
10,9
10,7
13,8
T60004-L2100-W629
T60004-L2100-W723
104
2,85
2,74
36,1
36,1
757
727
727
50,0
25,4
16,4
19,4
16,5
14,7
4,8
9,0
14,0
8,5
13,6
17,7
T60004-L2130-W567
T60004-L2130-W630
T60004-L2130-W587
130 x 100 x 25
134,5
95,0
28,5
2,74
36,1
917
917
20,1
13,0
13,1
11,7
11,3
17,6
17,1
22,3
T60004-L2160-W631
T60004-L2160-W720
160 x 130 x 25
194 x 155 x 25
165
200
125
149
28,5
28,5
2,74
45,6
1490
1490
45,3
14,7
14,7
13,2
6,9
20,7
12,5
26,4
T60004-L2194-V105
T60004-L2194-W908
3,71
54,8
NaNOcRysTallINE VITROPERM / EMc PROducTs
11
Nꢁnoꢅrꢆꢀtꢁꢂꢂine VITROPERM
ꢅoreꢀ in pꢂꢁꢀtiꢅ ꢅꢁꢀing
The plastic cases are suitable for direct winding and offer good mechanical
protection of the nanocrystalline core material. This enables the best mag-
netic properties and highest permeability levels to be maintained. Additional
winding protection is optional for heavy wire windings, where there may be
a danger of core damage. The plastic materials comply with the standards
UL94-V0 (UL file number: E41871), class B (130 °C) and UL94-V0 (UL file
number E41938), class F (155 °C).
*
AL
nominal core
dimensions
limiting dimensions
(incl. case)
iron cross
section
mean path
length
weight
saturation current
Icm**, typical
10 kHz
100 kHz
OD
mm
11,2
14,1
14,3
17,1
ID
mm
5,1
6,6
8,5
7,9
H
nominal
µH
10 kHz
100 kHz
part number
da x di x h
mm x mm x mm
9.8 x 6.5 x 4.5
12 x 8 x 4.5
12.5 x 10 x 5
15 x 10 x 4.5
AFe
lFe
mFe
g
cm2
0,06
mm
5,8
6,3
7,0
6,5
cm
2,6
3,1
3,5
3,9
A
1,1
1,7
1,3
2,6
25,5
6,4
6,8
3,6
6,7
0,2
0,2
0,4
0,3
0,4
0,4
0,8
0,5
T60006-L2009-W914
T60006-L2012-W902
T60006-L2012-W498
T60006-L2015-W865
0,07
0,05
0,09
28,0
10,0
27,0
4
4
43,0
11,7
10,1
6,5
0,3
1,2
0,6
1,7
T60006-L2016-W403
T60006-L2016-W308
16 x 10 x 6
17,9
8,1
8,1
0,14
4,1
17.5 x 12.6 x 6
19 x 15 x 10
19,0
21,2
11,0
13,0
8,0
0,12
0,16
4,7
5,3
4,1
6,3
30,0
36,1
6,9
8,8
0,3
0,4
0,7
0,7
T60006-L2017-W515
T60006-L2019-W838
12,3
9,0
9,0
55,2
14,3
13,6
9,1
0,4
1,4
0,7
2,1
T60006-L2020-W409
T60006-L2020-W450
20 x 12.5 x 8
25 x 20 x 10
22,6
27,6
10,3
17,4
10,2
12,8
0,24
0,20
5,1
7,1
10,4
28,4
7,3
0,6
1,1
T60006-L2025-W523
17
17
17
65,5
17,0
3,2
15,5
11,5
3,1
0,4
1,7
9,3
0,9
2,6
9,6
T60006-L2025-W380
T60006-L2025-W451
T60006-L2025-W980
25 x 16 x 10
27,9
13,6
12,5
0,36
6,4
23
23
23
59,3
15,5
2,9
14,0
11,1
2,8
0,5
2,1
1,0
3,1
T60006-L2030-W423
T60006-L2030-W358
T60006-L2030-W981
30 x 20 x 10
30 x 20 x 15
40 x 32 x 15
32,8
32,8
43,1
17,6
17,5
28,7
12,5
17,8
18,5
0,40
0,57
0,46
7,9
7,9
11,4
11,8
33
88,0
20,0
0,5
1,1
T60006-L2030-W514
38
38
38
47,2
12,2
2,3
11,1
7,9
0,8
3,7
1,5
5,1
T60006-L2040-W422
T60006-L2040-W452
T60006-L2040-W964
11,3
2,2
16,6
17,1
64
64
101,0
25,4
23,1
17,2
0,7
2,9
1,4
4,2
T60006-L2040-W424
T60006-L2040-W453
40 x 25 x 15
45 x 30 x 15
50 x 40 x 20
63 x 50 x 25
43,1
48,3
53,5
67,3
22,5
26,4
36,3
46,5
18,5
18,2
23,4
28,6
0,86
0,86
0,76
1,24
10,2
11,8
14,1
17,8
74
74
74
87,5
24,3
15,7
20,3
15,9
14,3
0,8
3,0
4,6
1,6
4,5
5,8
T60006-L2045-V102
T60006-L2045-V118
T60006-L2045-V101
79
79
45,3
18,0
14,0
10,0
1,4
3,5
2,7
5,3
T60006-L2050-W516
T60006-L2050-W565
161
161
163
58,6
23,3
3,3
18,1
13,5
3,2
1,8
4,4
3,5
6,7
T60006-L2063-W517
T60006-L2063-V110
T60006-L2063-W985
30,2
30,9
342
347
35,0
9,6
24,0
9,2
5,5
26,4
8,2
27,3
T60006-L2080-W531
T60006-L2080-V091
80 x 50 x 20
90 x 60 x 20
100 x 80 x 25
86,0
95,4
44,7
54,7
75,0
25,7
24,7
29,6
2,28
2,28
1,90
20,4
23,6
28,3
395
400
81,0
4,6
25,1
4,5
2,4
40,9
4,5
41,8
T60006-L2090-W518
T60006-L2090-W984
379
379
56,3
14,5
16,9
13,1
2,8
10,9
5,3
13,8
T60006-L2100-V082
T60006-L2100-V081
105,5
508
508
515
68,8
19,1
4,3
21,6
17,2
4,2
3,8
10,7
47,4
6,7
13,6
48,5
T60006-L2102-W468
T60006-L2102-V080
T60006-L2102-W947
102 x 76 x 25
160 x 130 x 25
108,1
70,0
30,3
30,5
2,47
28,0
2,74
2,74
2,74
2,85
45,6
45,6
45,6
45,6
917
917
917
967
26,8
20,1
12,9
3,0
13,7
13,1
11,7
2,9
8,4
13,6
17,1
22,3
81,1
T60006-L2160-V074
T60006-L2160-V088
T60006-L2160-V066
T60006-L2160-W982
11,3
17,6
79,3
166,9 123,9
* AL = inductance for N = 1 (tolerance +45 % / -25 %) ** Icm : the listed saturation currents are guidelines, only. They are
calculated for nominal core dimensions at room temperature and for approx. 70 % saturation flux density. The frequency-
dependent saturation behaviour is demonstrated in Fig. 12.
12
NaNOcRysTallINE VITROPERM / EMc PROducTs
core ꢀtꢁꢅk ꢁꢀꢀembꢂieꢀ
with
nꢁnoꢅrꢆꢀtꢁꢂꢂine ꢅoreꢀ
Single-turn chokes employing a number of nanocry-
stalline cores assembled in a stack are an effective
solution for bearing current problems or extremely
high common mode noise from other causes in
large-scale variable speed drives, wind generators
and other applications in which resonance pheno-
mena cause high-amplitude interference currents
(with peak values ranging from several 10 A to over
100 A). These generally take the form of short and
thus high-frequency current peaks. For these appli-
cations, VAC offers assembled core stacks which
can be easily and securely integrated into existing
applications with the minimum of effort.
1
0
.
.
.
1
0
0
A
p
e
a
k
<
1
µ
s
1
0
0
µ
s
I
n
v
e
r
t
e
r
M
o
t
o
r
The core stacks are available in two sizes with two
different through-hole diameters. They are custom-
designed, allowing an individual selection of core
type and the number of stacked cores (up to 7 pie-
ces) depending on the required saturation level and
the required inductance.
h
i
g
h
v
o
l
t
a
g
e
o
v
e
r
b
e
a
r
i
n
g
s
P
E
size 1
120
130
70
size 2
180
190
a (mm)
b (mm)
c (mm)
d (mm)
s (mm)
130
> 118
10
~ 70
7
n = number of stacked cores
H = maximum core height
y = 9.5 for epoxy coated cores, T60004...
y = 10.2 for cased cores, T60006...
The inductance L of a core stack can be calculated by multiplying
the number of stacked cores with the AL-value of the single core.
A
I
: inductance of single core
: maximum permissible leakage or common mode current.
L
cm
Calculated guideline for nominal core dimensions at room tempera-
ture and for approximately 70 % saturation flux density.
Dimensions of the core stack assemblies
core data
data of core stack
example for 5 stacked cores
nominal core
dimensions
limit core dimensions
(incl. Case/coating)
L (10 kHz) L (100 kHz)
AL (10 kHz) AL (100 kHz)
Icm (10 kHz)
typical
A
Icm(100 kHz)
typical
A
core part number
OD
ID
H
nominal
µH
nominal
µH
size
nominal
µH
nominal
µH
da x di x h
mm x mm x mm mm
mm
mm
T60004-L2100-W629
T60004-L2100-W723
T60006-L2100-V082
T60006-L2100-V081
T60006-L2102-W468
T60006-L2102-V080
T60006-L2102-W947
T60006-L2160-V074
T60006-L2160-V088
T60006-L2160-V066
T60006-L2160-W982
100 x 80 x 20
100 x 80 x 20
100 x 80 x 25
100 x 80 x 25
102 x 76 x 25
102 x 76 x 25
102 x 76 x 25
160 x 130 x 25
160 x 130 x 25
160 x 130 x 25
160 x 130 x 25
104,0
104,0
105,5
105,5
108,1
108,1
108,1
166,9
166,9
166,9
166,9
75,0
75,0
23,0
23,0
29,6
29,6
30,3
30,3
30,3
30,5
30,5
30,5
30,5
17,3
11,2
56,3
14,5
68,8
19,1
4,3
11,2
10,0
16,9
13,1
21,6
17,2
4,2
1
1
1
1
1
1
1
2
2
2
2
7,1
10,9
2,8
10,7
13,8
5,3
86,5
56,0
56,0
50,0
84,5
65,5
108,0
86,0
21,0
68,5
65,5
58,5
14,3
75,0
281,5
72,5
75,0
10,9
3,8
13,8
6,7
70,0
344,0
95,5
70,0
10,7
47,4
8,4
13,6
48,5
13,6
17,1
22,3
81,1
70,0
21,5
123,9
123,9
123,9
123,9
26,8
20,1
12,9
3,0
13,7
13,1
11,7
2,9
134,0
100,5
64,5
11,3
17,6
79,3
15,0
NaNOcRysTallINE VITROPERM / EMc PROducTs
13
coꢈꢈon ꢈode ꢆhoꢇes
UL1446 ꢅTꢉꢁꢂꢉRꢂ ꢅꢃRIꢃꢅ
Generꢁꢂ informꢁtion
Chokes are designed, manufactured and tested in compliance with
EN50178.
Plastic materials comply with the following UL standards:
UL94 (file number E41871)
UL1446 (file number OBJY2.E329745)
Temperature class B (130 °C)
IN
UN OVCat III / II
LN
Ambient temperature Ta = – 40°C...+70°C (short-term +90°C)
Operating temperature Top = – 40°C...+130°C (short-term +150°C)
= nominal current in each winding
= operating voltage for overvoltage category III / II
= nominal inductance, tolerance +50% / -30 %
The standard chokes are designed for a temperature rise of
ΔT = 45….60 K at Ta=70 °C and I=IN in each winding. Data
derating is necessary for deviating ambient temperature or
deviating nominal current. Please contact VAC for further de-
tailed information.
stꢁnꢃꢁrꢃ ꢀerieꢀ cMcꢀ for ꢀingꢂe-phꢁꢀe ꢁppꢂiꢅꢁtionꢀ
|Z|
RCu
fR
Icm
LN
IN
A
design
UN
dimensions
b
part number
OVCat III / II 10 kHz
100 kHz
typ.
m!
100kHz
!
typ.
MHz
10 kHz
mA
l
h
V
mH
mm
mm
mm
2
upright
300 / 600
300 / 600
300 / 600
300 / 600
300 / 600
300 / 600
300 / 600
300 / 600
300 / 600
300 / 600
300 / 600
300 / 600
300 / 600
300 / 600
300 / 600
300 / 600
2x12.1
2x10.8
2x28.3
2x29.1
2x16.4
2x11.4
2x11.4
2x11.4
2x11.4
2x8.6
2x12.9
2x6
2x2.8
2x2.5
2x6.6
2x6.7
2x3.7
2x2.6
2x2.6
2x2.6
2x2.6
2x2.2
2x3.1
2x1.5
2x0.7
2x0.4
2x1.6
2x1
101
27,5
36
3000
2320
6500
8500
4200
3200
3150
2950
2950
2250
3000
1600
830
3,6
1.2
0,4
0,25
0,5
0,7
0.7
0,7
0,7
1,1
3.0
1.0
3,3
11,5
5,7
7,1
2,4
4,9
7.0
4.0
8,2
6,7
9,3
1,6
17
12
18
14
20
16
16
22
22
28
37
35
60
40
35
50
55
50
50
65
90
110
150
200
22
22
27
35
35
35
35
38
35
35
40
38
36
35
43
12
12
17
21
21
35
21
22
35
35
40
21
21
35
43
25 T60405-R6131-X402
25 T60405-R6131-X204
29 T60405-R6161-X504
37 T60405-R6166-X206
36,5 T60405-R6166-X208
23 T60405-R6123-X210
37 T60405-R6166-X210
35 T60405-R6126-X212
25 T60405-R6123-X213
22 T60405-R6122-X100
24 T60405-R6123-X616
38 T60405-R6166-X033
38 T60405-R6166-X039
23,5 T60405-R6123-X220
24 T60405-R6123-X221
25 T60405-R6123-X226
32 T60405-R6123-X227
40 T60405-R6128-X225
29 T60405-R6123-X232
50 T60405-R6128-X031
32 T60405-R6123-X241
32 T60405-R6123-X248
32 T60405-R6123-X263
40 T60405-R6123-X285
4
upright
upright
4.5
6
upright
37,6
19,1
12,2
12,7
8.9
8
upright
10
10
12
12
13
16
16
16
20
20
25
25
25
30
30
40
48
63
85
low profile
upright
upright
low profile
low profile
low profile
upright
8,8
6,3
5,7
4,6
upright
2x2.9
2x1.8
2x6.6
2x4.2
2x12
3,9
low profile
low profile
low profile
3,2
500
2.9
1470
970
1.9
42,5 42,5
low profile 600 / 1000
upright
300 / 600
low profile 600 / 1000
upright
600 / 1000
2x2.8
2x1
3,5
2900
970
52
42
52
51
52
52
52
27
52
27
52
52
2x4.2
2x3.9
2x3.9
2x3.6
2x2.5
2x1.6
2x1.6
1.9
2x0.9
2x0.9
2x0.8
2x0.6
2x0.4
2x0.5
2.4
920
2,3
900
low profile 600 / 1000
low profile 600 / 1000
low profile 600 / 1000
low profile 600 / 1000
1.4
870
0.75
0,5
660
390
53,5 53,5
73 73
0.6
510
RCu: winding resistance per winding |Z| : choke impedance fR : choke resonance frequency
For more detailed technical information please see our product data sheets at www.vꢁꢅꢄꢄmꢀꢅhmeꢂze.ꢅom. Custom
CMCs for other nominal currents, in different designs and with other properties are available on request.
14
NaNOcRysTallINE VITROPERM / EMc PROducTs
3- and 4-phase cmcs
T
±
(
o
l
e
r
a
n
z
d
e
r
S
t
i
f
t
a
b
s
t
ä
n
B
d
e
e
s
c
h
r
i
f
t
u
n
g
e
D
C
=
D
a
t
e
C
o
d
e
T
r
n
n
s
t
F
=
F
a
c
t
o
r
y
( m
0
,
3
m
m
a
r
k
i
n
g
)
(
s
e
p
a
r
a
T
o
l
e
r
a
n
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e
s
g
r
i
d
d
i
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t
a
n
c
e
)
³
5
.
5
m
m
3
x
1
2
0
°
1
3
0
°
F
D
C
5
1
6
3
0
°
4
2
3
x
1
2
0
°
3
Ø
2
0
,
9
Ø
5
3
£
3
3
4
.
5
±
0
,
5
Ø
5
9
We provide more detailed technical information (data sheets) for all standard products on our web-page
www.vꢁꢅꢄꢄmꢀꢅhmeꢂze.ꢅom. Example outline of the 3-phase CMC T60405-S6123-X332.
standard series 3-phase chokes for 3-phase applications
|Z|
RCu
fR
Icm
LN
IN design
A
UN
OVCat III / II
V
dimensions
b
part number
10 kHz
100 kHz
100kHz
!
10 kHz
mA
l
h
mH
m!
MHz
mm
mm
mm
7
10
11
600 / 1000
600 / 1000
600 / 1000
600 / 1000
600 / 1000
600 / 1000
600 / 1000
600 / 1000
600 / 1000
600 / 1000
600 / 1000
600 / 1000
600 / 1000
600 / 1000
600 / 1000
3x31.8
3x13.9
3x10.6
3x5.7
3x4.8
3x9.4
3x10.6
3x2
3x7.4
3x3.2
3x2.5
3x3.7
3x3.1
3x2.2
3x2.4
3x1.3
3x1.1
3x0.8
3x0.6
3x0.8
3x0.5
3x0.5
3x0.6
24,6
14
8650
3500
2600
2650
2500
2400
2650
1000
1150
600
0,23
1,5
0,8
0,48
0,65
1,45
0,9
2,8
2
27
30
40,5 40,5 32,5 T60405-S6123-X306
low profile
low profile
low profile
low profile
low profile
low profile
low profile
low profile
low profile
low profile
low profile
low profile
low profile
low profile
low profile
51
42
51
59
51
42
51
59
32 T60405-S6123-X310
32 T60405-S6123-X308
32 T60405-S6123-X312
32 T60405-S6123-X316
34 T60405-S6123-X317
33 T60405-S6123-X320
33 T60405-S6123-X325
32 T60405-S6123-X326
33 T60405-S6123-X332
33 T60405-S6123-X140
37 T60405-S6123-X240
42 T60405-S6123-X363
53 T60405-S6123-X370
57 T60405-S6123-X311
8,5
40
12
16
16
20
25
25
32
40*
40*
63
70
110
11,8
6,5
150
200
35
5,9
51,5 51,5
4,1
60
59
60
59
60
2,27
2,1
380
60
3x4.9
3x1.2
3x2.5
3x1.5
3x1.6
3x0.8
3x0.7
51,5 51,5
1,4
4,9
4,7
4
480
100
380
190
900
1750
59
52
59
52
1,2
600
1,72
0,72
0,86
0,63
680
70
70
500
1
70
70
415
1,45
1,4
85
85
430
135
135
standard series 4-fold chokes
10**
12
16**
20
24**
30
600 / 1000
600 / 1000
600 / 1000
600 / 1000
4x6.9
4x3.6
4x3.2
4x1.4
4x1.6
4x0.8
4x0.7
4x0.3
7,66
2,75
1,5
1500
860
750
360
1,7
3,4
3,5
7
40
90
51
51
33 T60405-S6123-X400
33 T60405-S6123-X401
33,5 T60405-S6123-X402
33 T60405-S6123-X403
low profile
low profile
low profile
low profile
51,5 51,5
100
160
60
60
60
60
32**
40
0,82
* for Ta ! 60°C
** for Ta ! 85°C
NaNOcRysTallINE VITROPERM / EMc PROducTs
15
VacuuMscHMElZE GMBH & cO. KG
GRÜNER WEG 37
D 63450 HANAU / GERMANY
PHONE +49 6181 38 0
FAX +49 6181 38 2645
INFO@VACUUMSCHMELZE.COM
WWW.VACUUMSCHMELZE.COM
Vac salEs usa llc
2935 DOLPHIN DRIVE / SUITE 102
42701 ELIZABETHTOWN KY / USA
PHONE +1 270 769-1333
FAX +1 270 765 3118
INFO-USA@VACUUMSCHMELZE.COM
VacuuMscHMElZE salEs OFFIcE sINGaPuR
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SINGAPORE 417943
PHONE (+65) 63 91 26 00
Fax: (+65) 63 91 26 01
VACSINGAPORE@VACUUMSCHMELZE.COM
PKB-EMc Eꢃition 2010
All rights reserved.
VITROPERM® is a registered trademark of VACUUMSCHMELZE
GmbH & Co. KG in Germany, Austria and Switzerland. As far as pa-
tents or other rights of third parties are concerned, liability is only as-
sumed for product per se, not for applications, processes and circuits
implemented whithin theses products. The information describes the
type of product and shall not be considered as assured characteris-
tics. Terms of delivery and right to change design reserved.
adVaNcEd MaTERIals – THE KEy TO PROGREss
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