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MIC2133 数据表(PDF) 32 Page - Microchip Technology

部件名 MIC2133
功能描述  75V Dual Phase, Advanced COT Buck Controller with Selectable Droop Feature and Phase Shedding
PDF  50 Pages
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制造商  MICROCHIP [Microchip Technology]
网页  http://www.microchip.com
标志 MICROCHIP - Microchip Technology

MIC2133 数据表(HTML) 32 Page - Microchip Technology

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DS20006653B-page 32
MIC2133
5.0
APPLICATION INFORMATION
5.1
Inductor Selection
Certain values for inductance, peak and RMS currents
are required to select the output inductor. The input and
output voltages, as well as the inductance value,
determine the peak-to-peak inductor ripple current.
Generally, higher inductance values are used with
higher input voltages. Larger peak-to-peak ripple
currents increase the power dissipation in the inductor
and MOSFETs. Larger output ripple currents also
require more output capacitance to smooth out the
larger ripple current. Smaller peak-to-peak ripple
currents require a larger inductance value, and there-
fore, a larger and more expensive inductor. Higher
switching frequencies allow the use of a small
inductance, but increase power dissipation in the
inductor core and MOSFET switching loss. A good
compromise between size, loss and cost is to set the
inductor ripple current to be equal to 20% of the
maximum DC output current contributed per phase.
The inductance value of the inductor in each phase
channel is calculated by the equation below.
EQUATION 5-1:
The peak-to-peak inductor current ripple in each phase is:
EQUATION 5-2:
The peak inductor current per phase is equal to the
maximum average output current per phase, plus one
half of the peak-to-peak inductor current ripple, as
given in the following equation.
EQUATION 5-3:
The RMS inductor current in each phase is used to
calculate the I2R losses in the inductor per phase.
EQUATION 5-4:
Maximizing efficiency requires selecting the proper core
material and minimizing the winding resistance. The
high-frequency operation of the MIC2133 requires the
use of ferrite materials for all but the most cost-sensitive
applications. Lower cost iron powder cores may be
used, but the increase in core loss reduces the efficiency
of the buck converter. This is especially noticeable at low
output power. The winding resistance decreases
efficiency at the higher output current levels. The wind-
ing resistance must be minimized, although this usually
comes at the expense of a larger inductor size. The
power dissipated in the inductor is equal to the sum of
the core and copper losses. At higher output loads, the
core losses are usually insignificant and can be ignored.
At lower output currents, the core losses can be a
significant contributor. Core loss information is usually
available from the magnetics vendor. Copper loss in the
inductor is calculated by the equation below.
EQUATION 5-5:
The resistance of the copper wire, RWINDING, increases
with the temperature.The value of the winding resis-
tance used must be at the operating temperature for
accurate power dissipation estimation, as calculated in
the equation below:
EQUATION 5-6:
L
VOUT
Eff VIN MAX

VOUT

NPH
Eff VIN MAX

fSW
0.2
IOUT MAX

---------------------------------------------------------------------------------------------------
=
Where:
fSW = Switching Frequency, 500 kHz
0.2 = Ratio of AC Ripple Current to
Maximum DC Output Current
Contributed per Phase
VIN(MAX) = Maximum Power Stage Input Voltage
NPH = Total Number of Phases
Eff = Efficiency of the Buck Converter
IOUT(MAX) = Maximum DC Output Current
I
LPP

VOUT
Eff VIN MAX

VOUT

Eff VIN MAX

fSW
L
----------------------------------------------------------------------------------
=
IL_PH PK

IOUTPH MAX

0.5
I
LPP

+
=
Where:
IOUTPH(MAX) = Maximum Average DC Output Current
Contributed per Phase
IOUT(MAX) = Maximum Output Current
n = Total Number of Phases
IOUTPH MAX

IOUT MAX

n
--------------------------
=
IL_PH RMS

IOUTPH MAX

2
I
LPP

2
12
---------------------
+
=
PINDUCTOR Cu

IL_PH RMS

2
RWINDING
=
RWINDING HT

RWINDING 20C

10.0042
TH T20C

+

=
Where:
TH = Temperature of Wire Under Full Load
T20°C = Ambient Room Temperature
RWINDING(20°C) = Room Temperature Winding
Resistance (usually specified by the
manufacturer)



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