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AN2450 Datasheet(PDF) 9 Page - STMicroelectronics

Part # AN2450
Description  LLC resonant half-bridge converter design guideline
PDF  35 Pages
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Manufacturer  STMICROELECTRONICS [STMicroelectronics]
Direct Link  http://www.st.com
Logo STMICROELECTRONICS - STMicroelectronics

AN2450 Datasheet(HTML) 9 Page - STMicroelectronics

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AN2450
Voltage gain and input impedance
35
2
Voltage gain and input impedance
Starting from Equation 18 we can obtain the expression of the voltage gain:
Equation 20
with the following parameter definitions:
resonance frequency:
characteristic impedance:
quality factor:
inductance ratio:
normalized frequency:
Under no-load conditions, (i.e. Q = 0) the voltage gain assumes the following form:
Equation 21
Figure 3 shows a family of plots of the voltage gain versus normalized frequency. For
different values of Q, with
 = 0.2, it is clearly visible that the LLC resonant converter
presents a load-independent operating point at the resonance frequency fr (fn = 1), with
unity gain, where all the curves are tangent (and the tangent line has a slope -2
).
Fortunately, this load-independent point occurs in the inductive region of the voltage gain
characteristic, where the resonant tank current lags the input voltage square waveform
(which is a necessary condition for ZVS behavior).
The regulation of the converter output voltage is achieved by changing the switching
frequency of the square waveform at the input of the resonant tank: since the working region
is in the inductive part of the voltage gain characteristic, the frequency control circuit that
keeps the output voltage regulated acts by increasing the frequency in response to a
decrease of the output power demand or to an increase of the input dc voltage. Considering
this, the output voltage can be regulated against wide loads variations with a relatively
narrow switching frequency change, if the converter is operated close to the load-
independent point. Looking at the curves in Figure 3, it is obvious that the wider the input dc
voltage range is, the wider the operating frequency range will be, in which case it is difficult
Mfn  Q


1
1
fn
2
-------
–
+


 2
Q
2 f
n
1
fn
----
–

 2
+
----------------------------------------------------------------------------
=
fr
1
2
 L
rCr
-----------------------
=
Zo
Lr
Cr
------
2
f
rLr
1
2
f
rCr
-----------------
=
=
=
Q
Zo
Rac
---------
Zo
n
2R
oac
-------------------
2
8
------
Z0
n
2
------
Pout
V
2
out
--------------
=
=
=
.
Lr
Lm
-------
=
fn
fsw
fr
-------
=
MOL fn

1
1
fn
2
-------
–
+
-----------------------------
=



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