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DocID026130 Rev 2
17/70
AN4461
ZVS LC resonant stage description
70
4.1
LC stage customization
4.1.1
Resonant Cell ZVS design
In order to maintain the zero voltage switching condition Equation 5 needs to be met.
Equation 5
When the half-bridge switching frequency (fs) is close to the resonance frequency (fR) then
the shape of the resonant tank current is piecewise sinusoidal. Otherwise, when fs >> fR
then the shape of the resonant tank current is piecewise linear.
For the purpose of the analysis both the magnetizing current and the AC voltage across the
tank capacitor Cres are negligible.
Considering that the square wave voltage applied to the resonant tank has 50% duty cycle,
it is possible to state:
Equation 6
Furthermore the output current is given by the superposition of the currents through the
secondary rectifier (Dout) and is a series of contiguous triangles. The DC output current is
equal to half of the resonant current peak value multiplied by transfer ratio (n = NPRI /
NSEC).
Equation 7
It can be demonstrated that the switching frequency of the converter is represented by
Equation 8:
Equation 8
The half-bridge frequency depends directly on the input voltage and inversely on the LED
current and depends on the difference between the square of the input voltage and the
reflected value of the output voltage.
It should be noted that the half-bridge frequency has a hyperbolical behavior depending on
the output power (ILED, VLED). This behavior is the main difference when compared to
an LLC or LCC resonant converter (see AN2644 and AN2450 on www.st.com).
The LC minimum operating frequency is obtained at the maximum output current, maximum
output voltage and minimum PFC output voltage. The maximum frequency is, instead,
obtained at the minimum output current (ILED, min), minimum output voltage (consider
short-circuit if required) and maximum input voltage.
(
)
Vpfc
2
1
Vdout
VLED
n
⋅
<
+
⋅
(
)
Vpfc
2
1
Cres
V
⋅
≈
pk
Ires,
2
n
ILED
⋅
≈
(
)
[
]
Vpfc
Vdout
VLED
2n
Vpfc
Lres
ILED
16
n
f
2
2
hb
+
⋅
−
⋅
⋅
⋅
=



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