NSC LM675T

LM675
Power Operational Amplifier
General Description
The LM675 is a monolithic power operational amplifier featuring wide bandwidth and low input offset voltage, making it
equally suitable for AC and DC applications.
The LM675 is capable of delivering output currents in excess
of 3 amps, operating at supply voltages of up to 60V. The device overload protection consists of both internal current limiting and thermal shutdown. The amplifier is also internally
compensated for gains of 10 or greater.
1 mV typical offset voltage
Short circuit protection
Thermal protection with parole circuit (100% tested)
16V–60V supply range
Wide common mode range
Internal output protection diodes
90 dB ripple rejection
Plastic power package TO-220
Applications
Features
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3A current capability
AVO typically 90 dB
5.5 MHz gain bandwidth product
8 V/µs slew rate
Wide power bandwidth 70 kHz
Connection Diagram
High performance power op amp
Bridge amplifiers
Motor speed controls
Servo amplifiers
Instrument systems
Typical Applications
Non-Inverting Amplifier
TO-220 Power Package (T)
DS006739-1
*The tab is internally connected to pin 3 (−VEE)
Front View
Order Number LM675T
See NS Package T05D
DS006739-2
© 1999 National Semiconductor Corporation
DS006739
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LM675 Power Operational Amplifier
May 1999
Absolute Maximum Ratings (Note 1)
Storage Temperature
Junction Temperature
Power Dissipation (Note 2)
Lead Temperature
(Soldering, 10 seconds)
ESD rating to be determined.
If Military/Aerospace specified devices are required,
please contact the National Semiconductor Sales Office/
Distributors for availability and specifications.
± 30V
Supply Voltage
Input Voltage
Operating Temperature
−VEE to VCC
0˚C to +70˚C
−65˚C to +150˚C
150˚C
30W
260˚C
Electrical Characteristics
VS = ± 25V, TA = 25˚C unless otherwise specified.
Parameter
Typical
Tested Limit
POUT = 0W
VCM = 0V
Conditions
18
50 (max)
mA
1
10 (max)
mV
VCM = 0V
VCM = 0V
0.2
2 (max)
µA
50
500 (max)
nA
RL = ∞ Ω
∆VS = ± 5V
90
70 (min)
dB
90
70 (min)
dB
90
70 (min)
dB
Output Voltage Swing
VIN = ± 20V
RL = 8Ω
± 21
± 18 (min)
Offset Voltage Drift Versus Temperature
RS < 100 kΩ
Supply Current
Input Offset Voltage
Input Bias Current
Input Offset Current
Open Loop Gain
PSRR
CMRR
25
Offset Voltage Drift Versus Output Power
Output Power
Gain Bandwidth Product
Max Slew Rate
25
µV/W
20
5.5
W
MHz
8
± 22
Input Common Mode Range
V
µV/˚C
25
THD = 1%, fO = 1 kHz, RL = 8Ω
fO = 20 kHz, AVCL = 1000
Units
V/µs
± 20 (min)
V
Note 1: Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for which the device is functional, but do not guarantee specific performance limits. Electrical Characteristics state DC and AC electrical specifications under particular test conditions which guarantee specific performance limits. This assumes that the device is within the Operating Ratings. Specifications are not guaranteed for parameters where no limit is
given, however, the typical value is a good indication of device performance.
Note 2: Assumes TA equal to 70˚C. For operation at higher tab temperatures, the LM675 must be derated based on a maximum junction temperature of 150˚C.
Typical Applications
Generating a Split Supply From a Single Supply
DS006739-3
VS = ± 8V → ± 30V
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Typical Performance Characteristics
THD vs Power Output
Input Common Mode
Range vs Supply Voltage
Supply Current vs
Supply Voltage
DS006739-10
DS006739-11
PSRR vs Frequency
Device Dissipation vs
Ambient Temperature†
DS006739-12
Current Limit vs
Output Voltage*
DS006739-13
DS006739-14
†θ INTERFACE = 1˚ C/W
See Application Hints.
IB vs Supply Voltage
DS006739-15
*VS = ± 25V
Output Voltage
Swing vs Supply Voltage
DS006739-16
DS006739-17
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DS006739-5
Schematic Diagram
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tween the output of the amplifier and the supply rails. These
are part of the internal circuitry of the LM675, and needn’t be
added externally when standard reactive loads are driven.
Application Hints
STABILITY
The LM675 is designed to be stable when operated at a
closed-loop gain of 10 or greater, but, as with any other
high-current amplifier, the LM675 can be made to oscillate
under certain conditions. These usually involve printed circuit board layout or output/input coupling.
When designing a printed circuit board layout, it is important
to return the load ground, the output compensation ground,
and the low level (feedback and input) grounds to the circuit
board ground point through separate paths. Otherwise, large
currents flowing along a ground conductor will generate voltages on the conductor which can effectively act as signals at
the input, resulting in high frequency oscillation or excessive
distortion. It is advisable to keep the output compensation
components and the 0.1 µF supply decoupling capacitors as
close as possible to the LM675 to reduce the effects of PCB
trace resistance and inductance. For the same reason, the
ground return paths for these components should be as
short as possible.
Occasionally, current in the output leads (which function as
antennas) can be coupled through the air to the amplifier input, resulting in high-frequency oscillation. This normally
happens when the source impedance is high or the input
leads are long. The problem can be eliminated by placing a
small capacitor (on the order of 50 pF to 500 pF) across the
circuit input.
Most power amplifiers do not drive highly capacitive loads
well, and the LM675 is no exception. If the output of the
LM675 is connected directly to a capacitor with no series resistance, the square wave response will exhibit ringing if the
capacitance is greater than about 0.1 µF. The amplifier can
typically drive load capacitances up to 2 µF or so without oscillating, but this is not recommended. If highly capacitive
loads are expected, a resistor (at least 1Ω) should be placed
in series with the output of the LM675. A method commonly
employed to protect amplifiers from low impedances at high
frequencies is to couple to the load through a 10Ω resistor in
parallel with a 5 µH inductor.
THERMAL PROTECTION
The LM675 has a sophisticated thermal protection scheme
to prevent long-term thermal stress to the device. When the
temperature on the die reaches 170˚C, the LM675 shuts
down. It starts operating again when the die temperature
drops to about 145˚C, but if the temperature again begins to
rise, shutdown will occur at only 150˚C. Therefore, the device is allowed to heat up to a relatively high temperature if
the fault condition is temporary, but a sustained fault will limit
the maximum die temperature to a lower value. This greatly
reduces the stresses imposed on the IC by thermal cycling,
which in turn improves its reliability under sustained fault
conditions. This circuitry is 100% tested without a heat sink.
Since the die temperature is directly dependent upon the
heat sink, the heat sink should be chosen for thermal resistance low enough that thermal shutdown will not be reached
during normal operaton. Using the best heat sink possible
within the cost and space constraints of the system will improve the long-term reliability of any power semiconductor.
POWER DISSIPATION AND HEAT SINKING
The LM675 should always be operated with a heat sink,
even though at idle worst case power dissipation will be only
1.8W (30 mA x 60V) which corresponds to a rise in die temperature of 97˚C above ambient assuming θjA = 54˚C/W for
a TO-220 package. This in itself will not cause the thermal
protection circuitry to shut down the amplifier when operating
at room temperature, but a mere 0.9W of additional power
dissipation will shut the amplifier down since TJ will then increase from 122˚C (97˚C + 25˚C) to 170˚C.
In order to determine the appropriate heat sink for a given
application, the power dissipation of the LM675 in that application must be known. When the load is resistive, the maximum average power that the IC will be required to dissipate
is approximately:
CURRENT LIMIT AND SAFE OPERATING AREA
(SOA) PROTECTION
A power amplifier’s output transistors can be damaged by
excessive applied voltage, current flow, or power dissipation.
The voltage applied to the amplifier is limited by the design of
the external power supply, while the maximum current
passed by the output devices is usually limited by internal
circuitry to some fixed value. Short-term power dissipation is
usually not limited in monolithic operational power amplifiers,
and this can be a problem when driving reactive loads, which
may draw large currents while high voltages appear on the
output transistors. The LM675 not only limits current to
around 4A, but also reduces the value of the limit current
when an output transistor has a high voltage across it.
When driving nonlinear reactive loads such as motors or
loudspeakers with built-in protection relays, there is a possibility that an amplifier output will be connected to a load
whose terminal voltage may attempt to swing beyond the
power supply voltages applied to the amplifier. This can
cause degradation of the output transistors or catastrophic
failure of the whole circuit. The standard protection for this
type of failure mechanism is a pair of diodes connected be-
where VS is the total power supply voltage across the
LM675, RL is the load resistance and PQ is the quiescent
power dissipation of the amplifier. The above equation is
only an approximation which assumes an “ideal” class B output stage and constant power dissipation in all other parts of
the circuit. As an example, if the LM675 is operated on a 50V
power supply with a resistive load of 8Ω, it can develop up to
19W of internal power dissipation. If the die temperature is to
remain below 150˚C for ambient temperatures up to 70˚C,
the total junction-to-ambient thermal resistance must be less
than
Using θJC = 2˚C/W, the sum of the case-to-heat sink interface thermal resistance and the heat-sink-to-ambient thermal resistance must be less than 2.2˚C/W. The
case-to-heat-sink thermal resistance of the TO-220 package
varies with the mounting method used. A metal-to-metal interface will be about 1˚C/W if lubricated, and about 1.2˚C/W
if dry. If a mica insulator is used, the thermal resistance will
be about 1.6˚C/W lubricated and 3.4˚C/W dry. For this ex-
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Application Hints
The thermal requirements can become more difficult when
an amplifier is driving a reactive load. For a given magnitude
of load impedance, a higher degree of reactance will cause
a higher level of power dissipation within the amplifier. As a
general rule, the power dissipation of an amplifier driving a
60˚ reactive load will be roughly that of the same amplifier
driving the resistive part of that load. For example, some reactive loads may at some frequency have an impedance
with a magnitude of 8Ω and a phase angle of 60˚. The real
part of this load will then be 8Ω x cos 60˚ or 4Ω, and the amplifier power dissipation will roughly follow the curve of power
dissipation with a 4Ω load.
(Continued)
ample, we assume a lubricated mica insulator between the
LM675 and the heat sink. The heat sink thermal resistance
must then be less than
4.2˚C/W − 2˚C/W − 1.6˚C/W = 0.6˚C/W.
This is a rather large heat sink and may not be practical in
some applications. If a smaller heat sink is required for reasons of size or cost, there are two alternatives. The maximum ambient operating temperature can be restricted to
50˚C (122˚F), resulting in a 1.6˚C/W heat sink, or the heat
sink can be isolated from the chassis so the mica washer is
not needed. This will change the required heat sink to a
1.2˚C/W unit if the case-to-heat-sink interface is lubricated.
Typical Applications
Non-Inverting Unity Gain Operation
DS006739-6
Inverting Unity Gain Operation
DS006739-7
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Typical Applications
(Continued)
Servo Motor Control
DS006739-8
High Current Source/Sink
DS006739-9
IOUT = VIN x 2.5 amps/volt
i.e. IOUT = 1A when VIN = 400 mV
Trim pot for max ROUT
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LM675 Power Operational Amplifier
Physical Dimensions
inches (millimeters) unless otherwise noted
TO-220 Power Package (T)
Order Number LM675T
NS Package T05D
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