STMicroelectronics A 200 W ripple-free input current PFC pre-regulator with the L6563S EVL6563S-200ZRC EVL6563S-200ZRC Fiche De Données

Codes de produits
EVL6563S-200ZRC
Page de 39
   
   
   
Electrical equivalent circuit models of coupled inductors and transformers
AN3180
30/39
 Doc ID 17273 Rev 1
Figure 23.
Coupled inductors
The mutual inductance M cannot be assigned arbitrarily but must fulfill the inequality:
Equation 22
The case 
 is that of perfectly coupled inductors, that is when the magnetic flux 
generated by either winding is totally linked to the other. However, in real-world systems 
there is always some flux linking one winding but not the other or not completely linking the 
winding itself, e.g. because it “leaks” into the surrounding air; and so it is possible to write:
Equation 23
k, which lies in the range -1 k 1 is the so-called coupling coefficient and is a measure of the 
degree of magnetic coupling between the windings. For simplicity, from now on winding 
polarity is neglected and assume M>0 (and 0 k 1) always, the extension to the case M<0 
being obvious.
It is possible to prove that k is the geometric mean of the portion k1 of flux generated by the 
first winding that links the second one, and the portion k2 of flux generated by the second 
winding that links the first one:
Equation 24
Note that, in general, k
1
 
≠ k
2
: fluxes do not necessarily link windings symmetrically one to 
another.
It is often useful to represent a system of coupled inductors with an equivalent circuit 
including an ideal transformer, that is a circuit element with a transfer function v
2
'(t) / v
1
'(t)=a 
for voltages and i
2
'(t) / i
1
'(t)= 1/a for currents. This equivalent circuit is shown in 
.
!-V
L

W
L

W
0
/

/

Y

W
Y

W
L

W
L

W
0
/

/

Y

W
Y

W
0!
0
2
1
L
L
M
2
1
L
L
M
=
2
1
L
L
k
M
=
2
1
k
k
k
=