Ferrites and accessories
ETD 39/20/13
Core and accessories
Series/Type:
Date:
B66363, B66364
June 2013
Data Sheet
EPCOS AG 2015. Reproduction, publication and dissemination of this publication, enclosures hereto and the information
contained therein without EPCOS' prior express consent is prohibited.
EPCOS AG is a TDK Group Company.
ETD 39/20/13
Core
■
To IEC 61185
■
For SMPS transformers with optimum
B66363
weight/performance ratio at small volume
■
Delivery mode: single units
Magnetic characteristics
(per set)
l/A
l
e
A
e
A
min
V
e
= 0.74 mm
–1
= 92.2 mm
= 125 mm
2
= 123 mm
2
= 11500 mm
3
Approx. weight
60 g/set
Ungapped
Material A
L
value
nH
N27
N87
N97
e
B
S
*
mT
320
320
320
P
V
W/set
Ordering code
2550 +30/–20% 1500
2700 +30/–20% 1600
2800 +30/–20% 1650
< 2.22 (200 mT, 25 kHz, 100 °C) B66363G0000X127
< 6.00 (200 mT, 100 kHz, 100 °C) B66363G0000X187
< 5.10 (200 mT, 100 kHz, 100 °C) B66363G0000X197
* H = 250 A/m; f = 10 kHz; T = 100 °C
Gapped
Material
g
mm
0.100.02
0.200.02
0.500.05
1.00
0.05
A
L
value
approx.
nH
1062
639
326
196
e
Ordering code
** = 27 (N27)
**
= 87 (N87)
B66363G0100X1**
B66363G0200X1**
B66363G0500X1**
B66363G1000X1**
N27,
N87
622
374
191
115
The A
L
value in the table applies to a core set comprising one ungapped core (dimension g = 0) and
one gapped core (dimension g > 0).
Calculation factors
(for formulas, see
“E cores: general information”
)
Material
Relationship between
air gap – A
L
value
K1 (25 °C)
N27
N87
Validity range:
196
196
K2 (25 °C)
– 0.734
– 0.734
Calculation of saturation current
K3 (25 °C)
308
300
K4 (25 °C)
– 0.847
– 0.796
K3 (100 °C) K4 (100 °C)
287
280
– 0.865
– 0.873
K1, K2: 0.10 mm < s < 3.00 mm
K3, K4: 90 nH < A
L
< 850 nH
2
06/13
Please read
Cautions and warnings
and
Important notes
at the end of this document.
ETD 39/20/13
Accessories
Coil former
GFR polyterephthalate, UL 94 V-0, insulation class to IEC 60085:
B66364B: F max. operating temperature 155 °C, color code black
Valox 420-SE0
®
E45329 (M)
, GE PLASTICS B V
B66364W: H max. operating temperature 180 °C, color code black
Rynite FR 530
®
E41938 (M)
, E I DUPONT DE NEMOURS & CO INC
Solderability: to IEC 60068-2-20, test Ta, method 1 (aging 3): 235 °C, 2 s
Resistance to soldering heat: to IEC 60068-2-20, test Tb, method 1B: 350 °C, 3.5 s
Winding:
see Data Book 2013, chapter “Processing notes, 2.1”
Yoke
Material:
Coil former
Sections
1
A
N
mm
2
178
l
N
mm
69
A
R
value
13.3
Pins
16
B66364B1016T001
B66364W1016T001
B66364A2000X000
Stainless spring steel (0.4 mm)
Ordering code
Material:
B66364
Yoke (ordering code per piece, 2 are required)
Coil former
Yoke
Please read
Cautions and warnings
and
Important notes
at the end of this document.
3
06/13
Ferrites and accessories
Cautions and warnings
Cautions and warnings
Mechanical stress and mounting
Ferrite cores have to meet mechanical requirements during assembling and for a growing number
of applications. Since ferrites are ceramic materials one has to be aware of the special behavior
under mechanical load.
As valid for any ceramic material, ferrite cores are brittle and sensitive to any shock, fast changing
or tensile load. Especially high cooling rates under ultrasonic cleaning and high static or cyclic loads
can cause cracks or failure of the ferrite cores.
For detailed information see chapter
“Definitions”,
section 8.1.
Effects of core combination on A
L
value
Stresses in the core affect not only the mechanical but also the magnetic properties. It is apparent
that the initial permeability is dependent on the stress state of the core. The higher the stresses are
in the core, the lower is the value for the initial permeability. Thus the embedding medium should
have the greatest possible elasticity.
For detailed information see chapter
“Definitions”,
section 8.2.
Heating up
Ferrites can run hot during operation at higher flux densities and higher frequencies.
NiZn-materials
The magnetic properties of NiZn-materials can change irreversible in high magnetic fields.
Processing notes
– The start of the winding process should be soft. Else the flanges may be destroid.
– To strong winding forces may blast the flanges or squeeze the tube that the cores can no more
be mount.
– To long soldering time at high temperature (>300 °C) may effect coplanarity or pin arrangement.
– Not following the processing notes for soldering of the J-leg terminals may cause solderability
problems at the transformer because of pollution with Sn oxyd of the tin bath or burned insulation
of the wire. For detailed information see chapter
“Processing notes”,
section 8.2.
– The dimensions of the hole arrangement have fixed values and should be understood as
a recommendation for drilling the printed circuit board. For dimensioning the pins, the group
of holes can only be seen under certain conditions, as they fit into the given hole arrangement.
To avoid problems when mounting the transformer, the manufacturing tolerances for positioning
the customers’ drilling process must be considered by increasing the hole diameter.
4
06/13
Ferrites and accessories
Symbols and terms
Symbols and terms
Symbol
A
A
e
A
L
A
L1
A
min
A
N
A
R
B
B
ˆ
B
ˆ
B
B
DC
B
R
B
S
C
0
CDF
DF
d
E
a
f
f
cutoff
f
max
f
min
f
r
f
Cu
g
H
ˆ
H
H
DC
H
c
h
h/
i
2
I
I
DC
ˆ
I
J
k
k
3
k
3c
L
Meaning
Cross section of coil
Effective magnetic cross section
Inductance factor; A
L
= L/N
2
Minimum inductance at defined high saturation (
a
)
Minimum core cross section
Winding cross section
Resistance factor; A
R
= R
Cu
/N
2
RMS value of magnetic flux density
Flux density deviation
Peak value of magnetic flux density
Peak value of flux density deviation
DC magnetic flux density
Remanent flux density
Saturation magnetization
Winding capacitance
Core distortion factor
Relative disaccommodation coefficient DF = d/
i
Disaccommodation coefficient
Activation energy
Frequency
Cut-off frequency
Upper frequency limit
Lower frequency limit
Resonance frequency
Copper filling factor
Air gap
RMS value of magnetic field strength
Peak value of magnetic field strength
DC field strength
Coercive field strength
Hysteresis coefficient of material
Relative hysteresis coefficient
RMS value of current
Direct current
Peak value of current
Polarization
Boltzmann constant
Third harmonic distortion
Circuit third harmonic distortion
Inductance
5
06/13
Unit
mm
2
mm
2
nH
nH
mm
2
mm
2
= 10
–6
Vs/m
2
, mT
Vs/m
2
, mT
Vs/m
2
, mT
Vs/m
2
, mT
Vs/m
2
, mT
Vs/m
2
, mT
Vs/m
2
, mT
F = As/ V
mm
–4.5
J
s
–1
, Hz
s
–1
, Hz
s
–1
, Hz
s
–1
, Hz
s
–1
, Hz
mm
A/m
A/m
A/m
A/m
10
–6
cm/A
10
–6
cm/A
A
A
A
Vs/m
2
J/K
H = Vs/A
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