LT6108-1/LT6108-2
13
610812fa
APPLICATIONS INFORMATION
The low offset and corresponding large dynamic range of
the LT6108 make it more flexible than other solutions in this
respect. The 125µV maximum offset gives 72dB of dynamic
range for a sense voltage that is limited to 500mV max.
Sense Resistor Connection
Kelvin connection of the SENSEHI and SENSELO inputs
to the sense resistor should be used in all but the lowest
power applications. Solder connections and PC board
interconnections that carry high currents can cause sig-
nificant error in measurement due to their relatively large
resistances. One 10mm × 10mm square trace of 1oz 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 for a full-scale V
SENSE
of 100mV.
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 by orders of magnitude. A sense resistor with
integrated Kelvin sense terminals will give the best results.
Figure 3 illustrates the recommended method for connect-
ing the SENSEHI and SENSELO pins to the sense resistor.
Selection of External Input Gain Resistor, R
IN
R
IN
should be chosen to allow the required speed and
resolution while limiting the output current to 1mA. The
maximum value for R
IN
is 1k to maintain good loop sta-
bility. For a given V
SENSE
, larger values of R
IN
will lower
power dissipation in the LT6108 due to the reduction
in I
OUT
while smaller values of R
IN
will result in faster
response time due to the increase in I
OUT
. If low sense
currents must be resolved accurately in a system that has
a very wide dynamic range, a smaller R
IN
may be used
if the maximum I
OUTA
current is limited in another way,
such as with a Schottky diode across R
SENSE
(Figure 4).
This will reduce the high current measurement accuracy
by limiting the result, while increasing the low current
measurement resolution.
Figure 3. LT6108-1 Typical Connection
Figure 4. Shunt Diode Limits Maximum Input Voltage to Allow
Better Low Input Resolution Without Overranging
OUTA
I
OUTA
+
V
+
C1
SENSEHI
INC
6
7
8
5
610812 F03
V
+
V
+
V
LT6108-1
SENSELO
EN/RST
OUTC
1
2
3
4
V
RESET
R
C
V
PULLUP
LOAD
V
SUPPLY
V
SENSE
R
SENSE
OVERCURRENT
FLAG
R
IN
+
*R
OUT
= R1 + R2
V
I
SENSE
=
V
SENSE
R
SENSE
R1*
R2* C
L
V
OUT
400mV
REFERENCE
C
LC
+
D
SENSE
R
SENSE
V
+
LOAD
610812 F04
LT6108-1/LT6108-2
14
610812fa
APPLICATIONS INFORMATION
This approach can be helpful in cases where occasional
bursts of high currents can be ignored.
Care should be taken when designing the board layout for
R
IN
, especially for small R
IN
values. All trace and inter-
connect resistances will increase the effective R
IN
value,
causing a gain error.
The power dissipated in the sense resistor can create a
thermal gradient across a printed circuit board and con-
sequently a gain error if R
IN
and R
OUT
are placed such
that they operate at different temperatures. If significant
power is being dissipated in the sense resistor then care
should be taken to place R
IN
and R
OUT
such that the gain
error due to the thermal gradient is minimized.
Selection of External Output Gain Resistor, R
OUT
The output resistor, R
OUT
, determines how the output cur-
rent is converted to voltage. V
OUT
is simply I
OUTA
R
OUT
.
Typically, R
OUT
is a combination of resistors configured
as a resistor divider which has a voltage tap going to the
comparator input to set the comparator threshold.
In choosing an output resistor, the maximum output volt-
age must first be considered. If the subsequent circuit is a
buffer or ADC with limited input range, then R
OUT
must be
chosen so that I
OUTA(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 another circuit is being driven, then the input impedance
of that circuit must be considered. If the subsequent circuit
has high enough input impedance, then almost any use-
ful output impedance will be acceptable. However, if the
subsequent circuit has relatively low input impedance, or
draws spikes of current such as an ADC load, then a lower
output impedance may be required to preserve the accuracy
of the output. More information can be found in the Output
Filtering section. As an example, if the input impedance of
the driven circuit, R
IN(DRIVEN)
, is 100 times R
OUT
, then the
accuracy of V
OUT
will be reduced by 1% since:
V
OUT
= I
OUTA
R
OUT
R
IN(DRIVEN)
R
OUT
+R
IN(DRIVEN)
= I
OUTA
R
OUT
100
101
= 0.99 I
OUTA
R
OUT
Amplifier Error Sources
The current sense system uses an amplifier and resistors
to apply gain and level-shift the result. Consequently, the
output is dependent on the characteristics of the amplifier,
such as gain error and input offset, as well as the matching
of the external resistors.
Ideally, the circuit output is:
V
OUT
= V
SENSE
R
OUT
R
IN
; V
SENSE
= R
SENSE
I
SENSE
In this case, the only error is due to external resistor
mismatch, which provides an error in gain only. However,
offset voltage, input bias current and finite gain in the
amplifier can cause additional errors:
Output Voltage Error, V
OUT(VOS)
, Due to the Amplifier
DC Offset Voltage, V
OS
V
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
. As V
SENSE
is increased,
accuracy improves. This is the dominant error of the system
and it limits the available dynamic range.
Output Voltage Error, V
OUT(IBIAS)
, Due to the Bias
Currents I
B
+
and I
B
The amplifier bias current I
B
+
flows into the SENSELO pin
while I
B
flows into the SENSEHI pin. The error due to I
B
is the following:
V
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,
V
OUT(IBIAS)
= –R
OUT
(I
BIAS
)
It is useful to refer the error to the input:
V
VIN(IBIAS)
= –R
IN
(I
BIAS
)
For instance, if I
BIAS
is 100nA and R
IN
is 1k, the input re-
ferred error is 100µV. This error becomes less significant
as the value of R
IN
decreases. The bias current error can
LT6108-1/LT6108-2
15
610812fa
APPLICATIONS INFORMATION
Output Current Limitations Due to Power Dissipation
The LT6108 can deliver a continuous current of 1mA to the
OUTA pin. This current flows through R
IN
and enters the
current sense amplifier via the SENSEHI pin. The power
dissipated in the LT6108 due to the output signal is:
P
OUT
= (V
SENSEHI
– V
OUTA
) • I
OUTA
Since V
SENSEHI
≈ V
+
, P
OUTA
≈ (V
+
– V
OUTA
) • I
OUTA
There is also power dissipated due to the quiescent power
supply current:
P
S
= I
S
• V
+
The comparator output current flows into the comparator
output pin and out of the V
pin. The power dissipated in
the LT6108 due to the comparator is often insignificant
and can be calculated as follows:
P
OUTC
= (V
OUTC
– V
) • I
OUTC
The total power dissipated is the sum of these
dissipations:
P
TOTAL
= P
OUTA
+ P
OUTC
+ P
S
At maximum supply and maximum output currents, the
total power dissipation can exceed 150mW. This will cause
significant heating of the LT6108 die. In order to prevent
damage to the LT6108, the maximum expected dissipa-
tion in each application should be calculated. This number
can be multiplied by the θ
JA
value, 163°C/W for the MS8
package or 64°C/W for the DFN, to find the maximum
expected die temperature. Proper heat sinking and thermal
relief should be used to ensure that the die temperature
does not exceed the maximum rating.
Output Filtering
The AC output voltage, V
OUT
, is simply I
OUTA
Z
OUT
. This
makes filtering straightforward. Any circuit may be used
which generates the required Z
OUT
to get the desired filter
response. For example, a capacitor in parallel with R
OUT
will give a lowpass response. This will reduce noise at the
output, and may also be useful as a charge reservoir to
keep the output steady while driving a switching circuit
be reduced if an external resistor, R
IN
+
, is connected as
shown in Figure 5, the error is then reduced to:
V
OUT(IBIAS)
= ±R
OUT
• I
OS
; I
OS
= I
B
+
– I
B
Minimizing low current errors will maximize the dynamic
range of the circuit.
Figure 6. Gain Error vs Resistor Tolerance
Figure 5. R
IN
+
Reduces Error Due to I
B
SENSEHI
LT6108
I
SENSE
R
SENSE
V
+
7
V
4
V
+
R
IN
V
BATT
SENSELO
8
1
OUTA 6
610812 F05
R
OUT
V
OUT
R
IN
+
+
RESISTOR TOLERANCE (%)
0.01
0.01
RESULTING GAIN ERROR (%)
0.1
1
10
0.1 1 10
610812 F06
R
IN
= 100Ω
R
IN
= 1k
Output Voltage Error, V
OUT(GAIN ERROR)
, Due to
External Resistors
The LT6108 exhibits a very low gain error. As a result,
the gain error is only significant when low tolerance
resistors are used to set the gain. Note the gain error is
systematically negative. For instance, if 0.1% resistors
are used for R
IN
and R
OUT
then the resulting worst-case
gain error is –0.4% with R
IN
= 100Ω. Figure 6 is a graph
of the maximum gain error which can be expected versus
the external resistor tolerance.

LT6108HDCB-1#TRMPBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Current Sense Amplifiers High Side Current Sense Amplifier with Reference and Comparators
Lifecycle:
New from this manufacturer.
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