IR3720MTRPBF International Rectifier, IR3720MTRPBF Datasheet - Page 10

IC POWER SUPPLY MONITOR 10-DFN

IR3720MTRPBF

Manufacturer Part Number
IR3720MTRPBF
Description
IC POWER SUPPLY MONITOR 10-DFN
Manufacturer
International Rectifier
Series
TruePower™r
Datasheet

Specifications of IR3720MTRPBF

Package / Case
10-DFN
Mounting Type
Surface Mount
Current - Supply
480µA
Voltage - Supply
3.135 V ~ 3.465 V
Operating Temperature
0°C ~ 125°C
Applications
Power Supply Monitor
Voltage - Input
-
Input Voltage
3.3V
No. Of Outputs
1
Supply Voltage Range
3.135V To 3.465V
No. Of Pins
10
Operating Temperature Range
0°C To +125°C
Filter Terminals
SMD
Input Voltage Primary Max
3.3V
Rohs Compliant
Yes
Frequency
400kHz
Package
10 Lead 3x3 DFN
Vk Range
0.5V - 1.8V
Bias Supply Voltage
+3.3V +/-5%
Junction Temperature
0oC to 125oC
Pbf
Yes
Lead Free Status / RoHS Status
Lead free / RoHS Compliant
Voltage - Input
-
Lead Free Status / Rohs Status
Lead free / RoHS Compliant

Available stocks

Company
Part Number
Manufacturer
Quantity
Price
Part Number:
IR3720MTRPBF
Manufacturer:
WIMA
Quantity:
1 200
Company:
Part Number:
IR3720MTRPBF
Quantity:
1 888
INDUCTOR DCR CURRENT SENSING APPLICATION
Referring to the Functional Description Diagram, it
can be seen that the shunt function can be
accomplished by the DC resistance of the inductor
that is already present. Omitting the resistive shunt
reduces BOM cost and increases efficiency. In
exchange for these two significant advantages two
easily compensated design complications are
introduced, a time constant and a temperature
coefficient.
The inductor voltage sensed between the Rcs1
resistors is not simply proportional to the inductor
current, but rather is expressed in the Laplace
equation below.
This inductor time constant is canceled when
Let
A second equation is used to set the full scale
inductor current.
Page 10 of 20
I
R
DCR
FS
CS1
V
L
L
=
R
R
+
=
V
R
CS1
=
CS1
IG
R
Ι
T
L
R
R
CS2
+
CS1
CS1
R
(
DCR
R
R
CS2
=
CS2
CS1
+
R
R
DCR
R
sum
CS2
+
1
CS2
=
+
R
R
CS2
s
and solve for Rsum.
eq
DCR
C
.
L
CS1
)
. Let
.
www.irf.com
Select a standard value C
We now know Req and Rsum, but we do not know
the individual resistor values R
step is to solve for them simultaneously. By
substituting R
can be written:
Note that this equation is of the form
c=Req•Rsum. The roots of this quadratic equation
will be R
as R
and
R
R
R
R
ax
DCR
eq
2
CS1
CS1
CS1
2
+
4
=
CS1
=
=
bx
R
R
L
R
R
R
CS1
SUM
in order to minimize ripple current in C
CS1
CS1
+
SUM
SUM
R
c
sum
and R
R
=
. Solve for R
R
sum
CS2
1
1
0
sum
+
where a=0, b=-Rsum, and
into the R
, which can then be rearranged to
+
CS2
1
1
R
. Use the higher value resistor
2
eq
4
2
4
R
R
R
R
R
eq
SUM
SUM
CS1
sum
eq
.
eq
eq
equation the following
that is larger than
=
CS1
0
.
or R
CS2
. The next
09/09/08
CS1
.

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