参数资料
型号: NCP3121QPBCKGEVB
厂商: ON Semiconductor
文件页数: 15/41页
文件大小: 0K
描述: EVAL BOARD FOR NCP3121QPBCKG
设计资源: NCP3121 EVB BOM
NCP3121QPBCKGEVB Gerber Files
NCP3121QPBCKGEVB Schematic
标准包装: 1
主要目的: DC/DC,步降
输出及类型: 2,非隔离
输出电压: 3.3V,5V
电流 - 输出: 3A,3A
输入电压: 12V
稳压器拓扑结构: 降压
板类型: 完全填充
已供物品:
已用 IC / 零件: NCP3121
其它名称: NCP3121QPBCKGEVBOS
NCP3121
APPLICATION & DESIGN INFORMATION
I LP + I LOAD ) 1 D I L
V OUT V IN * V OUT
V IN @ D I L @ f OSC
I LP + I LOAD )
Inductor
The output inductor may be the most critical component
in the converter because it will directly affect the choice of
other components and dictate both the steady state and
transient performance of the converter. When choosing
inductors, one might have to consider maximum load
current, core and copper losses, component height, output
ripple, EMI, saturation and cost. Lower inductor values are
chosen to reduce the physical size of the inductor. A higher
value cuts down the ripple current and core losses and allows
more output current. In general, the output inductance value
should be as low and the output inductor physically as small
as possible to provide the best transient response and
minimum cost. If a large inductance value is used, the
converter will not respond quickly to rapid changes in the
load current. On the other hand, an inductance value that is
too low will result in very large ripple currents in the power
components, resulting in increased dissipation and lower
converter efficiency.
A good standard for determining the inductance to use is
to select the inductor peak ? to ? peak ripple current to be
approximately 25% of the maximum switch current. Also,
make sure that the inductor peak current is below the
maximum switch current limit and the selected inductor type
saturation current specification is higher than the peak
current through the switch.
The maximum current in the inductor while operating in
the continuous current mode is defined as the load current
plus one half of the D I L currrent:
2
The inductance value can be calculated by:
L +
Therefore, the inductor peak current, I LP , can be
calculated by:
V OUT V IN * V OUT
2 @ V IN @ L @ f OSC
where;
I LOAD is the output load current
V OUT is the output voltage
V IN is the input voltage
D I L is the peak ? to ? peak inductor ripple current
f OSC is the switching frequency of the oscillator
The choice of the appropriate inductor type depends not
only on the calculated inductance value, saturation current
rating and parasitic serial resistance, but also on the required
physical dimensions, EMI requirements (shielded or open
inductor) and the price. Examples of suitable inductors from
various manufacturers are shown in the table below.
Table 1. Calculated Inductor Values
Calculated coils, I ripple peak ? peak 20%
f [kHz]
200
350
500
750
I out [A]
12 V in to 7.5 V out
12 V in to 5 V out
12 V in to 3.3 V out
5 V in to 3.3 V out
5 V in to 2.5 V out
5 V in to 1.8 V out
2A
3A
2A
3A
2A
3A
2A
2A
2A
3A
36 m H
24 m H
36 m H
24 m H
30 m H
20 m H
14 m H
16 m H
15 m H
10 m H
20 m H
14 m H
20 m H
14 m H
17 m H
12 m H
8 m H
9 m H
8.2 m H
5.5 m H
14 m H
10 m H
15 m H
10 m H
12 m H
8 m H
5.6 m H
6.3 m H
5.8 m H
3.8 m H
10 m H
6.5 m H
10 m H
6.5 m H
8 m H
5.4 m H
3.7 m H
4 m H
3.8 m H
2.6 m H
http://onsemi.com
15
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