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參數(shù)資料
| 型號： | LTC3633EUFD#TRPBF |
| 廠商： | LINEAR TECHNOLOGY CORP |
| 元件分類： | 穩(wěn)壓器 |
| 英文描述： | SWITCHING REGULATOR, PQCC28 |
| 封裝： | 4 X 5 MM, LEAD FREE, PLASTIC, MO-220, QFN-28 |
| 文件頁數(shù)： | 4/28頁 |
| 文件大?。?/td> | 384K |
| 代理商： | LTC3633EUFD#TRPBF |
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LTC3633
12
3633f
APPLICATIONS INFORMATION
A general LTC3633 application circuit is shown on the
rst page of this data sheet. External component selection
is largely driven by the load requirement and switching
frequency. Component selection typically begins with
the selection of the inductor L and resistor RT. Once the
inductor is chosen, the input capacitor, CIN, and the out-
put capacitor, COUT, can be selected. Next, the feedback
resistors are selected to set the desired output voltage.
Finally, the remaining optional external components can be
selected for functions such as external loop compensation,
track/soft-start, VIN UVLO, and PGOOD.
Programming Switching Frequency
Selection of the switching frequency is a trade-off between
efciency and component size. High frequency operation
allows the use of smaller inductor and capacitor values.
Operation at lower frequencies improves efciency by
reducing internal gate charge losses but requires larger
inductance values and/or capacitance to maintain low
output ripple voltage.
Connecting a resistor from the RT pin to SGND programs
the switching frequency (f) between 500kHz and 4MHz
according to the following formula:
RRT =
3.2E
11
f
where RRT is in Ω and f is in Hz.
When RT is tied to INTVCC, the switching frequency will
default to approximately 2MHz, as set by an internal re-
sistor. This internal resistor is more sensitive to process
and temperature variations than an external resistor
(see Typical Performance Characteristics) and is best used
for applications where switching frequency accuracy is
not critical.
Inductor Selection
For a given input and output voltage, the inductor value and
operating frequency determine the inductor ripple current.
More specically, the inductor ripple current decreases
with higher inductor value or higher operating frequency
according to the following equation:
IL =
VOUT
f L
1– VOUT
VIN
Where ΔIL=inductorripplecurrent,f=operatingfrequency
and L = inductor value. A trade-off between component
size, efciency and operating frequency can be seen from
this equation. Accepting larger values of ΔIL allows the
use of lower value inductors but results in greater inductor
core loss, greater ESR loss in the output capacitor, and
larger output voltage ripple. Generally, highest efciency
operation is obtained at low operating frequency with
small ripple current.
A reasonable starting point is to choose a ripple current
that is about 40% of IOUT(MAX). Note that the largest
ripple current occurs at the highest VIN. Exceeding 60%
of IOUT(MAX) is not recommended. To guarantee that
ripple current does not exceed a specied maximum, the
inductance should be chosen according to:
L =
VOUT
f IL(MAX)
1– VOUT
VIN(MAX)
Once the value for L is known, the type of inductor must
be selected. Actual core loss is independent of core size
for a xed inductor value, but is very dependent on the
inductance selected. As the inductance increases, core
losses decrease. Unfortunately, increased inductance
requires more turns of wire, leading to increased DCR
and copper loss.
0
FREQUENCY
(kHz)
1000
2000
3000
5000
200
700
600
3633 F01
0
6000
4000
100
300
400
500
RT RESISTOR (kΩ)
Figure 1. Switching Frequency vs RT
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