STMicroelectronics A 200 W ripple-free input current PFC pre-regulator with the L6563S EVL6563S-200ZRC EVL6563S-200ZRC Data Sheet

Product codes
EVL6563S-200ZRC
Page of 39
   
   
   
Zero-ripple current phenomenon: practice
AN3180
14/39
 Doc ID 17273 Rev 1
3. 
As a result of the aforementioned current splitting action, the same happens to the 
magnetic flux: the AC winding is responsible for generating the AC component of the 
flux and the DC winding for its DC component, but their sum is the same as in a single 
inductor carrying the total current. This means that no core size increase is expected 
because of flux density limitations (core saturation) or core loss reasons. Also the core 
size selection approach is the same.
To complete the picture, an important property of the “gapped ferrite core plus bobbin” 
assembly should be recalled. The reluctance of the leakage flux path is constant for a given 
core geometry and is independent of the gap thickness, l
gap
: essentially, it is a function of 
the physical dimensions of the core and the distance between the windings. This implies 
that the leakage inductance of the primary winding, Ll1, depends only on the turn number 
N
1
 and does not change if l
gap
 is adjusted. However, the total primary inductance L
1
= L
l1
L
M
 is strongly affected by the gap thickness, but it is only the magnetizing inductance L
M
 that 
changes. With reference to the zero-ripple current condition in 
:
Equation 13
once the ferrite core and the associated bobbin are defined, it is thereby possible to control 
LL
l1
 and L
M
 separately, acting on N
1
 and l
gap
 respectively, then the secondary turn number 
N
2
 is determined so that the ratio n = N
2
/N
1
 meets the condition in 
.
Figure 9.
Two-section slotted bobbin 
suggested for the realization of a 
coupled inductor - top view
Figure 10.
Two-section slotted bobbin 
suggested for the realization of a 
coupled inductor - side view
         
         
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L
L
L
L
L
1
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