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Transcript
New Comparators Feature Micropower Operation
Under All Conditions – Design Note 137
Jim Williams
Some micropower comparators have operating modes
that allow excessive current drain. In particular, poorly
designed devices can conduct large transient currents
during switching. Such behavior causes dramatically
increased power drain with rising frequency, or when
the inputs are nearly balanced, as in battery monitoring
applications.
resulting in greatly reduced power consumption versus
frequency, or when the inputs are nearly balanced. Figure 2’s
plot contrasts the LTC1440’s power consumption versus
frequency with that of another comparator specified as a
micropower component. The LTC1440 has about 200 times
lower current consumption at higher frequencies, while
maintaining a significant advantage below 1kHz.
Figure 1 shows a popular micropower comparator’s current
consumption during switching. Trace A is the input pulse,
trace B is the output response and trace C is the supply
current. The device, specified for micropower level supply drain, pulls 40mA during switching. This undesirable
surprise can upset a design’s power budget or interfere
with associated circuitry’s operation.
Table 1 shows some LTC1440 family characteristics. A voltage reference and programmable hysteresis are included
in some versions, with 5µs response time for all devices.
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.
10000
SUPPLY CURRENT (µA)
The LTC®1440 series comparators are true micropower
devices. They eliminate current peaking during switching,
The new devices permit high performance circuitry with
low power drain. Figure 3’s quartz oscillator, using a
A = 1V/DIV
B = 10V/DIV
C = 20mA/DIV
1000
100
Figure 1. Poorly Designed “Micropower” Comparator
Pulls Huge Currents During Transitions. Result Is
Excessive Current Consumption with Frequency
“MICROPOWER”
COMPARATOR
LTC1440
10
1
DN137 F01
1µs/DIV
VS = 5V
1
10
1k
10k
100
INPUT FREQUENCY (Hz)
100k
DN137 F02
Figure 2. The LTC1440 Family Draws 200 Times Lower
Current at Frequency Than Another Comparator
Table 1. Some Characteristics of the LTC1440 Family of Micropower Comparators
PART
NUMBER
NUMBER OF
PROGRAMMABLE
COMPARATORS REFERENCE
HYSTERESIS
PACKAGE
PROP. DELAY
(100mV OVERDRIVE)
SUPPLY
RANGE
SUPPLY
CURRENT
LTC1440
1
1.182V
Yes
8-Lead PDIP, SO
5µs
2V to 11V
4.7µA
LTC1441
2
No
No
8-Lead PDIP, SO
5µs
2V to 11V
5.7µA
LTC1442
2
1.182V
Yes
8-Lead PDIP, SO
5µs
2V to 11V
5.7µA
LTC1443
4
1.182V
No
16-Lead PDIP, SO
5µs
2V to 11V
8.5µA
LTC1444
4
1.221V
Yes
16-Lead PDIP, SO
5µs
2V to 11V
8.5µA
LTC1445
4
1.221V
Yes
16-Lead PDIP, SO
5µs
2V to 11V
8.5µA
09/96/137_conv
standard 32.768kHz crystal, starts under all conditions
with no spurious modes. Current drain is only 9µA at a
2V supply.
Figure 4’s voltage-to-frequency converter takes full advantage of the LTC1441’s low power consumption under
dynamic conditions. A 0V to 5V input produces a 0Hz to
10kHz output, with 0.02% linearity, 60ppm/°C drift and
40ppm/V supply rejection. Maximum current consumption is only 26µA, 100 times lower than currently available
circuits. C1 switches a charge pump, comprising Q5, Q6
and the 100pF capacitor, to maintain its negative input
32.768kHz
1M
V+
2V TO 11V
470k
OUT
–
1.2M
10pF
Start-up or input overdrive can cause the circuit’s ACcoupled feedback to latch. If this occurs, C1’s output goes
low; C2, detecting this via the 2.7M/0.1µF lag, goes high.
This lifts C1’s positive input and grounds the negative
input with Q7, initiating normal circuit action.
Figure 5 shows the circuit’s power consumption versus
frequency. Zero frequency current is just 15µA, increasing
to only 26µA at 10kHz.
+
1/2 LTC1441
at 0V. The LT1004s and associated components form a
temperature-compensated reference for the charge pump.
The 100pF capacitor charges to a fixed voltage; hence,
the repetition rate is the circuit’s only degree of freedom
to maintain feedback. Comparator C1 pumps uniform
packets of charge to its negative input at a repetition rate
precisely proportional to the input voltage derived current.
This action ensures that circuit output frequency is strictly
and solely determined by the input voltage.
A detailed description of this circuit’s operation appears
in the August 1996 issue of Linear Technology magazine.
DN137 F03
= STATEK CX1-V
Figure 3. 32.768kHz “Watch Crystal” Oscillator Has No
Spurious Modes. Circuit Pulls 9µA at VS = 2V
V + = 6.2 TO 12V
35
2.2µF
6.04k*
Q8
Q1
–
C1
1/2 LTC1441
0.01µF
LT1004
1.2V
×3
+
50pF
+
Q2
0.47µF
CURRENT CONSUMPTION (µA)
INPUT
0V TO 5V
+
10kHz
TRIM
1.2M* 200k
LM334
30
25
20
SLOPE = 1.1µA/kHz
15
10
5
100k
0
Q3
15k
Q5
Q7
100Hz TRIM
3M TYP
Q6
100pF†
Q1, Q2, Q8 = 2N5089
ALL OTHER = 2N2222
†
= POLYSTYRENE
* = 1% METAL FILM
GROUND ALL UNUSED 74C14 INPUTS
10M
1
2
3
4 5 6 7 8 9 10 11 12
FREQUENCY (kHz)
DN137 F05
Q4
74C14
OUTPUT
= HP5082-2810
= 1N4148
0
2.7M
0.1
Figure 5. Current Consumption vs Frequency
for the V-to-F Converter. Discharge Cycles
Dominate 1.1µA/kHz Current Drain Increase
–
C2
1/2 LTC1441
+
DN137 F04
Figure 4. LTC1441-Based 0.02% V/F Converter Requires
Only 26µA Supply Current
Data Sheet Download
www.linear.com/LTC1440
Linear Technology Corporation
For applications help,
call (408) 432-1900
dn137f_conv LT/GP 0996 155K • PRINTED IN THE USA
1630 McCarthy Blvd., Milpitas, CA 95035-7417
(408) 432-1900
●
FAX: (408) 434-0507 ● www.linear.com
 LINEAR TECHNOLOGY CORPORATION 1996