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参数资料
| 型号： | LTC3568IDD#TRPBF |
| 厂商： | Linear Technology |
| 文件页数： | 8/18页 |
| 文件大小： | 0K |
| 描述： | IC REG BUCK SYNC ADJ 1.8A 10DFN |
| 标准包装： | 2,500 |
| 类型： | 降压（降压） |
| 输出类型： | 可调式 |
| 输出数： | 1 |
| 输出电压： | 0.8 V ~ 5 V |
| 输入电压： | 2.5 V ~ 5.5 V |
| PWM 型： | 电流模式，混合 |
| 频率 - 开关： | 最高 4MHz |
| 电流 - 输出： | 1.8A |
| 同步整流器： | 是 |
| 工作温度： | -40°C ~ 125°C |
| 安装类型： | 表面贴装 |
| 封装/外壳： | 10-WFDFN 裸露焊盘 |
| 包装： | 带卷 (TR) |
| 供应商设备封装： | 10-DFN（3x3） |
LTC3568
APPLICATIONS INFORMATION
V OUT ?
V OUT
? Δ I
f O L
V IN ( MAX ) ?
A general LTC3568 application circuit is shown in
Figure 5. External component selection is driven by the load
requirement, and begins with the selection of the inductor
L1. Once L1 is chosen, C IN and C OUT can be selected.
Operating Frequency
Selection of the operating frequency is a tradeoff between
efficiency and component size. High frequency operation
allows the use of smaller inductor and capacitor values.
Operation at lower frequencies improves efficiency by
reducing internal gate charge losses but requires larger
inductance values and/or capacitance to maintain low
output ripple voltage.
The operating frequency, f O , of the LTC3568 is determined
by an external resistor that is connected between the R T
pin and ground. The value of the resistor sets the ramp
current that is used to charge and discharge an internal
timing capacitor within the oscillator and can be calculated
by using the following equation:
A reasonable starting point for setting ripple current is
Δ I L = 0.4 ? I OUT , where I OUT is the maximum output cur-
rent. The largest ripple current ?I L occurs at the maximum
input voltage. To guarantee that the ripple current stays
below a specified maximum, the inductor value should be
chosen according to the following equation:
?
L = ? ? 1 ? ?
?
The inductor value will also have an effect on Burst Mode
operation. The transition from low current operation
begins when the peak inductor current falls below a level
set by the burst clamp. Lower inductor values result in
higher ripple current which causes this to occur at lower
load currents. This causes a dip in efficiency in the upper
range of low current operation. In Burst Mode operation,
lower inductance values will cause the burst frequency
to increase.
R T = 9 . 78 ? 10
11
( f O )
? 1 . 08
( Ω )
4.5
4.0
T A = 25°C
or can be selected using Figure 2.
The maximum usable operating frequency is limited by
the minimum on-time and the duty cycle. This can be
calculated as:
3.5
3.0
2.5
2.0
1.5
f O(MAX) ≈ 6.67 ? (V OUT / V IN(MAX) ) (MHz)
The minimum frequency is limited by leakage and noise
coupling due to the large resistance of R T .
1.0
0.5
0
0
500
R T (k )
1000
1500
3568 F02
? ? 1 ? OUT ?
V OUT ? V ?
Δ I L =
Inductor Selection
Although the inductor does not influence the operat-
ing frequency, the inductor value has a direct effect on
ripple current. The inductor ripple current Δ I L decreases
with higher inductance and increases with higher V IN or
V OUT :
f O ? L ? V IN ?
Accepting larger values of Δ I L allows the use of low induc-
tances, but results in higher output voltage ripple, greater
core losses, and lower output current capability.
Figure 2. Frequency vs R T
Inductor Core Selection
Different core materials and shapes will change the size/cur-
rent and price/current relationship of an inductor. Toroid or
shielded pot cores in ferrite or permalloy materials are small
and don’t radiate much energy, but generally cost more than
powdered iron core inductors with similar electrical char-
acteristics. The choice of which style inductor to use often
depends more on the price vs size requirements and any
radiated field/EMI requirements than on what the LTC3568
requires to operate. Table 1 shows some typical surface
mount inductors that work well in LTC3568 applications.
3568fa
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