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SLVSAC4 Datenblatt(PDF) 12 Page - Texas Instruments

Teilenummer SLVSAC4
Bauteilbeschribung  TLV62065 3-MHz 2-A Step-Down Converter in 2 × 2 WSON Package
PDF  27 Pages
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Hersteller  TI2 [Texas Instruments]
Direct Link  https://www.ti.com
Logo TI2 - Texas Instruments

SLVSAC4 Datenblatt(HTML) 12 Page - Texas Instruments

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background image
L
L max
out max
I
I
I
2
D
=
+
L
Vout
1
Vin
I
Vout
L ƒ
-
D =
´
´
c
1
=
= 50kHz
2
(1 H
10 F)
f
p
´
´
´
TLV62065
SLVSAC4B – NOVEMBER 2010 – REVISED DECEMBER 2015
www.ti.com
Typical Application (continued)
8.2.2.2 Output Filter Design (Inductor and Output Capacitor)
The internal compensation network of TLV62065 is optimized for a LC output filter with a corner frequency of:
The device operates with nominal inductors of 1.0 µH to 1.2 µH and with 10 µF to 22 µF small X5R and X7R
ceramic capacitors. Please refer to the lists of inductors and capacitors. The device is optimized for a 1-µH
inductor and 10-µF output capacitor.
8.2.2.2.1
Inductor Selection
The inductor value has a direct effect on the ripple current. The selected inductor has to be rated for its DC
resistance and saturation current. The inductor ripple current (
ΔIL) decreases with higher inductance and
increases with higher VI or VO.
Equation 5 calculates the maximum inductor current in PWM mode under static load conditions. The saturation
current of the inductor should be rated higher than the maximum inductor current as calculated with Equation 6.
This is recommended because during heavy load transient the inductor current rises above the calculated value.
(5)
where
•
f = Switching frequency (3 MHz typical)
•
L = Inductor value
•
ΔIL = Peak-to-peak inductor ripple current
•
ILmax = Maximum inductor current
(6)
A more conservative approach is to select the inductor current rating just for the switch current limit ILIMF of the
converter.
The total losses of the coil have a strong impact on the efficiency of the DC–DC conversion and consist of both
the losses in the DC resistance R(DC) and the following frequency-dependent components:
•
The losses in the core material (magnetic hysteresis loss, especially at high switching frequencies)
•
Additional losses in the conductor from the skin effect (current displacement at high frequencies)
•
Magnetic field losses of the neighboring windings (proximity effect)
•
Radiation losses
Table 1. List of Inductors
DIMENSIONS [mm3]
INDUCTANCE
μH
INDUCTOR TYPE
SUPPLIER
3.2 x 2.5 x 1.0 max
1.0
LQM32PN (MLCC)
Murata
3.7 x 4 x 1.8 max
1.0
LQH44 (wire wound)
Murata
4.0 x 4.0 x 2.6 max
1.2
NRG4026T (wire wound)
Taiyo Yuden
3.5 x 3.7 x 1.8 max
1.2
DE3518 (wire wound)
TOKO
12
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Copyright © 2010–2015, Texas Instruments Incorporated
Product Folder Links: TLV62065



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