CS5171GDR8G ON Semiconductor, CS5171GDR8G Datasheet - Page 13

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CS5171GDR8G

Manufacturer Part Number
CS5171GDR8G
Description
IC MULTI CONFIG SYNC 1.5A 8SOIC
Manufacturer
ON Semiconductor
Type
Step-Up (Boost), Flyback, Forward Converter, Sepicr
Datasheet

Specifications of CS5171GDR8G

Internal Switch(s)
Yes
Synchronous Rectifier
No
Number Of Outputs
1
Current - Output
1.5A
Frequency - Switching
280kHz
Voltage - Input
2.7 ~ 30 V
Operating Temperature
0°C ~ 125°C
Mounting Type
Surface Mount
Package / Case
8-SOIC (3.9mm Width)
Output Current
1.5 A
Input Voltage
2.7 V to 30 V
Switching Frequency
280 KHz
Operating Temperature Range
0 C to + 125 C
Mounting Style
SMD/SMT
Duty Cycle (max)
94 %
Lead Free Status / RoHS Status
Lead free / RoHS Compliant
Voltage - Output
-
Power - Output
-
Lead Free Status / Rohs Status
Lead free / RoHS Compliant
Other names
CS5171GDR8GOSTR

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Part Number
Manufacturer
Quantity
Price
Part Number:
CS5171GDR8G
Manufacturer:
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20 000
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Part Number:
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Magnetic Component Selection
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 (V
assuming 100% energy transfer efficiency. In continuous
conduction mode, inductor ripple current is
where:
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
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 V
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.
When choosing a magnetic component, one must consider
The peak inductor current is equal to average current plus
In boost circuits, the inductor becomes part of the input
f = 280 kHz for CS5171/2 and 560 kHz for CS5173/4.
Figure 34. Boost Input Voltage and Current
I RIPPLE +
Ripple Waveforms
V CC (V OUT * V CC )
(f)(L)(V OUT)
CC
ripple. In most
OUT
V
I
I
IN
L
CC
http://onsemi.com
/V
ripple
CC
),
13
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 V
as close as possible to the chip.
Output Capacitor Selection
see that the output voltage ripple comes from two major
sources,
charging/discharging of the output capacitor. In boost
circuits, when the power switch turns off, I
output capacitor causing an instant DV = I
same time, current I
increases the output voltage gradually. When the power
switch is turned on, I
discharges the output capacitor. When the I
enough, I
current I
The situation is different in a flyback circuit. The input
By examining the waveforms shown in Figure 36, we can
V
Figure 35. Boost Circuit Effective Input Filter
CC
Figure 36. Typical Output Voltage Ripple
IN
L
.
can be treated as a constant and is equal to input
namely
+
L
L
− I
capacitor
is shunted to ground and I
I
IN
OUT
R
charges the capacitor and
ESR
C
IN
ESR
IN
L
L
CC
ripple is small
flows into the
× ESR. At the
I
and ground
and
L
V
I
L
OUT
ripple
OUT
the

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