Application Note 2 August 1984 Performance Enhancement Techniques for Three-Terminal Regulators Jim Williams Three terminal regulators provide a simple, effective solution to voltage regulation requirements. In many situations the regulator can be used with no special considerations. Some applications, however, require special techniques to enhance the performance of the device. Probably the most common modification involves extending the output current of regulators. Conceptually, the simplest way to do this is by paralleling devices. In practice, the voltage output tolerance of the regulators can cause problems. Figure 1 shows a way to use two regulators to achieve an output current equal to their sum. This circuit capitalizes on the 1% output tolerance of the specified regulators to achieve a simple paralleled configuration. Both regulators sense from the same divider string and the small value resistors provide ballast to account for the slightly differing output voltages. This added impedance degrades total circuit regulation to about 1%.
Figure 2 shows another way to extend current capability in a regulator. Although this circuit is more complex than Figure 1, it eliminates the ballasting resistor’s effects and has a fast-acting logic-controlled shutdown feature. Additionally, the current limit may be set to any desired value. This circuit extends the 1A capacity of the LT®1005 multifunction regulator to 12A, while retaining the LT1005’s enable feature and auxiliary 5V output. Q1, a booster transistor, is servo-controlled by the LT1005, while Q2 senses the current dependent voltage across the 0.05Ω shunt. When the shunt voltage is large enough, Q2 comes on, biasing Q3 and shutting down the regulator via the LT1005’s enable pin. The shunt’s value can be selected for the desired current limit. The 100°C thermo-switch limits dissipation in Q1 during prolonged short circuits by disabling the LT1005. It should be mounted on Q1’s heat sink. L, LT, LTC, LTM, Linear Technology and the Linear logo are registered trademarks of Linear Technology Corporation. All other trademarks are the property of their respective owners.
0.01Ω VIN ≥ 6.5V
IN
LT1083 ADJ
5V 15A
OUT
UPDATE The LT3080 and LT3083 are better for parallel operation
0.01Ω IN
+
LT1083 ADJ
OUT 121Ω
100μF
+ 200μF AN02 F01
365Ω
NOTE: THIS CIRCUIT WILL NOT WORK WITH LM-TYPE DEVICES
Figure 1
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AN2-1
Application Note 2 Boosted regulator schemes of this type are often poorly dynamically damped. Such improper loop compensation results in large output transients for shifts in the load. In particular, because Q1’s common emitter configuration has voltage gain, transients approaching the input voltage are possible when the load drops out. Here, the 100μF capacitor damps Q1’s tendency to overshoot, while the 20Ω value provides turn-off bias. The 250μF unit maintains Q1’s emitter at DC. Figure 3 shows that this “brute force” compensation works quite well. Normally the regulator sees no load. When Trace A goes high, a 12A load (regulator output current is Trace C) is placed across the output terminals. The regulator output voltage recovers quickly, with minimal aberration.
While the 100μF output capacitor aids stability, it prevents the regulator output from dropping quickly when the enable command is given. Because Q1 cannot sink current, the 100μF unit’s discharge time is load limited. Q4 corrects this problem, even when there is no load. When the enable command is given (Trace A, Figure 4) Q3 comes on, cutting off the LT1005 and forcing Q1 off. Simultaneously, Q4 comes on, pulling down the regulator output (Trace B), and sinks the 100μF capacitor’s discharge current (Trace C). If fast turn-off is not needed, Q4 may be omitted.
250μF
+ 0.05Ω*
8.5 MIN INPUT
Q1 2N4398 (HEAT SINK)
+ 1k
20Ω
0.05Ω
100μF
OUTPUT 5V 12A
Q2 2N2907 IN
OUT LT1005 GND AUXILIARY ENABLE
Q4 2N6387
10k 10k
ENABLE “LO”
10k
Q3 2N2222
1k
100°C N.0. THERMO-SWITCH ON HEAT SINK
1k
*SELECT FOR I LIMIT = 12A
AN02 F02
Figure 2
A = 10V/DIV
A = 10V/DIV B = 2V/DIV
B = 0.5V/DIV AC-COUPLED
C = 5A/DIV
C = 2A/DIV
HORIZONTAL = 10μs/DIV
Figure 3
AN02 F03
HORIZONTAL = 100μs/DIV
AN02 F04
Figure 4
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AN2-2
Application Note 2 Power dissipation control is another area where regulators can be helped by additional circuitry. Increasing heat sink area can be used to offset dissipation problems, but is a wasteful and inefficient approach. Instead, the regulator can be placed within a switched-mode loop that servo-controls the voltage across the regulator. In this arrangement the regulator functions normally while the switched-mode control loop maintains the voltage across it at a minimal value, regardless of line or load changes. Although this approach is not quite as efficient as a classical switching regulator, it offers lower noise and the fast transient response of the linear regulator. Figure 5 details a DC driven version
of the circuit. The LT350A functions in the conventional fashion, supplying a regulated output at 3A capacity. The remaining components form the switched-mode dissipation limiting control. This loop forces the potential across the LT350A to equal the 3.7V value of VZ. When the input of the regulator (Trace A, Figure 6) decays far enough, the LT1018 output (Trace B) switches low, turning on Q1 (Q1 collector is Trace D). This allows current flow (Trace C) from the circuit input into the 4500μF capacitor, raising the regulator’s input voltage. When the regulator input rises far enough, the comparator goes high, Q1 cuts off and the capacitor ceases charging.
2.2k VZ
Q1 2N6667
1MHY
28V INPUT 10k
IN
+
1N4003
4500
LT350A ADJ
LT1004 1.2 VZ
68pF
1M 28V
OUTPUT
OUT 240Ω*
2.0k
10k
LT1004 2.5
UPDATE The LT3083 allows adjustment to zero. Various single chip switching regulators can be used
15k
+
1k
10k
LT1018
15k
*1% FILM RESISTOR 1MHY = DALE TD-5 TYPE
–
AN02 F05
Figure 5
A = 100mV/DIV AC-COUPLED ON 15.7V DC LEVEL B = 50V/DIV C = 4A/DIV
D = 20V/DIV HORIZONTAL = 100μs/DIV
AN02 F06
Figure 6
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AN2-3
Application Note 2 The 1N4003 damps the flyback spike of the current-limiting inductor. The 4.7kΩ unit ensures circuit start-up and the 68pF-1MΩ combination sets loop hysteresis at about 80mVP-P . This free-running oscillation control mode substantially reduces dissipation in the regulator, while preserving its performance. Despite changes in the input voltage, different regulated outputs or load shifts, the loop always ensures the minimum possible dissipation in the regulator.
Figure 7 shows the dissipation limiting technique applied in a more sophisticated circuit. The AC-powered version provides 0V-35V, 10A regulation under high line-low line (90VAC-140VAC) conditions with good efficiency. In this version, two SCRs and a center-tapped transformer source power to the inductor-capacitor combination. The transformer output is also diode rectified (Trace A, Figure 8), divided down, and used to reset the 0.1μF unit (Trace B)
VZ †
STANCOR P-8675
1MHY 1N4003
20Ω 3
110AC
1
20Ω
t t
LT1038 OR LT1083
+
750Ω*
10,000μF
2
LT1004 1.2
T1
20k
VZ
LT1004 2.5
2.7k –15V LT1004 1.2V
1N4003
15V
+
82k
16k*
1k
1μF
100μF
4
†
1N4003
+
0V-35V 0A-10A (7.5A FOR LT1083)
15V 2
3
8
+
C1 LT1011
10k
15V
–
11k*
200k 7 1
0.1
4
*1% FILM RESISTOR T1 = SPRAGUE 11Z-2003 †SCRs = G.E. C-220B 1MHY = DALE TD-5 TYPE
–15V 15k 15V 2N3904
1N4148
100pF
15V
15V
8
– 7
C2 LT1011 1
+
UPDATE Paralled LT3083s allow adjustment to zero without the LT1004
3
15V 1 15k
2
8
10k
4
+
A1 LM301A
16k*
–
1μF
11k*
–15V –15V
AN02 F07
Figure 7
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AN2-4
Application Note 2 (3.7V). As a result, the circuit functions over all line, load and output voltage conditions with good efficiency. The 1.2V LT1004 at the LT1038 allows the output voltage to be set down to 0.00 and the 2N3904 clamp at A1 prevents loop “hang-up”. Figure 7A shows a way to trigger the SCRs without using a transformer.
via C1. The resulting AC line synchronous ramp at C1’s output is compared to A1’s offset output by C2. A1’s output represents the deviation from the VZ value that the loop is trying to force across the LT1038. When the ramp output exceeds C2’s “+” input value, C2 pulls low, dumping current through T1’s primary (Trace C). This fires the appropriate SCR and a path from the main transformer to the LC pair occurs (Trace D). The resultant current flow (Trace E) is limited by the inductor and charges the capacitor. When the AC line cycle drops low enough, the SCR commutates and charging ceases. On the next half cycle the process repeats, except that the alternate SCR does the work. In this fashion, the loop controls the phase angle at which the SCRs fire to keep the voltage across the LT1038 at VZ
Although A1’s output is an analog voltage, the AC-driven nature of the circuit makes it approximate a smoothed, sample loop response. Conversely, the regulator constitutes a true linear system. Because these two feedback systems are interlocked, frequency compensation can be difficult.
1N4148 20Ω
TO SCR GATES
TO 10k-15k JUNCTION FROM A1 OUTPUT
–
2
+
10,000μF
20Ω
15V 3
10k
1MHY
15V 0.68
10k C2
2N2219
TO C1 OUTPUT
1N4148 AN02 F07A
Figure 7A
A = 50V/DIV B = 10V/DIV C = 100mA/DIV D = 50V/DIV E = 10A/DIV HORIZONTAL = 2ms/DIV
AN02 F08
Figure 8
an2f
AN2-5
Application Note 2 In practice, A1’s 1μF capacitor keeps dissipation loop gain at a low enough frequency for stable characteristics, without influencing the LT1038’s transient response characteristic. Trace A, Figure 9 shows the output noise while the circuit is operating at 35V into a 10A load (350W). Note the absence of fast switching transients and harmonics. The output noise is made up of residual 120Hz ripple and regulator noise. Reflected noise into the AC power line is also negligible (Trace B) because the inductor limits current rise time to about 1ms, much slower than the normal switching supplies. Figure 10 shows a plot of efficiency versus output voltage for a 10A load. At low output voltages, where the static losses across the regulator and SCRs are significant, efficiency suffers, but 85% is attained at the upper extreme.
High voltage output is another area for regulator enhancement. In theory, because the regulator does not have a ground pin, it can regulate high voltages. In normal operation the regulator floats at the supply’s upper level, and as long as the VIN–VOUT maximum differential is not exceeded there are no problems. However, if the output is shorted, the VIN–VOUT maximum is exceeded and device destruction will occur. The circuit of Figure 11 shows a complete high voltage regulator that delivers 100V at 100mA and withstands shorts to ground. Even at 100V output the LT317A functions in the normal mode, maintaining 1.2V between its output and adjustment pin.
100 P = 300W
90
P = 200W
80 EFFICIENCY (%)
10mV/DIV AC-COUPLED ON 35V OUTPUT
70
P = 100W
60 P = 50W
50 40 30 20
200V/DIV
P = 10W
10
LOAD CURRENT = 10A FOR ALL CONDITIONS
0 5
0
15 20 10 OUTPUT VOLTAGE
AN02 F09
HORIZONTAL = 2ms/DIV
30
25
AN02 F10
Figure 9
TRIAD N-48X
Figure 10
1N4004 100V OUTPUT
1N4004
≈120V 115AC
IN
+ 500μF
LT317AT ADJ
OUT 10Ω
Q1 2N6533
0.02μF 1N4148
UPDATE Newer regulators such as the LT3080 and LT3081 allow adjustment to zero
500pF
1N3031 30V
2k 5W
332Ω 1k OUTPUT ADJ 25.5k
AN02 F11
Figure 11
an2f
AN2-6
Application Note 2 Under these conditions the 30V Zener is off and Q1 conducts. When an output short occurs, the Zener conducts, forcing Q1’s base to 30V. This causes Q1’s emitter to clamp 2 VBEs below VZ, well within the VIN–VOUT rating of the regulator. Under these conditions, Q1, a high voltage device, sustains 90V VCE at whatever current the transformer and the regulator’s current limit will support. The transformer specified saturates at 130mA, keeping Q1 well within its safe area as it dissipates 12W. If Q1 and the LT317A are thermally coupled, the regulator will soon go into thermal shutdown and oscillation will commence. This action will continue, protecting the load and the regulator as long as the output remains shorted. the 500pF capacitor and the 10Ω-0.02μF damper aid transient response and the diodes provide safe discharge paths for the capacitors. This approach to high voltage regulation is primarily limited by the power dissipation capability of the device in series with the regulator. Figure 11A uses a vacuum tube (remember them?) to achieve very high short-circuit dissipation capability. The tube allows high voltage operation and is extremely tolerant of overloads. This circuit allows the LT317A to control 600W at 2000V (V1’s plate limit is 300mA) with full short-circuit protection.
75-TH EIMAC
Power is not the only area in which regulator performance can be augmented. Figure 12 shows a way to increase the stability of a regulator’s output over time and temperature. This is particularly useful in powering strain gauge-based transducers. In this circuit the output voltage is divided down and compared to the 2.5V reference by A1, a precision amplifier. A1’s output is used to force the LT317A’s adjustment pin to whatever voltage is required to maintain the 10V output. A1 contributes negligible error. The resistors specified will track within 5ppm/°C and the reference contributes about 20ppm/°C. The regulator’s internal circuitry protects against short circuits and thermal overload. Figure 13’s circuit allows a regulator to remotely sense the feedback voltage, eliminating the effects of voltage drop in the supply lines. This is a concern where high currents must be transmitted over relatively long supply rails or PC traces. Figure 13’s circuit uses A1 to sense the voltage at the point of load. A1’s output, summed with the regulator’s output, modifies the adjustment pin voltage to compensate for the voltage lost across RDROP . The feedback divider is returned through a separate lead from the load, completing the remote sensing scheme. The 5μF capacitor filters noise and the 1k value limits bypass capacitor discharge when power is turned off.
FILIMENT V1
2500V IN 180k 50W
LT317AT ADJ
OUTPUT 2000V
OUT
VIN
IN
LT317AH ADJ
OUTPUT 10V
OUT 2k
1.2k
1N3031
+
2k
A1 LT1001
500k OUTPUT TRIM
UPDATE The LT3085 will allow VOUT to go to zero
1.8M 2W
– *RESISTORS = TRW MAR-6
LT1009 2.5V
AN02 F11A
Figure 11A
15k*
4.99k* AN02 F12
Figure 12
an2f
Information furnished by Linear Technology Corporation is believed to be accurate and reliable. However, no responsibility is assumed for its use. Linear Technology Corporation makes no representation that the interconnection of its circuits as described herein will not infringe on existing patent rights.
AN2-7
Application Note 2 A final circuit allows voltage regulator-powered circuity to run from 110VAC or 220VAC without having to switch transformer windings. Regulator dissipation does not increase for 220VAC inputs. In Figure 14, when T1 is driven from 110VAC, the LT1011 output goes high, allowing the SCR to receive gate bias through the 1.2k resistor. The 1N4002 is off. T1’s output is rectified by the SCR and the regulator sees about 8.5V at its input. If T1 is plugged into a 220VAC source, the negative input at the LT1011 is driven beyond 2.5V and the device’s output clamps low. This steers the SCR’s gate bias to ground through the LT1011’s output transistor. The diodes in the LT1011 output line prevent
reverse voltages from reaching the SCR or the LT1011 output. Now, the SCR goes off and the 1N4002 sources current to the regulator from T1’s center tap. Although T1’s input voltage has doubled, its output potential has halved and the regulator power dissipation remains the same. Figure 15 shows the AC line input versus regulator input voltage transfer function. The switch to center tap drive occurs midway between 110VAC and 220VAC. The hysteresis, a desirable characteristic, occurs because T1’s output voltage shifts with the step change in loading.
RDROP (MAX DROP = 300mV) VIN
IN
LT350A ADJ
5V AT 3A
OUT VIN
–
22Ω
RLOAD
A1 LM301A
+
1
121Ω
1k
8
4 365Ω
25Ω
100pF
5μF AN02 F13
+
HIGH CURRENT RETURN TO GROUND
Figure 13 C-106 (G.E.) T1
IN
+ 5000μF
LT1086 ADJ
OUT 240Ω*
VOUT 5V
+ 10μF
1N4002 110-220AC
720Ω*
1k
18
AN02 F14
1k
*1% FILM RESISTOR T1 = STACO #SP05A012 = 1N4148 UNLESS MARKED
1.6k
3 1M
8
–
1μF
7
LT1011 2
1
+
6.2k
UPDATE The LT3080 regulator allows VOUT to go to zero
16 REGULATOR INPUT VOLTAGE
1.2k
14 12 10 8 6 4 2
4
0 0
LT1009C 2.5V
40
80 120 160 200 AC LINE VOLTAGE—RMS
240
280
AN02 F15
Figure 14
Figure 15 an2f
AN2-8
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