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CS5172 데이터시트(PDF) 13 Page - ON Semiconductor

부품명 CS5172
상세설명  1.5 A 280 kHz/560 kHz Boost Regulators
PDF  22 Pages
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제조업체  ONSEMI [ON Semiconductor]
홈페이지  http://www.onsemi.com
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CS5172 데이터시트(HTML) 13 Page - ON Semiconductor

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CS5171, CS5172, CS5173, CS5174
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Magnetic Component Selection
When choosing a magnetic component, one must consider
factors such as peak current, core and ferrite material, output
voltage ripple, EMI, temperature range, physical size and
cost. In boost circuits, the average inductor current is the
product of output current and voltage gain (VOUT/VCC),
assuming 100% energy transfer efficiency. In continuous
conduction mode, inductor ripple current is
IRIPPLE +
VCC(VOUT * VCC)
(f)(L)(VOUT)
where:
f = 280 kHz for CS5171/2 and 560 kHz for CS5173/4.
The peak inductor current is equal to average current plus
half of the ripple current, which should not cause inductor
saturation. The above equation can also be referenced when
selecting the value of the inductor based on the tolerance of
the ripple current in the circuits. Small ripple current
provides the benefits of small input capacitors and greater
output current capability. A core geometry like a rod or
barrel is prone to generating high magnetic field radiation,
but is relatively cheap and small. Other core geometries,
such as toroids, provide a closed magnetic loop to prevent
EMI.
Input Capacitor Selection
In boost circuits, the inductor becomes part of the input
filter, as shown in Figure 35. In continuous mode, the input
current waveform is triangular and does not contain a large
pulsed current, as shown in Figure 34. This reduces the
requirements imposed on the input capacitor selection.
During continuous conduction mode, the peak to peak
inductor ripple current is given in the previous section. As
we can see from Figure 34, the product of the inductor
current ripple and the input capacitor’s effective series
resistance (ESR) determine the VCC ripple. In most
applications, input capacitors in the range of 10
mF to 100 mF
with an ESR less than 0.3
W work well up to a full 1.5 A
switch current.
VCC ripple
Figure 34. Boost Input Voltage and Current
Ripple Waveforms
IIN
IL
+
Figure 35. Boost Circuit Effective Input Filter
VCC
CIN
RESR
IL
IIN
The situation is different in a flyback circuit. The input
current is discontinuous and a significant pulsed current is
seen by the input capacitors. Therefore, there are two
requirements for capacitors in a flyback regulator: energy
storage and filtering. To maintain a stable voltage supply to
the chip, a storage capacitor larger than 20
mF with low ESR
is required. To reduce the noise generated by the inductor,
insert a 1.0
mF ceramic capacitor between VCC and ground
as close as possible to the chip.
Output Capacitor Selection
Figure 36. Typical Output Voltage Ripple
VOUT ripple
IL
By examining the waveforms shown in Figure 36, we can
see that the output voltage ripple comes from two major
sources,
namely
capacitor
ESR
and
the
charging/discharging of the output capacitor. In boost
circuits, when the power switch turns off, IL flows into the
output capacitor causing an instant
DV = IIN × ESR. At the
same time, current IL − IOUT charges the capacitor and
increases the output voltage gradually. When the power
switch is turned on, IL is shunted to ground and IOUT
discharges the output capacitor. When the IL ripple is small
enough, IL can be treated as a constant and is equal to input
current IIN.



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