ACPL-782T-500E Avago Technologies US Inc., ACPL-782T-500E Datasheet - Page 15

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ACPL-782T-500E

Manufacturer Part Number
ACPL-782T-500E
Description
OPTO AMP ISOLATION AUTO 8-DIP GW
Manufacturer
Avago Technologies US Inc.
Series
R²Coupler™r
Datasheet

Specifications of ACPL-782T-500E

Amplifier Type
Isolation
Number Of Circuits
1
Output Type
Differential
-3db Bandwidth
100kHz
Voltage - Input Offset
300µV
Current - Supply
10.86mA
Current - Output / Channel
18.6mA
Voltage - Supply, Single/dual (±)
4.5 V ~ 5.5 V
Operating Temperature
-40°C ~ 125°C
Mounting Type
Surface Mount
Package / Case
8-SMD Gull Wing
No. Of Amplifiers
1
Isolation Voltage
891V
Gain Non-linearity Max
2%
Slew Rate
1500V/µs
Supply Voltage Range
4.5V To 5.5V
Input Offset Voltage
300µV
Bandwidth
100kHz
Lead Free Status / RoHS Status
Lead free / RoHS Compliant
Gain Bandwidth Product
-
Current - Input Bias
-
Lead Free Status / Rohs Status
Compliant

Available stocks

Company
Part Number
Manufacturer
Quantity
Price
Part Number:
ACPL-782T-500E
Manufacturer:
AVAGO/安华高
Quantity:
20 000
Company:
Part Number:
ACPL-782T-500E
Quantity:
105
Current Sensing Resistors
The current sensing resistor should have low resistance (to
minimize power dissipation), low inductance (to minimize
di/dt induced voltage spikes which could adversely
affect operation), and reasonable tolerance (to maintain
overall circuit accuracy). Choosing a particular value for
the resistor is usually a compromise between minimiz-
ing power dissipation and maximizing accuracy. Smaller
sense resistance decreases power dissipation, while larger
sense resistance can improve circuit accuracy by utilizing
the full input range of the ACPL -782T.
The first step in selecting a sense resistor is determining
how much current the resistor will be sensing. The graph in
Figure 20 shows the RMS current in each phase of a three-
phase induction motor as a function of average motor
output power (in horsepower, hp) and motor drive supply
voltage. The maximum value of the sense resistor is deter-
mined by the current being measured and the maximum
recommended input voltage of the isolation amplifier. The
maximum sense resistance can be calculated by taking
the maximum recommended input voltage and dividing
by the peak current that the sense resistor should see
during normal operation. For example, if a motor will have
a maximum RMS current of 10 A and can experience up
to 50% overloads during normal operation, then the peak
current is 21.1 A (=10 x 1.414 x 1.5). Assuming a maximum
input voltage of 200 mV, the maximum value of sense re-
sistance in this case would be about 10 m:.
The maximum average power dissipation in the sense
resistor can also be easily calculated by multiplying the
sense resistance times the square of the maximum RMS
current, which is about 1 W in the previous example. If the
power dissipation in the sense resistor is too high, the re-
sistance can be decreased below the maximum value to
decrease power dissipation. The minimum value of the
sense resistor is limited by precision and accuracy require-
Figure 20. Motor Output Horsepower vs. Motor Phase Current and Supply
Voltage.
15
40
35
30
25
20
15
10
5
0
0
5
440 V
380 V
220 V
120 V
MOTOR PHASE CURRENT - A (rms)
10
15
20
25
30
35
ments of the design. As the resistance value is reduced,
the output voltage across the resistor is also reduced,
which means that the offset and noise, which are fixed,
become a larger percentage of the signal amplitude. The
selected value of the sense resistor will fall somewhere
between the minimum and maximum values, depending
on the particular requirements of a specific design.
When sensing currents large enough to cause significant
heating of the sense resistor, the temperature coefficient
(tempco) of the resistor can introduce nonlinearity due to
the signal dependent temperature rise of the resistor. The
effect increases as the resistor-to-ambient thermal resis-
tance increases. This effect can be minimized by reducing
the thermal resistance of the current sensing resistor or
by using a resistor with a lower tempco. Lowering the
thermal resistance can be accomplished by reposition-
ing the current sensing resistor on the PC board, by using
larger PC board traces to carry away more heat, or by
using a heat sink.
For a two-terminal current sensing resistor, as the value of
resistance decreases, the resistance of the leads become a
significant percentage of the total resistance. This has two
primary effects on resistor accuracy. First, the effective
resistance of the sense resistor can become dependent
on factors such as how long the leads are, how they are
bent, how far they are inserted into the board, and how far
solder wicks up the leads during assembly (these issues
will be discussed in more detail shortly). Second, the leads
are typically made from a material, such as copper, which
has a much higher tempco than the material from which
the resistive element itself is made, resulting in a higher
tempco overall.
Both of these effects are eliminated when a four-terminal
current sensing resistor is used. A four- terminal resistor
has two additional terminals that are Kelvin-connected
directly across the resistive element itself; these two
terminals are used to monitor the voltage across the
resistive element while the other two terminals are used
to carry the load current. Because of the Kelvin connec-
tion, any voltage drops across the leads carrying the load
current should have no impact on the measured voltage.
When laying out a PC board for the current sensing resistors,
a couple of points should be kept in mind. The Kelvin con-
nections to the resistor should be brought together under
the body of the resistor and then run very close to each
other to the input of the ACPL-782T; this minimizes the
loop area of the connection and reduces the possibility of
stray magnetic fields from interfering with the measured
signal. If the sense resistor is not located on the same PC
board as the ACPL-782T circuit, a tightly twisted pair of
wires can accomplish the same thing.

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