LTC6102
LTC6102-1/LTC6102HV
13
6102fe
For more information www.linear.com/LTC6102
Dynamic Range vs Maximum
Power Dissipation in R
SENSE
applicaTions inForMaTion
a significant load on the power supply and create thermal
design headaches. In addition, heating in the sense resistor
can reduce its accuracy and reliability.
In contrast, the large dynamic range of the LTC6102 allows
the use of a much smaller sense resistor. The LTC6102
allows the minimum sense voltage to be reduced to less
than 10µV. The peak sense voltage would then be 10mV,
dissipating only 1W at 100A in a 100µΩ sense resistor!
With a specialized sense resistor, the same system would
allow peak currents of more than 1000A without exceeding
the input range of the LTC6102 or damaging the shunt.
Figure 2. Kelvin Input Connection Preserves Accuracy
with Large Load Current and Large Output Current
LTC6102
R
OUT
V
OUT
6102 F02
R
IN
V
+
LOAD
R
SENSE
R
IN
+
+
V
+
–INF
V
OUT
V
REG
0.1µF
TIE AS CLOSE TO R
IN
AS POSSIBLE
–INS+IN
LOADV
+
V
OUTPUT
R
SENSE
*
R
OUT
LTC6102
R
IN
R
IN
+
C
REG
*VISHAY VCS1625 SERIES
WITH 4 PAD KELVIN CONNECTION
V
high-current paths, this error can be reduced by orders of
magnitude. A sense resistor with integrated Kelvin sense
terminals will give the best results. Figure 2 illustrates the
recommended method. Note that the LTC6102 has a Kelvin
input structure such that current flows into –INF. The –INS
and –INF pins should be tied as close as possible to R
IN
.
This reduces the parasitic series resistance so that R
IN
may be as low as 1Ω, allowing high gain settings to be
used with very little gain error.
Sense Resistor Connection
Kelvin connection of +IN and –INS to the sense resistor
should be used in all but the lowest power applications.
Solder connections and PC board interconnections that
carry high current can cause significant error in measure
-
ment due to their relatively large resistances. One 10mm
× 10mm square trace of one-ounce copper is approxi-
mately 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. An additional error is caused by the
change in copper resistance over temperature, which is in
excess of 0.4%/°C. By isolating the sense traces from the
Selection of External Input Resistor, R
IN
The external input resistor, R
IN
, controls the transconduc-
tance of the current sense circuit, I
OUT
= V
SENSE
/R
IN
. For
example, if R
IN
= 100, then I
OUT
= V
SENSE
/100 or I
OUT
=
1mA for V
SENSE
= 100mV.
R
IN
should be chosen to provide the required resolution
while limiting the output current. At low supply voltage,
I
OUT
may be as much as 1mA. By setting R
IN
such that
MAXIMUM POWER DISSIPATION (W)
DYNAMIC RANGE (dB)
110
100
90
80
70
60
50
40
30
20
6102 AI01
0.001 0.01 0.1 1 10 100
MAX I
SENSE
= 1A
MAX I
SENSE
= 10A
MAX I
SENSE
= 100A
DYNAMIC RANGE RELATIVE
TO 10µV, MINIMUM V
SENSE
R
SENSE
= 10mΩR
SENSE
= 100mΩ
100dB: MAX
V
SENSE
= 1V
40dB: MAX
V
SENSE
= 1mV
R
SENSE
= 10µΩ
R
SENSE
= 100µΩ
R
SENSE
= 1Ω
R
SENSE
= 1mΩ
LTC6102
LTC6102-1/LTC6102HV
14
6102fe
For more information www.linear.com/LTC6102
the largest expected sense voltage gives I
OUT
= 1mA, then
the maximum output dynamic range is available. Output
dynamic range is limited by both the maximum allowed
output current (Note 1) and the maximum allowed output
voltage, as well as the minimum practical output signal. If
less dynamic range is required, then R
IN
can be increased
accordingly, reducing the output current and power dis-
sipation. If small sense currents must be resolved ac-
curately in a system that has very wide dynamic range, a
smaller R
IN
may be used if the max current is limited in
another way, such as with a Schottky diode across R
SENSE
(Figure 3). This will reduce the high current measurement
accuracy by limiting the result, while increasing the low
current measurement resolution. This approach can be
helpful in cases where occasional large burst currents
may be ignored.
applicaTions inForMaTion
the LTC6102, and into R
OUT
via the OUT pin. In order to
minimize gain error, –INS should be routed in a separate
path from –INF to a point as close to R
IN
as possible. In
addition, the higher potential terminal of R
IN
should be
connected directly to the positive terminal of R
SENSE
(or
any input voltage source). For the highest accuracy, R
IN
should be a four-terminal resistor if it is less than 10Ω.
Selection of External Output Resistor, R
OUT
The output resistor, R
OUT
, determines how the output cur-
rent is converted to voltage. V
OUT
is simply I
OUT
• R
OUT
.
In choosing an output resistor, the max output voltage
must first be considered. If the circuit that is driven by the
output does not have a limited input voltage, then R
OUT
must be chosen such that the max output voltage does
not exceed the LTC6102 max output voltage rating. If the
following circuit is a buffer or ADC with limited input range,
then R
OUT
must be chosen so that I
OUT(MAX)
R
OUT
is less
than the allowed maximum input range of this circuit.
In addition, the output impedance is determined by R
OUT
. If
the circuit to be driven has high enough input impedance,
then almost any output impedance will be acceptable.
However, if the driven circuit has relatively low input imped
-
ance, or draws spikes of current, such as an ADC might
do, then a lower R
OUT
value may be required in order to
preserve the accuracy of the output. As an example, if the
input impedance of the driven circuit is 100 times R
OUT
,
then the accuracy of V
OUT
will be reduced by 1% since:
VI
RR
RR
OUT OUT
OUT IN DRIVEN
OUT IN DRIVEN
=
+
=
()
()
IIR
IR
OUT OUT OUT OUT
•• .•
100
101
099=
Error Sources
The current sense system uses an amplifier and resistors
to apply gain and level shift the result. The output is then
dependent on the characteristics of the amplifier, such as
gain and input offset, as well as resistor matching.
Figure 3. Shunt Diode Limits Maximum Input Voltage to Allow
Better Low Input Resolution Without Overranging
V
+
LOAD
D
SENSE
6102 F03
R
SENSE
Care should be taken when designing the PC board lay-
out for R
IN
, especially for small R
IN
values. All trace and
interconnect impedances will increase the effective R
IN
value, causing a gain error. It is important to note that the
large temperature drift of copper resistance will cause a
change in gain over temperature if proper care is not taken
to reduce this effect.
To further limit the effect of trace resistance on gain,
maximizing the accuracy of these circuits, the LTC6102 has
been designed with a Kelvin input. The inverting terminal
(–INS) is separate from the feedback path (–INF). During
operation, these two pins must be connected together.
The design of the LTC6102 is such that current into –INS
is input bias current only, which is typically 60pA at 25°C.
Almost all of the current from R
IN
flows into –INF, through
LTC6102
LTC6102-1/LTC6102HV
15
6102fe
For more information www.linear.com/LTC6102
Figure 5. Second Input R Minimizes
Error Due to Input Bias Current
–INF
V
REG
0.1µF
–INS
6102 F05
R
IN
+
=
R
IN
R
SENSE
LTC6102
R
OUT
V
OUT
V
+
LOAD
R
SENSE
+
V
+
V
OUT
+IN
R
IN
R
IN
+
applicaTions inForMaTion
For instance if I
BIAS
is 1nA and R
OUT
is 10k, the output
error is –10µV.
Note that in applications where R
SENSE
≈ R
IN
, I
B
(+) causes
a voltage offset in R
SENSE
that cancels the error due to
I
B
(–) and E
OUT(IBIAS)
≈ 0. In applications where R
SENSE
<
R
IN
, the bias current error can be similarly reduced if an
external resistor R
IN
(+) = (R
IN
– R
SENSE
) is connected as
shown in Figure 5. Under both conditions:
E
OUT(IBIAS)
= ± R
OUT
• I
OS
; I
OS
= I
B
(+) – I
B
(–)
Adding R
IN
+
as described will maximize the dynamic
range of the circuit. For less sensitive designs, R
IN
+
is
not necessary.
Ideally, the circuit output is:
VV
R
R
VRI
OUT SENSE
OUT
IN
SENSESENSE SENSE
==
•;
In this case, the only error is due to resistor mismatch,
which provides an error in gain only.
Output Error, E
OUT
, Due to the Amplifier DC Offset
Voltage, V
OS
E
OUT(VOS)
= V
OS
• (R
OUT
/R
IN
)
The DC offset voltage of the amplifier adds directly to
the value of the sense voltage, V
SENSE
. This error is very
small (3µV typ) and may be ignored for reasonable values
of R
IN
. See Figure 4. For very high dynamic range, this
offset can be calibrated in the system due to its extremely
low drift.
INPUT VOLTAGE (V)
OUTPUT ERROR (%)
100
10
1
0.1
0.01
0.001
0.0001
6102 F04
0.00001 0.0001 0.001 0.01 0.1 1
FOR A 500µΩ SHUNT
V
IN
= 100mV, I
SHUNT
= 200A
ERROR DUE TO V
OS
IS 6mA
V
IN
= 10µV
Figure 4. LTC6102 Output Error Due to Typical Input Offset
vs Input Voltage
Output Error, E
OUT
, Due to the Bias Currents,
I
B
(+) and I
B
(–)
The input bias current of the LTC6102 is vanishingly small.
However, for very high resolution, or at high temperatures
where I
B
increases due to leakage, the current may be
significant.
The bias current I
B
(+) flows into the positive input of the
internal op amp. I
B
(–) flows into the negative input.
E
OUT(IBIAS)
= R
OUT
((I
B
(+) • (R
SENSE
/R
IN
) – I
B
(–))
Since I
B
(+) ≈ I
B
(–) = I
BIAS
, if R
SENSE
<< R
IN
then,
E
OUT(IBIAS)
≈ –R
OUT
• I
BIAS
Clock Feedthrough, Input Bias Current
The LTC6102 uses auto-zeroing circuitry to achieve an
almost zero DC offset over temperature, sense voltage,
and power supply voltage. The frequency of the clock
used for auto-zeroing is typically 10kHz. The term clock
feedthrough is broadly used to indicate visibility of this
clock frequency in the op amp output spectrum. There are
typically two types of clock feedthrough in auto zeroed
amps like the LTC6102.
The first form of clock feedthrough is caused by the
settling of the internal sampling capacitor and is input
referred; that is, it is multiplied by the internal loop gain

LTC6102HMS8-1#TRPBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Current Sense Amplifiers Zero-Drift Current Sense Amplifier with Shutdown
Lifecycle:
New from this manufacturer.
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