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IR3721 Datasheet(PDF) 6 Page - International Rectifier

Part # IR3721
Description  Power Monitor IC with
PDF  16 Pages
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Manufacturer  IRF [International Rectifier]
Direct Link  http://www.irf.com
Logo IRF - International Rectifier

IR3721 Datasheet(HTML) 6 Page - International Rectifier

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IR3721
DATA SHEET
Page 6 of 16
www.irf.com
09/15/08
THERMAL COMPENSATION FOR INDUCTOR DCR CURRENT
SENSING
The positive temperature coefficient of the inductor
DCR can be compensated if RT varies inversely
proportional to the DCR. DCR of a copper coil, as a
function of temperature, is approximated by
)
⋅
)
(
+
(
⋅
)
(
=
)
(
Cu
R
R
TCR
T
T
T
DCR
T
DCR
-
1
Equation 2
TR is some reference temperature, usually 25 °C, and
TCRCu is the resistive temperature coefficient of
copper, usually assumed to be 0.39 %/°C near room
temperature. Note that equation 2 is linearly
increasing with temperature and has an offset of
DCR(TR) at the reference temperature.
If RT incorporates a negative temperature coefficient
thermistor then temperature effects of DCR can be
minimized. Consider a circuit of two resistors and a
thermistor as shown below.
Rs
Rth
Rp
Figure 2 RT Network
If Rth is an NTC thermistor then the value of the
network will decrease as temperature increases.
Unfortunately, most thermistors exhibit far more
variation with temperature than copper wire. One
equation used to model thermistors is
⎟
⎟
⎠
⎞
⎜
⎜
⎝
⎛
⎟⎟
⎠
⎞
⎜⎜
⎝
⎛
⋅
)
(
=
)
(
0
1
1
0
T
T
th
th
e
T
R
T
R
-
β
Equation 3
where Rth(T) is the thermistor resistance at some
temperature T, Rth(T0) is the thermistor resistance at
the reference temperature T0, and β is the material
constant provided by the thermistor manufacturer.
Kelvin degrees are used in the exponential term of
equation 3. If RS is large and RP is small, the
curvature of the equivalent network resistance can be
reduced from the curvature of the thermistor alone.
Although the exponential equation 3 can never
compensate linear equation 2 at all temperatures, a
spreadsheet can be constructed to minimize error
over the temperature interval of interest. The
equivalent resistance RT of the network shown as a
function of temperature is
)
(
+
+
=
)
(
T
R
R
R
T
R
th
p
s
T
1
1
1
Equation 4
using Rth(T) from equation 3.
Equation 2 may be rewritten as a new function of
temperature using equations 2 and 4 as follows:
()
)
(
+
⋅
)
(
=
)
(
Τ
T
DCR
R
R
T
R
V
T
I
2
CS
1
CS
T
R
FS
Equation 5
With Rs and Rp as additional free variables, use a
spreadsheet to solve equation 5 for the desired full
scale current while minimizing the IFS(T) variation
over temperature.



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