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LTC1430CS8#TR 参数 Datasheet PDF下载

LTC1430CS8#TR图片预览
型号: LTC1430CS8#TR
PDF下载: 下载PDF文件 查看货源
内容描述: [暂无描述]
分类和应用: 稳压器开关光电二极管控制器
文件页数/大小: 16 页 / 214 K
品牌: Linear [ Linear ]
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LTC1430  
U
W U U  
APPLICATIO S I FOR ATIO  
Once the threshold voltage has been selected, RON should  
be chosen based on input and output voltage, allowable  
power dissipation and maximum required output current.  
In a typical LTC1430 buck converter circuit operating in  
continuous mode, the average inductor current is equal to  
the output load current. This current is always flowing  
through either M1 or M2 with the power dissipation split  
up according to the duty cycle:  
Note that the required RON for M2 is roughly twice that of  
M1 in this example. This application might specify a single  
0.03device for M2 and parallel two more of the same  
devices to form M1. Note also that while the required RON  
values suggest large MOSFETs, the dissipation numbers  
are only 1.1W per device or less—large TO-220 packages  
and heat sinks are not necessarily required in high effi-  
ciency applications. Siliconix Si4410DY (in SO-8) and  
Motorola MTD20N03HL (in DPAK) are two small, surface  
mount devices with RON values of 0.03or below with 5V  
of gate drive; both work well in LTC1430 circuits with up  
to 10A output current. A higher PMAX value will generally  
decrease MOSFET cost and circuit efficiency and increase  
MOSFET heat sink requirements.  
VOUT  
V
IN  
DC (M1) =  
VOUT  
V
IN  
DC (M2) = 1−  
V V  
(
)
IN  
OUT  
=
Inductor  
V
IN  
TheinductorisoftenthelargestcomponentinanLTC1430  
design and should be chosen carefully. Inductor value and  
type should be chosen based on output slew rate require-  
mentsandexpectedpeakcurrent. Inductorvalueisprima-  
rily controlled by the required current slew rate. The  
maximum rate of rise of the current in the inductor is set  
byitsvalue,theinput-to-outputvoltagedifferentialandthe  
maximum duty cycle of the LTC1430. In a typical 5V to  
3.3V application, the maximum rise time will be:  
The RON required for a given conduction loss can now be  
calculated by rearranging the relation P = I2R:  
PMAX(M1)  
RON (M1) =  
2
DC (M1)IMAX  
V PMAX(M1)  
IN  
=
2
VOUT IMAX  
V V  
(
)
AMPS  
SECOND  
1.53A I  
µs L  
IN  
OUT  
PMAX(M2)  
90%•  
=
RON (M2) =  
L
2
DC (M2)IMAX  
where L is the inductor value in µH. A 2µH inductor would  
have a 0.76A/µs rise time in this application, resulting in a  
6.5µsdelayinrespondingtoa5Aloadcurrentstep.During  
this6.5µs,thedifferencebetweentheinductorcurrentand  
the output current must be made up by the output capaci-  
tor, causing a temporary droop at the output. To minimize  
this effect, the inductor value should usually be in the 1µH  
to 5µH range for most typical 5V to 3.xV LTC1430 circuits.  
Different combinations of input and output voltages and  
expected loads may require different values.  
V PMAX(M2)  
IN  
=
2
V V  
I  
MAX  
(
)
IN  
OUT  
PMAX should be calculated based primarily on required  
efficiency. A typical high efficiency circuit designed for 5V  
in, 3.3V at 10A out might require no more than 3%  
efficiency loss at full load for each MOSFET. Assuming  
roughly 90% efficiency at this current level, this gives a  
MAX value of (3.3V • 10A/0.9) • 0.03 = 1.1W per FET and  
a required RON of:  
P
Once the required value is known, the inductor core type  
can be chosen based on peak current and efficiency  
requirements. Peak current in the inductor will be equal to  
the maximum output load current added to half the peak-  
to-peakinductorripplecurrent.Ripplecurrentissetbythe  
5V 1.1W  
RON (M1) =  
= 0.017Ω  
3.3V 10A2  
5V 1.1W  
RON (M2) =  
= 0.032Ω  
5V 3.3V 10A2  
(
)
8
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