AD8532AR Analog Devices Inc, AD8532AR Datasheet - Page 12
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AD8532AR
Manufacturer Part Number
AD8532AR
Description
Amplifier IC
Manufacturer
Analog Devices Inc
Datasheet
1.AD8531ARTZ-REEL7.pdf
(20 pages)
Specifications of AD8532AR
No. Of Amplifiers
2
Bandwidth
3MHz
Slew Rate
5V/µs
No. Of Pins
8
Peak Reflow Compatible (260 C)
No
Leaded Process Compatible
No
Mounting Type
Surface Mount
Package / Case
8-SOIC
Rohs Status
RoHS non-compliant
Amplifier Type
General Purpose
Number Of Circuits
2
Output Type
Rail-to-Rail
Gain Bandwidth Product
3MHz
Current - Input Bias
5pA
Voltage - Input Offset
25000µV
Current - Supply
750µA
Current - Output / Channel
250mA
Voltage - Supply, Single/dual (±)
2.7 V ~ 6 V, ±1.35 V ~ 3 V
Operating Temperature
-40°C ~ 85°C
Lead Free Status / RoHS Status
Contains lead / RoHS non-compliant
-3db Bandwidth
-
Lead Free Status / RoHS Status
Contains lead / RoHS non-compliant
Available stocks
Company
Part Number
Manufacturer
Quantity
Price
Company:
Part Number:
AD8532AR
Manufacturer:
AD
Quantity:
5 510
Part Number:
AD8532AR
Manufacturer:
ADI/亚德诺
Quantity:
20 000
Part Number:
AD8532AR-REEL
Manufacturer:
ADI/亚德诺
Quantity:
20 000
Part Number:
AD8532AR-REEL7
Manufacturer:
ADI/亚德诺
Quantity:
20 000
Part Number:
AD8532AR-TEEL
Manufacturer:
ADI/亚德诺
Quantity:
20 000
Part Number:
AD8532ARM
Manufacturer:
ADI/亚德诺
Quantity:
20 000
Company:
Part Number:
AD8532ARM-REEL
Manufacturer:
AD
Quantity:
5 510
AD8531/AD8532/AD8534
The thermal resistance curves were determined using the
AD8531/AD8532/AD8534 thermal resistance data for each
package and a maximum junction temperature of 150°C. The
following formula can be used to calculate the internal junction
temperature of the AD8531/AD8532/AD8534 for any application:
where:
T
P
θ
T
To calculate the power dissipated by the AD8531/AD8532/
AD8534, the following equation can be used:
where:
I
V
V
The quantity within the parentheses is the maximum voltage
developed across either output transistor. As an additional
design aid in calculating available load current from the
AD8531/AD8532/AD8534, Figure 5 illustrates the output
voltage of the AD8531/AD8532/AD8534 as a function of
load resistance.
POWER CALCULATIONS FOR VARYING OR
UNKNOWN LOADS
Often, calculating power dissipated by an integrated circuit to
determine if the device is being operated in a safe range is not
as simple as it may seem. In many cases, power cannot be directly
measured, which may be the result of irregular output waveforms
or varying loads; indirect methods of measuring power are
required.
There are two methods to calculate power dissipated by an
integrated circuit. The first can be done by measuring the
package temperature and the board temperature, and the
other is to directly measure the supply current of the circuit.
CALCULATING POWER BY MEASURING AMBIENT
AND CASE TEMPERATURE
Given the two equations for calculating junction temperature
where:
T
T
θ
LOAD
JA
JA
DISS
J
A
J
A
S
OUT
is the junction temperature.
is the junction temperature.
is the supply voltage.
is the package thermal resistance, junction-to-case.
is the ambient temperature of the circuit.
is the ambient temperature.
is the junction to ambient thermal resistance.
T
is the power dissipation.
P
T
is the output load current.
is the output voltage.
J
DISS
J
= P
= T
= I
DISS
A
+ P
LOAD
× θ
DISS
× (V
JA
θ
+ T
JA
S
− V
A
OUT
)
Rev. F | Page 12 of 20
where:
T
θ
The two equations can be solved for P (power)
Once power is determined, it is necessary to go back and calculate
the junction temperature to ensure that it has not been exceeded.
The temperature measurements should be directly on the package
and on a spot on the board that is near the package but not
touching it. Measuring the package could be difficult. A very
small bimetallic junction glued to the package can be used, or
measurement can be done using an infrared sensing device if
the spot size is small enough.
CALCULATING POWER BY MEASURING SUPPLY
CURRENT
Power can be calculated directly, knowing the supply voltage
and current. However, supply current may have a dc component
with a pulse into a capacitive load, which can make rms current
very difficult to calculate. It can be overcome by lifting the supply
pin and inserting an rms current meter into the circuit. For this
to work, be sure the current is being delivered by the supply pin
being measured. This is usually a good method in a single-supply
system; however, if the system uses dual supplies, both supplies
may need to be monitored.
INPUT OVERVOLTAGE PROTECTION
As with any semiconductor device, whenever the condition
exists for the input to exceed either supply voltage, the input
overvoltage characteristic of the device must be considered.
When an overvoltage occurs, the amplifier can be damaged,
depending on the magnitude of the applied voltage and the
magnitude of the fault current. Although not shown here, when
the input voltage exceeds either supply by more than 0.6 V, pn
junctions internal to the AD8531/AD8532/AD8534 energize,
allowing current to flow from the input to the supplies. As
illustrated in the simplified equivalent input circuit (see Figure 36),
the AD8531/AD8532/AD8534 do not have any internal current
limiting resistors; therefore, fault currents can quickly rise to
damaging levels.
This input current is not inherently damaging to the device, as
long as it is limited to 5 mA or less. For the AD8531/AD8532/
AD8534, once the input voltage exceeds the supply by more than
0.6 V, the input current quickly exceeds 5 mA. If this condition
continues to exist, an external series resistor should be added.
The size of the resistor is calculated by dividing the maximum
overvoltage by 5 mA. For example, if the input voltage could
reach 10 V, the external resistor should be (10 V/5 mA) = 2 kΩ.
This resistance should be placed in series with either or both
inputs if they are exposed to an overvoltage condition.
JA
C
is the case temperature.
and θ
T
T
P
DISS
J
A
= T
+ P
JC
= (T
are given in the data sheet.
C
DISS
+ P
A
θ
− T
JA
DISS
= T
C
θ
)/(θ
JA
C
+ Pθ
JC
− θ
JC
JA
)