English
Language : 

MIC2165_1011 Datasheet, PDF (20/28 Pages) Micrel Semiconductor – Adaptive On-Time DC-DC Controller Featuring HyperLight Load®
Micrel, Inc.
MIC2165
Solving for RS:
RS =
LP
Cp
With the feedforward capacitor, VFB ripple is very close to
the output voltage ripple:
(33)
ΔVFB(pp) ≈ ΔVOUT
(36)
Figure 7 shows the snubber in the circuit and the damped
switch node waveform. The snubber capacitor, CS, is
charged and discharged each switching cycle. The energy
stored in CS is dissipated by the snubber resistor, RS, two
times per switching period. This power is calculated in
Equation 34:
3) Virtually no ripple at VOUT due to the very low ESR of the
output capacitors.
In this situation, the output voltage ripple is less than 20mV.
Therefore, additional ripple is injected into the FB pin from
the switching node SW via a resistor Rinj and a capacitor
Cinj, as shown in Figure 8c. The injected ripple is:
PSNUBBER = fSW × CS × VIN2
(34)
Ripple Injection
The VFB ripple required for proper operation of the
MIC2165 gm amplifier and error comparator is 20mV to
100mV. However, the output voltage ripple is generally
designed as 1% to 2% of the voltage. For a low output
voltage, such as a 1V output, the output voltage ripple is
only 10mV to 20mV, and the VFB ripple is less than 20mV.
If the VFB ripple is so small that the gm amplifier and error
comparator cannot sense it, the MIC2165 will lose control
and the output voltage is not regulated. In order to have
some amount of VFB ripple, a ripple injection method is
applied for low output voltage ripple applications.
The applications are divided into three situations according
to the amount of the VFB ripple:
1) Enough ripple at VOUT due to the large ESR of the
output capacitors.
As shown in Figure 8a, the converter is stable without any
ripple injection. The VFB ripple is:
ΔVFB(PP)
=
VIN
× K div
× D × (1- D) ×
1
fSW × τ
K div
=
R1//R2
Rinj + R1//R2
(37)
(38)
where:
VIN = Power stage input voltage at VIN pin
D = Duty Cycle
fSW = switching frequency
τ = (R1// R2 // Rinj ) ⋅ Cff
In Equations 37 and 38, it is assumed that the time
constant associated with Cff must be much greater than
the switching period:
1 = T << 1
fSW × τ τ
ΔVFB(pp)
=
R2
R1+ R2
×
ΔVOUT
(35)
where: ΔVOUT = ESRCOUT ⋅ ΔIL(PP) , ΔIL(PP) is the peak-to-
peak value of the inductor current ripple.
If the voltage divider resistors R1 and R2 are in the kΩ
range, a Cff of 1nF to 100nF can easily satisfy the large
time constant consumption. Also, a 100nF injection
capacitor Cinj is used in order to be considered as short for
a wide range of the frequencies.
2) Inadequate ripple at VOUT due to the small ESR of the
output capacitors.
The output voltage ripple is fed into the FB pin through a
feedforward capacitor Cff in this situation, as shown in
Figure 8b. The typical Cff value is between 1nF and 100nF.
Figure 8a.
R2
R1+ R2
× ΔVOUT
>
20mV
September 2010
20
M9999-092410-E