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AN1882 Datasheet(PDF) 18 Page - STMicroelectronics

Part # AN1882
Description  This application note details the main features
PDF  30 Pages
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Manufacturer  STMICROELECTRONICS [STMicroelectronics]
Direct Link  http://www.st.com
Logo STMICROELECTRONICS - STMicroelectronics

AN1882 Datasheet(HTML) 18 Page - STMicroelectronics

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Application information
AN1882
18/30
Doc ID 10209 Rev 4
5.1.4
Compensation network (R1C3)
As it is shown in the
Section 3.2 the system stability can be studied with the loop transfer
function given by the
Equation 3Equation 3. If the output capacitor is a ceramic type the zero
due to the ESR generally will be out of the system bandwidth, so the stability of the system
will be ensured by the cancellation between the pole due to the output capacitor and the
equivalent load and the R1C3 zero. In the Equation 15Equation 15, a simplified gain loop
expression, valid around the transition frequency fT is given by:
Equation 15
Supposing C2 = 22 µF, the transition frequency at 0 dB equal to 30 kHz (fT is equal to the
system bandwidth), and the output voltage equal to 1.8 V the R1 value can be calculated as:
Equation 16
The nearest standard E12 series value is R1 = 47 kΩ.
The higher is the bandwidth, the faster will be the transient response but the bandwidth (and
so the R1 value) must be lower than fSW/10 to avoid the effect due to the sampling effect
poles as mentioned in the
Section 3.2. The zero due to the compensation network must be
at the least 5 times before the frequency transition, so the C3 value will be:
Equation 17
The nearest standard value is C3 = 470 pF. If the output capacitors are tantalum type the
ESR zero is in the system bandwidth and it can be used to stabilize the system so the zero
due to the compensation network will be useless (the C3 is necessary to the integrator
function).
5.2
Losses and efficiency
There are losses affecting the efficiency of the application. Some of these losses are related
to the device and others are related to the external components. The most important losses
are listed below.
5.2.1
Conduction losses
These losses are basically due to the not negligible resistances of the internal switches and
the external inductor. Usually the current ripple across the inductor is negligible and so to
estimate the conduction losses of the inductor, the average output current can be
considered. The conduction losses of the switches depend also on the duty cycle of the
application. The RMS current flowing through the high side MOSFET is (IO)
2 · D while the
RMS current flowing through the low side MOSFET is (IO)
2 · (1-D). So, the total conduction
losses are:
G
LOOP s
()
g
mR1α
sC
2
-------------------
=
R
1
2
πf
TC2
g
mα
-------------------
=
C
3
5
2
πf
TR1
-------------------
500pF
=
=



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