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TPS61196 参数 Datasheet PDF下载

TPS61196图片预览
型号: TPS61196
PDF下载: 下载PDF文件 查看货源
内容描述: 6串400 mA的WLED驱动器,带有独立的PWM调光的每个字符串 [6-String 400-mA WLED Driver with Independent PWM Dimming for Each String]
分类和应用: 驱动器
文件页数/大小: 30 页 / 1948 K
品牌: TI [ TEXAS INSTRUMENTS ]
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TPS61196  
www.ti.com  
SLVSBG1C OCTOBER 2012REVISED FEBRUARY 2013  
APPLICATION INFORMATION  
Inductor Selection  
The inductor is the most important component in switching power regulator design because it affects power  
supply steady state operation, transient behavior, and loop stability. The inductor value, dc resistance and  
saturation current are important specifications to be considered for better performance. Although the boost power  
stage can be designed to operate in discontinuous mode at maximum load, where the inductor current ramps  
down to zero during each switching cycle, most applications will be more efficient if the power stage operates in  
continuous conduction mode, where a DC current flows through the inductor. Therefore, the Equation 8 and  
Equation 9 below are for CCM operation only. The TPS61196 is designed to work with inductor values between  
10 µH and 100 µH, depending on the switching frequency. Running the controller at higher switching frequencies  
allows the use of smaller and/or lower profile inductors in the 10µH range. Running the controller at slower  
switching frequencies requires the use of larger inductors, near 100µH, to maintain the same inductor current  
ripple but may improve overall efficiency due to smaller switching losses. Inductor values can have ±20%  
tolerance with no current bias. When the inductor current approaches saturation level, its inductance can  
decrease 20% to 35% from the 0A value depending on how the inductor vendor defines saturation.  
In a boost regulator, the inductor DC current can be calculated with Equation 7.  
VOUT ´ IOUT  
IL(DC)  
=
V
´ η  
IN  
(7)  
Where:  
VOUT = boost output voltage  
IOUT = boost output current  
VIN = boost input voltage  
η = power conversion efficiency, use 95% for TPS61196 applications  
The inductor current peak-to-peak ripple can be calculated with Equation 8.  
V ´ V  
- V  
IN  
(
L ´ fSW ´ VOUT  
)
IN  
OUT  
DIL(P-P)  
=
(8)  
Where:  
ΔIL(P-P) = inductor ripple current  
L = inductor value  
fSW = switching frequency  
VOUT = boost output voltage  
VIN = boost input voltage  
Therefore, the inductor peak current is calculated with Equation 9.  
DIL(P-P)  
IL(P) = IL(DC)  
+
2
(9)  
Select an inductor, which saturation current is higher than calculated peak current. To calculate the worst case  
inductor peak current, use the minimum input voltage, maximum output voltage and maximum load current.  
Regulator efficiency is dependent on the resistance of its high current path and switching losses associated with  
the switch FET and power diode. Besides the external switch FET, the overall efficiency is also affected by the  
inductor DC resistance (DCR). Usually the lower dc resistance shows higher efficiency. However, there is a trade  
off between DCR and inductor footprint; furthermore, shielded inductors typically have higher DCR than  
unshielded ones.  
Schottky Diode  
The TPS61196 demands a high-speed rectification for optimum efficiency. Ensure that the diode's average and  
peak current rating exceed the output LED current and inductor peak current. In addition, the diode's reverse  
breakdown voltage must exceed the application output voltage.  
Copyright © 2012–2013, Texas Instruments Incorporated  
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