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AN1673 Datasheet(PDF) 17 Page - STMicroelectronics

Part # AN1673
Description  L6598 OFF-LINE CONTROLLER FOR RESONANT CONVERTERS
PDF  24 Pages
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Manufacturer  STMICROELECTRONICS [STMicroelectronics]
Direct Link  http://www.st.com
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AN1673 Datasheet(HTML) 17 Page - STMicroelectronics

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AN1673 APPLICATION NOTE
Using the "Product Area" (AP) criterion, we can get a first approximation of the core area product. The
required AP can be found using the equations Ap1 and Ap2 (we use the same formulas as for the standard
half bridge forward converter).
AP (=AW*Ae) is the winding area (AW, associated to the former) time the magnetic cross section (Ae, as-
sociated to the ferrite).
N.B. For choosing the resonant elements (inductance and capacitor) and its relation with the frequency to
be set, one can have an easy task referring to the convention described in appendix A.
– Start choosing the minimum operative frequency (corresponding to full load) at 65kHz.
[14]
Ap1)
# related to core losses limit
Where: Kh = 4 · 10-5; Ke = 4 · 10-10; ƒsw = 65kHz
For the present design, AP1 = 0.38cm4
[15]
Ap2)
# related to saturation limit
Where:
K = 0.165 related to the Half Bridge connection;
∆Bmax 0.4T; Pin is the power handled by the transformer.
In the present design, should be AP2 = 0.17cm4
The needed AP will be the larger of the two resulting values.
To met the current target specification, we need AP = AP1 = 0.38cm4.
Select the ferrite's set EE30 (E30 · 15 · 7) in high frequency (e.g. B2 or F1) material.
(Ve = 3.9cm3; Aw = 0.8 cm2; Ae = 0.6cm2) => AP=Aw · Ae=0.48 cm4.
Transformer's Winding
To define the winding, first it must be fixed the input DC Bus value.
Since in the discussed design the pre regulator stage (see later in Power Factor section) is requested, let's
start fixing the voltage bus range at 360V to 420V.
The second resonant inductor of the LCL resonant converter can be achieved managing the proper value
of primary inductance of Transformer.
This second inductance allows to properly operating in light load condition holding in the same time the
higher efficiency for the entire load range. In our experience, to take advantage by using the primary in-
ductance as second inductor, a good ratio between its value and the stray inductance (Lmag/Lstray) is in
the range of 3.5 to 7.
The relation between the primary and the stray inductances can be adjusted using the slotted bobbin (that
increases the stray inductance) and introducing an air gap in the transformer's ferrite set (that reduces the
magnetizing inductance).
We choose a two layer slotted former (split the primary and secondary sides). See fig.20.
Figure 20. Transformer
AP1
41.7 Pin
⋅
Kƒ
sw
⋅
-------------------------

 1.58
Kh ƒt
Ke ƒt
2
⋅
+
⋅
()
0.66
⋅
=
AP2
11.1 Pin
⋅
KBmax
∆
ƒ
sw
⋅⋅
-------------------------------------------

 1.31
=
Secondary
Slotted former
Primary
Aux.
N1
Prim.
Aux.
N2a
N2b
T
Sec.
D03IN1460



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