NSC LM12CLK Datasheet

LM12CL 80W Operational Amplifier
General Description
The LM12 is a power op amp capable of driving±25V at
±
10Awhile operating from±30V supplies. The monolithic IC
0.01%distortion. Power bandwidth is 60 kHz. Further, a peak dissipation capability of 800W allows it to handle reac­tive loads such as transducers, actuators or small motors without derating. Important features include:
input protection
controlled turn on
thermal limiting
overvoltage shutdown
output-current limiting
dynamic safe-area protection
±
The IC delivers yet is completely protected against overloads, including shorts to the supplies. The dynamic safe-area protection is provided by instantaneous peak-temperature limiting within the power transistor array.
The turn-on characteristics are controlled by keeping the output open-circuited until the total supply voltage reaches 14V.The output is also opened as the case temperature ex-
10A output current at any output voltage
May 1999
ceeds 150˚C or as the supply voltage approaches the BV
of the output transistors. The IC withstands overvolt-
CEO
ages to 80V. This monolithic op amp is compensated for unity-gain feed-
back, with a small-signal bandwidth of 700 kHz. Slew rate is 9V/µs, even as a follower. Distortion and capacitive-load sta­bility rival that of the best designs using complementary out­put transistors. Further, the IC withstands large differential input voltages and is well behaved should the common-mode range be exceeded.
The LM12 establishes that monolithic ICs can deliver consid­erable output power without resorting to complex switching schemes. Devices can be paralleled or bridged for even greater output capability. Applications include operational power supplies, high-voltage regulators, high-quality audio amplifiers, tape-head positioners, x-y plotters or other servo-control systems.
The LM12 is supplied in a four-lead, TO-3 package with V− on the case. A gold-eutectic die-attach to a molybdenum in­terface is used to avoid thermal fatigue problems. The LM12 is specified for either military or commercial temperature range.
LM12CL 80W Operational Amplifier
Connection Diagram Typical Application
4-pin glass epoxy TO-3 socket is available from AUGAT INC. Part number 8112-AG7
Bottom View
Order Number LM12CLK
See NS Package Number K04A
© 1999 National Semiconductor Corporation DS008704 www.national.com
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*Low distortion (0.01%) audio amplifier
*
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Absolute Maximum Ratings (Note 1)
If Military/Aerospace specified devices are required, please contact the National Semiconductor Sales Office/
Storage Temperature Range −65˚C to 150˚C Lead Temperature
(Soldering, 10 seconds) 300˚C
Distributors for availability and specifications.
Total Supply Voltage (Note 1) 80V Input Voltage (Note 2) Output Current Internally Limited
Operating Ratings
Total Supply Voltage 15V to 60V Case Temperature (Note 4) 0˚C to 70˚C
Junction Temperature (Note 3)
Electrical Characteristics (Note 4)
Parameter Conditions Typ
25˚C
Input Offset Voltage
±
10V VS≤±0.5 V Input Bias Current V− + 4V V Input Offset Current V− +4V V Common Mode V− +4V V
MAX,VCM
V+ −2V 0.15 0.7/1.0 µA (max)
CM
V+ −2V 0.03 0.2/0.3 µA (max)
CM
V+ −2V 86 70/65 dB (min)
CM
=
0 2 15/20 mV (max)
Rejection Power Supply V+=0.5 V Rejection −6V V− −0.5 V
V−=−0.5 V
6V V+ 0.5 V Output Saturation t Threshold V
=
ON
IN
=
I
OUT
, 90 70/65 dB (min)
MAX
MAX
, 110 75/70 dB (min)
MAX
MAX
1 ms,
=
5(10 ) mV,
1A 1.8 2.2/2.5 V (max) 8A 4 5/7 V (max) 10A 5 V (max)
Large Signal Voltage t Gain V
Thermal Gradient P
=
2 ms,
ON
=
SAT
=
V
SAT
=
DISS
2V, I 8V, R
50W, t
=
0 100 30/20 V/mV (min)
OUT
=
4 50 15/10 V/mV (min)
L
=
65 ms 30 100 µV/W (max)
ON
Feedback Output-Current Limit t
ON
t
ON
=
10 ms, V
=
100 ms, V
=
10V 13 16 A (max)
DISS
=
58V 1.5 0.9/0.6 A (min)
DISS
1.5 1.7 A (max) Power Dissipation t Rating V
ON
DISS
=
100 ms, V =
DC Thermal Resistance (Note 5) V
=
V
DISS
58V 80 52/35 W (min)
DISS
58V 2.7 4.5 ˚C/W (max)
=
20V 100 80/55 W (min)
DISS
=
20V 2.3 2.9 ˚C/W (max)
AC Thermal Resistance (Note 5) 1.6 2.1 ˚C/W (max) Supply Current V
Note 1: Absolute maximum ratings indicate limits beyondwhichdamagetothedevicemay occur. The maximum voltage forwhichtheLM12isguaranteedto operate is given in the operating ratings and in Note 4. With inductive loads or output shorts, other restrictions described in applications section apply.
Note 2: Neither input should exceed the supply voltage by more than 50 volts nor should the voltage between one input and any other terminal exceed 60 volts. Note 3: Operating junction temperature is internally limited near 225˚C within the power transistor and 160˚C for the control circuitry. Note 4: The supply voltage is
internal power dissipation is P face type refers to limits or special conditions over full temperature range. With no heat sink, the package will heat at a rate of 35˚C/sec per 100W of internal dissipation.
Note 5: This thermal resistance is based upon a peak temperature of 200˚C in the center of the power transistor and a case temperature of 25˚C measured at the center of the package bottom. The maximum junction temperature of the control circuitry can be estimated based upon a dc thermal resistance of 0.9˚C/W or an ac thermal resistance of 0.6˚C/W for any operating voltage.
±
30V (V
. Temperaturerange is 0˚C TC≤ 70˚C where TCis the case temperature. Standard typeface indicates limits at 25˚C while bold-
DISS
=
OUT
=
60V), unless otherwise specified. The voltage across the conducting output transistor (supply to output) is V
MAX
0, I
=
0 60 120/140 mA (max)
OUT
LM12CL Units
Limits
DISS
and
Although the output and supply leads are resistant to electrostatic discharges from handling, the input leads are not. The part should be treated accordingly.
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Output-Transistor Ratings (guaranteed)
Safe Area
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DC Thermal Resistance
Typical Performance Characteristics
Pulse Power Limit
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Output Saturation Voltage
Pulse Power Limit
Large Signal Response
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Pulse Thermal Resistance
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Peak Output Current
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Follower Pulse Response
Large Signal Gain
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Thermal Response
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Total Harmonic Distortion
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Typical Performance Characteristics (Continued)
Frequency Response
Input Bias Current
Supply Current
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Output Impedance
Input Noise Voltage
Supply Current
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Power Supply Rejection
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Common Mode Rejection
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Cross-Supply Current
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Application Information
GENERAL
Twenty five years ago the operational amplifier was a spe­cialized design tool used primarily for analog computation. However, the availability of low cost IC op amps in the late 1960’s prompted their use in rather mundane applications, replacing a few discrete components. Once a few basic prin­ciples are mastered, op amps can be used to give exception­ally good results in a wide range of applications while mini­mizing both cost and design effort.
The availability of a monolithic power op amp now promises to extend these advantages to high-power designs. Some conventional applications are given here to illustrate op amp design principles as they relate to power circuitry. The inevi­table fall in prices, as the economies of volume production
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are realized, will prompt their use in applications that might now seem trivial. Replacing single power transistors with an op amp will become economical because of improved per­formance, simplification of attendant circuitry, vastly im­proved fault protection, greater reliability and the reduction of design time.
Power op amps introduce new factors into the design equa­tion. With current transients above 10A, both the inductance and resistance of wire interconnects become important in a number of ways. Further, power ratings are a crucial factor in determining performance. But the power capability of the IC cannot be realized unless it is properly mounted to an ad­equate heat sink. Thus, thermal design is of major impor­tance with power op amps.
This application summary starts off by identifying the origin of strange problems observed while using the LM12 in a
Application Information (Continued)
wide variety of designs with all sorts of fault conditions.A few simple precautions will eliminate these problems. One
would do well to read the section on supply bypassing, lead inductance, output clamp diodes, ground loops and reactive loading before doing any experimentation. Should there be problems with erratic operation, blow-outs, excessive distortion or oscillation, another look at these sections is in order.
The management and protection circuitry can also affect op­eration. Should the total supply voltage exceed ratings or drop below 15–20V, the op amp shuts off completely. Case temperatures above 150˚C also cause shut down until the temperature drops to 145˚C. This may take several seconds, depending on the thermal system. Activation of the dynamic safe-area protection causes both the main feedback loop to lose control and a reduction in output power, with possible oscillations. In ac applications, the dynamic protection will cause waveform distortion. Since the LM12 is well protected against thermal overloads, the suggestions for determining power dissipation and heat sink requirements are presented last.
SUPPLY BYPASSING
All op amps should have their supply leads bypassed with low-inductance capacitors having short leads and located close to the package terminals to avoid spurious oscillation problems. Power op amps require larger bypass capacitors. The LM12 is stable with good-quality electrolytic bypass ca­pacitors greater than 20 µF. Other considerations may re­quire larger capacitors.
The current in the supply leads is a rectified component of the load current. If adequate bypassing is not provided, this distorted signal can be fed back into internal circuitry. Low distortion at high frequencies requires that the supplies be bypassed with 470 µF or more, at the package terminals.
LEAD INDUCTANCE
With ordinary op amps, lead-inductance problems are usu­ally restricted to supply bypassing. Power op amps are also sensitive to inductance in the output lead, particularly with heavy capacitive loading. Feedback to the input should be taken directly from the output terminal, minimizing common inductance with the load. Sensing to a remote load must be accompanied by a high-frequency feedback path directly from the output terminal. Lead inductance can also cause voltage surges on the supplies. With long leads to the power source, energy stored in the lead inductance when the out­put is shorted can be dumped back into the supply bypass capacitors when the short is removed. The magnitude of this transient is reduced by increasing the size of the bypass ca­pacitor near the IC. With 20 µF local bypass, these voltage surges are important only if the lead length exceeds a couple
>
feet (
1 µH lead inductance). Twisting together the supply
and ground leads minimizes the effect.
GROUND LOOPS
With fast, high-current circuitry, all sorts of problems can arise from improper grounding. In general, difficulties can be avoided by returning all grounds separately to a common point. Sometimes this is impractical. When compromising, special attention should be paid to the ground returns for the supply bypasses, load and input signal. Ground planes also help to provide proper grounding.
Many problems unrelated to system performance can be traced to the grounding of line-operated test equipment used for system checkout. Hidden paths are particularly difficult to sort out when several pieces of test equipment are used but can be minimized by using current probes or the new iso­lated oscilloscope pre-amplifiers. Eliminating any direct ground connection between the signal generator and the os­cilloscope synchronization input solves one common prob­lem.
OUTPUT CLAMP DIODES
When a push-pull amplifier goes into power limit while driv­ing an inductive load, the stored energy in the load induc­tance can drive the output outside the supplies.Although the LM12 has internal clamp diodes that can handle several am­peres for a few milliseconds, extreme conditions can cause destruction of the IC. The internal clamp diodes are imper­fect in that about half the clamp current flows into the supply to which the output is clamped while the other half flows across the supplies. Therefore, the use of external diodes to clamp the output to the power supplies is strongly recom­mended. This is particularly important with higher supply voltages.
Experience has demonstrated that hard-wire shorting the output to the supplies can induce random failures if these ex­ternal clamp diodes are not used and the supply voltages are
±
above
20V. Therefore it is prudent to use outputclamp di­odes even when the load is not particularly inductive. This also applies to experimental setups in that blowouts have been observed when diodes were not used. In packaged equipment, it may be possible to eliminate these diodes, pro­viding that fault conditions can be controlled.
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Heat sinking of the clamp diodes is usually unimportant in that they only clamp current transients. Forward drop with 15A fault transients is of greater concern. Usually, these transients die out rapidly. The clamp to the negative supply can have somewhat reduced effectiveness under worst case conditions should the forward drop exceed 1.0V. Mounting this diode to the power op amp heat sink improves the situ­ation. Although the need has only been demonstrated with some motor loads, including a third diode (D3 above) will eliminate any concern about the clamp diodes. This diode, however, must be capable of dissipating continuous power as determined by the negative supply current of the op amp.
REACTIVE LOADING
The LM12 is normally stable with resistive, inductive or smaller capacitive loads. Larger capacitive loads interact with the open-loop output resistance (about 1) to reduce the phase margin of the feedback loop, ultimately causing oscillation. The critical capacitance depends upon the feed­back applied around the amplifier; a unity-gain follower can handle about 0.01 µF, while more than 1 µF does not cause problems if the loop gain is ten. With loop gains greater than unity, a speedup capacitor across the feedback resistor will
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