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參數(shù)資料
| 型號： | ISL6557CB-T |
| 廠商： | INTERSIL CORP |
| 元件分類： | 穩(wěn)壓器 |
| 英文描述： | Multi-Phase PWM Controller for Core-Voltage Regulation |
| 中文描述： | SWITCHING CONTROLLER, 1500 kHz SWITCHING FREQ-MAX, PDSO24 |
| 封裝： | PLASTIC, MS-013AD, SOIC-24 |
| 文件頁數(shù)： | 12/17頁 |
| 文件大?。?/td> | 532K |
| 代理商： | ISL6557CB-T |
12
The one-cycle uncertainty in Equation 9 is due to the
possibility that the VID code change may occur up to one full
cycle before being recognized. The time required for a
converter running with f
S
= 500kHz to make a 1.5V to 1.7V
reference-voltage change is between 30
μ
s and 32
μ
s as
calculated using Equation 9. This example is also illustrated
in Figure 11.
General Design Guide
This design guide is intended to provide a high-level
explanation of the steps necessary to create a multi-phase
power converter. It is assumed that the reader is familiar with
many of the basic skills and techniques referenced below. In
addition to this guide, Intersil provides complete reference
designs that include schematics, bills of materials, and
example board layouts for all common microprocessor
applications.
Power Stages
The first step in designing a multi-phase converter is to
determine the number of phases. This determination
depends heavily on the cost analysis which in turn depends
on system constraints that differ from one design to the next.
Principally, the designer will be concerned with whether
components can be mounted on both sides of the circuit
board; whether through-hole components are permitted on
either side; and the total board space available for power-
supply circuitry. Generally speaking, the most economical
solutions will be for each phase to handle between 15A and
20A. All-surface-mount designs will tend toward the lower
end of this current range and, if through-hole MOSFETs can
be used, higher per-phase currents are possible. In cases
where board space is the limiting constraint, current can be
pushed as high as 30A per phase, but these designs require
heat sinks and forced air to cool the MOSFETs.
MOSFETs
The choice of MOSFETs depends on the current each
MOSFET will be required to conduct; the switching frequency;
the capability of the MOSFETs to dissipate heat; and the
availability and nature of heat sinking and air flow.
LOWER MOSFET POWER CALCULATION
The calculation for heat dissipated in the lower MOSFET is
simple, since virtually all of the heat loss in the lower
MOSFET is due to current conducted through the channel
resistance (r
DS(ON)
). In Equation 10, I
M
is the maximum
continuous output current; I
L,PP
is the peak-to-peak inductor
current (see Equation 1); d is the duty cycle (V
OUT
/V
IN
); and
L is the per-channel inductance.
An additional term can be added to the lower-MOSFET loss
equation to account for additional loss accrued during the
dead time when inductor current is flowing through the
lower-MOSFET body diode. This term is dependent on the
diode forward voltage at I
M
, V
D(ON)
; the switching
frequency, f
S
; and the length of dead times, t
d1
and t
d2
, at
the beginning and the end of the lower-MOSFET conduction
interval respectively.
Thus the total power dissipated in each lower MOSFET is
approximated by the summation of P
L
and P
D
.
UPPER MOSFET POWER CALCULATION
In addition to r
DS(ON)
losses, a large portion of the upper-
MOSFET losses are due to currents conducted across the
input voltage (V
IN
) during switching. Since a substantially
higher portion of the upper-MOSFET losses are dependant
on switching frequency, the power calculation is somewhat
more complex. Upper MOSFET losses can be divided into
separate components involving the upper-MOSFET
switching times; the lower-MOSFET body-diode reverse-
recovery charge, Q
rr
; and the upper MOSFET r
DS(ON)
conduction loss.
When the upper MOSFET turns off, the lower MOSFET
does not conduct any portion of the inductor current until the
voltage at the phase node falls below ground. Once the
lower MOSFET begins conducting, the current in the upper
MOSFET falls to zero as the current in the lower MOSFET
ramps up to assume the full inductor current. In Equation 12,
the required time for this commutation is t
1
and the
associated power loss is P
UP,1
.
Similarly, the upper MOSFET begins conducting as soon as
it begins turning on. In Equation 13, this transition occurs
over a time t
2
, and the approximate the power loss is P
UP,2
.
A third component involves the lower MOSFET’s reverse-
recovery charge, Q
rr
. Since the inductor current has fully
commutated to the upper MOSFET before the lower-
MOSFET’s body diode can recover all of Q
rr
, it is conducted
through the upper MOSFET across VIN. The power
dissipated as a result is P
UP,3
and is simply
1
f
S
----
2 V
----------------
1
–
t
DV
1
f
S
----
2 V
ID
----------------
≤
<
(EQ. 9)
P
LOW 1
,
r
DS ON
(
)
I
M
N
-----
2
1
d
–
(
)
I
,
-------------------------------
2
1
(
d
–
)
+
=
(EQ. 10)
P
LOW 2
,
V
D ON
(
)
f
S
I
M
N
-----
I
--------
+
t
d1
I
M
N
-----
I
--------
–
t
d2
+
=
(EQ. 11)
P
UP 1
,
V
IN
I
M
N
-----
I
,
-------------
+
t
1
2
----
f
S
≈
(EQ. 12)
P
UP 2
,
V
IN
I
M
N
-----
I
,
-------------
–
t
2
2
----
f
S
≈
(EQ. 13)
P
UP 3
,
V
IN
Q
rr
f
S
=
(EQ. 14)
ISL6557
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相關(guān)代理商/技術(shù)參數(shù) |
參數(shù)描述 |
|---|---|
| ISL6557CB-T WAF | 制造商:Intersil Corporation 功能描述: |
| ISL6558CB | 功能描述:DC/DC 開關(guān)控制器 Precision MultiPhase RoHS:否 制造商:Texas Instruments 輸入電壓:6 V to 100 V 開關(guān)頻率: 輸出電壓:1.215 V to 80 V 輸出電流:3.5 A 輸出端數(shù)量:1 最大工作溫度:+ 125 C 安裝風(fēng)格: 封裝 / 箱體:CPAK |
| ISL6558CB-T | 功能描述:IC REG CTRLR BUCK PWM 16-SOIC RoHS:否 類別:集成電路 (IC) >> PMIC - 穩(wěn)壓器 - DC DC 切換控制器 系列:- 標(biāo)準(zhǔn)包裝:4,000 系列:- PWM 型:電壓模式 輸出數(shù):1 頻率 - 最大:1.5MHz 占空比:66.7% 電源電壓:4.75 V ~ 5.25 V 降壓:是 升壓:無 回掃:無 反相:無 倍增器:無 除法器:無 Cuk:無 隔離:無 工作溫度:-40°C ~ 85°C 封裝/外殼:40-VFQFN 裸露焊盤 包裝:帶卷 (TR) |
| ISL6558CBZ | 制造商:Intersil Corporation 功能描述:- Rail/Tube |
| ISL6558CBZA | 功能描述:DC/DC 開關(guān)控制器 W/ANNEAL 16LD N 2-4 PHS PWM BUCK CNTRLR RoHS:否 制造商:Texas Instruments 輸入電壓:6 V to 100 V 開關(guān)頻率: 輸出電壓:1.215 V to 80 V 輸出電流:3.5 A 輸出端數(shù)量:1 最大工作溫度:+ 125 C 安裝風(fēng)格: 封裝 / 箱體:CPAK |
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