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ADCMP609(RevPrA) 데이터 시트보기 (PDF) - Analog Devices

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ADCMP609 Datasheet PDF : 16 Pages
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ADCMP608/ADCMP609
COMPARATOR PROPAGATION
DELAY DISPERSION
The ADCMP608 and ADCMP609 comparator is designed to
reduce propagation delay dispersion over a wide input overdrive
range of 5 mV to VCCI − 1 V. Propagation delay dispersion is the
variation in propagation delay that results from a change in the
degree of overdrive or slew rate (how far or how fast the input
signal exceeds the switching threshold).
Propagation delay dispersion is a specification that becomes
important in high speed, time-critical applications, such as data
communication, automatic test and measurement, and instru-
mentation. It is also important in event-driven applications,
such as pulse spectroscopy, nuclear instrumentation, and
medical imaging. Dispersion is defined as the variation in
propagation delay as the input overdrive conditions are changed
(see Figure 14 and Figure 15).
ADCMP608 and ADCMP609 dispersion is typically <5 ns as
the overdrive varies from 5 mV to 500 mV, and the input slew
rate varies from 2 V/ns to 10 V/ns. This specification applies to
both positive and negative signals because the device has very
closely matched delays for both positive-going and negative-
going inputs, and very low output skews. Remember to add the
actual device offset to the overdrive for repeatable dispersion
measurements.
500mV OVERDRIVE
INPUT VOLTAGE
10mV OVERDRIVE
VN ± VOS
DISPERSION
Q/Q OUTPUT
Figure 14. Propagation Delay—Overdrive Dispersion
INPUT VOLTAGE
1V/ns
10V/ns
VN ± VOS
DISPERSION
Q/Q OUTPUT
Figure 15. Propagation Delay—Slew Rate Dispersion
Preliminary Technical Data
COMPARATOR HYSTERESIS
The addition of hysteresis to a comparator is often desirable in a
noisy environment, or when the differential input amplitudes
are relatively small or slow moving. The transfer function for a
comparator with hysteresis is shown in Figure 16. As the input
voltage approaches the threshold (0.0 V, in this example) from
below the threshold region in a positive direction, the
comparator switches from a low to a high when the input crosses
+VH/2. The new switching threshold becomes −VH/2. The
comparator remains in the high state until the threshold −VH/2
is crossed from below the threshold region in a negative
direction. In this manner, noise or feedback output signals
centered on 0.0 V input cannot cause the comparator to switch
states unless it exceeds the region bounded by ±VH/2.
OUTPUT
VOH
VOL
0
–VH
2
INPUT
+VH
2
Figure 16. Comparator Hysteresis Transfer Function
The customary technique for introducing hysteresis into a
comparator uses positive feedback from the output back to the
input. One limitation of this approach is that the amount of
hysteresis varies with the output logic levels, resulting in
hysteresis that is not symmetric about the threshold. The
external feedback network can also introduce significant
parasitics that reduce high speed performance, and can even
induce oscillation in some cases.
The ADCMP609 comparator offers a programmable hysteresis
feature that significantly improves accuracy and stability.
Connecting an external pull-down resistor or a current source
from the LE/HYS pin to GND, varies the amount of hysteresis
in a predictable and stable manner. Leaving the LE/HYS pin
disconnected or driving it high removes the hysteresis. The
maximum hysteresis that can be applied using this pin is
approximately 160 mV. Figure 17 illustrates the amount of
hysteresis applied as a function of external resistor value.
Figure TBD illustrates hysteresis as a function of current.
Rev. PrA | Page 10 of 16

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