参数资料
| 型号： | LTC3565IMSE#TRPBF |
| 厂商： | Linear Technology |
| 文件页数： | 10/22页 |
| 文件大小： | 0K |
| 描述： | IC REG BUCK SYNC ADJ 10MSOP |
| 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： | 0.6 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： | 1.25A |
| 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-TFSOP，10-MSOP（0.118"，3.00mm 宽）裸露焊盘 |
| 包装： | 带卷 (TR) |
| 供应商设备封装： | 10-MSOP 裸露焊盘 |
LTC3565
APPLICATIONS INFORMATION
V OUT ?
V OUT
? ?? 1 ?
V IN(MAX) ? ?
A general LTC3565 application circuit is shown in
Figure 4. External component selection is driven by the load
requirement, and begins with the selection of the induc-
tor L1. Once L1 is chosen, C IN and C OUT can be selected.
Operating Frequency
Selection of the operating frequency is a trade-off 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 LTC3565 is determined
by an external resistor that is connected between the RT
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:
inductances, but results in higher output ripple voltage,
greater core loss and lower output capability.
A reasonable starting point for setting ripple current is
Δ I L = 0.4 ? I OUT(MAX) , where I OUT(MAX) is 1.25A. The largest
ripple current Δ 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 = ?
f O ? Δ I L ?
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 induc-
tance values will cause the burst frequency to increase.
f O(MAX) ≈ 6.67 ?
V OUT
R T =1.21×10 6 (f O ) –1.2674 (kΩ)
where R T is in kΩ and f O is in kHz or can be selected us-
ing Figure 1.
The maximum usable operating frequency is limited by
the minimum on-time and the duty cycle. This can be
calculated as:
(MHz)
V IN(MAX)
5000
4500
4000
3500
3000
2500
2000
1500
1000
500
T A = 25°C
The minimum frequency is limited by leakage and noise
coupling due to the large resistance of R T .
0
0
100
200
300
R T (k )
400
500
600
3565 F01
V OUT ?
? ? 1 ? OUT ?
f O ? L ?
V IN ?
InductorSelection
The operating frequency, f O , has a direct effect on the
inductor value, which in turn influences the inductor ripple
current, Δ I L :
V ?
Δ I L =
The inductor ripple current decreases with larger induc-
tance or frequency, and increases with higher V IN or V OUT .
Accepting larger values of Δ I L allows the use of lower
Figure 1. Frequency vs R T
Inductor Core Selection
Different core materials and shapes will change the
size/current and price/current relationship of an induc-
tor. 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 characteristics. 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 LTC3565 requires to operate. Table 1
3565fc
10
For more information www.linear.com/LTC3565
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