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LT1787 Datasheet(PDF) 7 Page - Analog Devices

Part # LT1787
Description  36V Low Cost High Side Current Sense in a SOT-23
PDF  14 Pages
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Manufacturer  AD [Analog Devices]
Direct Link  http://www.analog.com
Logo AD - Analog Devices

LT1787 Datasheet(HTML) 7 Page - Analog Devices

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LT6106
7
Rev. C
For more information www.analog.com
APPLICATIONS INFORMATION
Introduction
TheLT6106highsidecurrentsenseamplifier(Figure1)pro-
videsaccuratemonitoringofcurrentthroughauser-selected
sense resistor. The sense voltage is amplified by a user-
selected gain and level shifted from the positive power sup-
ply to a ground-referred output. The output signal is analog
and may be used as is, or processed with an output filter.
Theory of Operation
An internal sense amplifier loop forces –IN to have the
same potential as +IN. Connecting an external resistor,
RIN, between –IN and V+ forces a potential across RIN
that is the same as the sense voltage across RSENSE. A
corresponding current, VSENSE/RIN, will flow through RIN.
The high impedance inputs of the sense amplifier will not
conduct this current, so it will flow through an internal
PNP to the output pin as IOUT.
The output current can be transformed into a voltage by
adding a resistor from OUT to V–. The output voltage is
then VO = V– + IOUT • ROUT.
Table 1. Useful Gain Configurations
GAIN
RIN
ROUT
VSENSE at VOUT = 5V
IOUT at VOUT = 5V
20
499Ω
10k
250mV
500µA
50
200Ω
10k
100mV
500µA
100
100Ω
10k
50mV
500µA
GAIN
RIN
ROUT VSENSE at VOUT = 2.5V IOUT at VOUT = 2.5V
20
249Ω
5k
125mV
500µA
50
100Ω
5k
50mV
500µA
100
50Ω
5k
25mV
500µA
Selection of External Current Sense Resistor
The external sense resistor, RSENSE,hasasignificanteffect
on the function of a current sensing system and must be
chosen with care.
First, the power dissipation in the resistor should be
considered. The system load current will cause both heat
and voltage loss in RSENSE. As a result, the sense resis-
tor should be as small as possible while still providing
the input dynamic range required by the measurement.
Note that input dynamic range is the difference between
the maximum input signal and the minimum accurately
measuredsignal,andislimitedprimarilybyinputDCoffset
of the internal amplifier of the LT6106. In addition, RSENSE
must be small enough that VSENSE does not exceed the
maximum input voltage specified by the LT6106, even
under peak load conditions. As an example, an application
may require that the maximum sense voltage be 100mV.
If this application is expected to draw 2A at peak load,
RSENSE should be no more than 50mΩ.
Once the maximum RSENSE value is determined, the mini-
mum sense resistor value will be set by the resolution or
dynamic range required. The minimum signal that can be
accurately represented by this sense amplifier is limited by
the input offset. As an example, the LT6106 has a typical
input offset of 150µV. If the minimum current is 20mA, a
sense resistor of 7.5mΩ will set VSENSE to 150µV. This is
the same value as the input offset. A larger sense resis-
tor will reduce the error due to offset by increasing the
sense voltage for a given load current. Choosing a 50mΩ
RSENSE will maximize the dynamic range and provide a
system that has 100mV across the sense resistor at peak
load (2A), while input offset causes an error equivalent to
only 3mA of load current. Peak dissipation is 200mW. If a
5mΩsenseresistorisemployed,thentheeffectivecurrent
error is 30mA, while the peak sense voltage is reduced to
10mV at 2A, dissipating only 20mW.
The low offset and corresponding large dynamic range of
the LT6106 make it more flexible than other solutions in
this respect. The 150µV typical offset gives 60dB of dy-
namic range for a sense voltage that is limited to 150mV
maximum, and over 70dB of dynamic range if the rated
input maximum of 0.5V is allowed.
Sense Resistor Connection
Kelvin connection of the –IN and +IN inputs to the sense
resistor should be used in all but the lowest power ap-
plications. Solder connections and PC board interconnec-
tions that carry high current can cause significant error
in measurement due to their relatively large resistances.
One 10mm × 10mm square trace of one-ounce copper
is approximately 0.5mΩ. A 1mV error can be caused by
as little as 2A flowing through this small interconnect.
This will cause a 1% error in a 100mV signal. A 10A load
current in the same interconnect will cause a 5% error
for the same 100mV signal. By isolating the sense traces
from the high current paths, this error can be reduced



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