LT1016
10
1016fc
applicaTions inForMaTion
In Figure 7 the probes are properly selected and applied
but the LT1016’s output rings and distorts badly. In this
case, the probe ground lead is too long. For general pur
-
pose work most probes come with ground leads about six
inches long. At low frequencies this is fine. At high speed,
the long ground lead looks inductive, causing the ringing
shown. High quality probes are always supplied with some
short ground straps to deal with this problem. Some come
with very short spring clips which fix directly to the probe
tip to facilitate a low impedance ground connection. For
fast work, the ground connection to the probe should not
exceed one inch in length. Keep the probe ground con
-
nection as short as possible.
Figure 8 shows the LT1016’s output (Trace B) oscillating
near 40MHz as it responds to an input (Trace A). Note that
the input signal shows artifacts of the oscillation. This
example is caused by improper grounding of the com
-
parator. In
this case, the LT1016’s GND pin connection is
one
inch long. The ground lead of the LT1016 must be as
short
as possible and connected directly to a low impedance
ground
point. Any substantial impedance in the LT1016’s
ground path will generate effects like this. The reason for
this is related to the necessity of bypassing the power
supplies. The inductance created by a long device ground
lead permits mixing of ground currents, causing undesired
effects in the device. The solution here is simple. Keep the
LT1016’s ground pin connection as short (typically 1/4
inch) as possible and run it directly to a low impedance
ground. Do not use sockets.
Figure 9 addresses the issue of thelow impedance
ground,” referred to previously. In this example, the
output is clean except for chattering around the edges.
This photograph was generated by running the LT1016
without aground plane.” A ground plane is formed by
using a continuous conductive plane over the surface of
the circuit board. The only breaks in this plane are for the
circuit’s necessary current paths. The ground plane serves
two functions. Because it is flat (AC currents travel along
the surface of a conductor) and covers the entire area of
the board, it provides a way to access a low inductance
ground from anywhere on the board. Also, it minimizes
the effects of
stray capacitance in the circuit by referring
them
to ground. This breaks up potential unintended and
harmful feedback paths. Always use a ground plane with the
LT1016 when input signal levels are low or slow moving.
Figure 9. Transition Instabilities Due to No Ground Plane
Figure 7. Typical Results Due to Poor Probe Grounding
Figure 8. Excessive LT1016 Ground Path
Resistance Causes Oscillation
1V/DIV
20ns/DIV
1016 F07
TRACE A
1V/DIV
TRACE B
2V/DIV
100ns/DIV
1016 F08
2V/DIV
100ns/DIV
1016 F09
LT1016
11
1016fc
applicaTions inForMaTion
“Fuzz” on the edges is the difficulty in Figure 10. This
condition appears similar to Figure 10, but the oscillation
is more stubborn and persists well after the output has
gone low. This condition is due to stray capacitive feed
-
back from the outputs to the inputs. A 3kΩ input source
impedance
and 3pF of stray feedback allowed this oscil-
lation. The
solution for this condition is not too difficult.
Keep
source impedances as low as possible, preferably
1k or less. Route output and input pins and components
away from each other.
The opposite of stray-caused oscillations appears in
Figure 11. Here
,
the output response (Trace B) badly lags
the input (Trace A). This is due to some combination of
high source impedance and stray capacitance to ground
at the input. The resulting RC forces a lagged response
at the input and output delay occurs. An RC combination
of 2k source resistance and 10pF to ground gives a 20ns
time constant—significantly longer than the LT1016’s
response time. Keep source impedances low and minimize
stray input capacitance to ground.
Figure 12 shows another capacitance related problem.
Here the output does not oscillate, but the transitions
are discontinuous and
relatively slow.
The villain of this
situation is a large output load capacitance. This could
be
caused by cable driving, excessive output lead
length or the input characteristics of the circuit being
driven. In most situations this is undesirable and may be
eliminated by buffering heavy capacitive loads. In a few
circumstances it may not affect overall circuit operation
and is tolerable. Consider the comparator’s output load
characteristics and
their potential effect on the circuit. If
necessary, buffer the load.
Figure 11. Stray 5pF Capacitance from
Input to Ground Causes Delay
Figure 12. Excessive Load Capacitance Forces Edge Distortion
Figure 10. 3pF Stray Capacitive Feedback
with 3kΩ Source Can Cause Oscillation
2V/DIV
50ns/DIV
1016 F10
TRACE A
2V/DIV
TRACE B
2V/DIV
10ns/DIV
1016 F11
2V/DIV
100ns/DIV
1016 F12
LT1016
12
1016fc
applicaTions inForMaTion
Another output-caused fault is shown in Figure 13. The
output transitions are initially correct but end in a ringing
condition. The key to the solution here is the ringing. What
is happening is caused by an output lead that is too long.
The output lead looks like an unterminated transmission
line at high frequencies and reflections occur. This ac
-
counts for the abrupt reversal of direction on the leading
edge and the ringing. If the comparator is driving TTL this
may be acceptable, but other loads may not tolerate it. In
this instance, the direction reversal on the leading edge
might cause trouble in a fast TTL load. Keep output lead
lengths short. If they get much longer than a few inches,
terminate with a resistor (typically 250Ω to 400Ω).
200ns-0.01% Sample-and-Hold Circuit
Figure 14’s circuit uses the LT1016’s high speed to
improve upon
a standard circuit function. The 200ns
acquisition time is well beyond monolithic sample-and-
hold capabilities. Other specifications exceed the best
commercial unit’s performance. This circuit also gets
around many of the problems associated with standard
sample-and-hold approaches, including FET switch errors
and amplifier settling time. To achieve this, the
LT1016’s
high speed is used in a circuit which completely abandons
traditional sample-and-hold methods.
Important specifications for this circuit include:
Acquisition Time <200ns
Common Mode Input Range ±3V
Droop 1µV/µs
Hold Step 2mV
Hold Settling Time 15ns
Feedthrough Rejection >>100dB
When the sample-and-hold line goes low, a linear ramp
starts just below the input level and ramps upward. When
the ramp voltage reaches the input voltage, A1 shuts off the
ramp, latches itself off and sends out a signal indicating
sampling is complete.
Figure 14. 200ns Sample-and-Hold
Figure 13. Lengthy, Unterminated Output Lines
Ring from Reflections
1V/DIV
50ns/DIV
1016 F13
+
1k
DELAY
COMP
1N4148
1N4148
1N4148
8pF
100Ω
390Ω
470Ω 100Ω
100Ω
300Ω
Q1
2N5160
Q3
2N2369
Q6
2N2222
Q2
2N2907A
5.1k
5.1k 1.5k
0.1µF
1000pF
(POLYSTYRENE)
390Ω
1k
SN7402 SN7402
SN7402
NOW
A1
LT1016
SAMPLE-HOLD
COMMAND (TTL)
OUTPUT
5V
5V
–15V
INPUT
3V
220Ω
1.5k
1.5k
Q5
2N2222
LT1009
2.5V
820Ω
1016 F14
Q7
2N5486
LATCH
Q4
2N2907A

LT1016IS8#PBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Analog Comparators High Speed COMPARATOR
Lifecycle:
New from this manufacturer.
Delivery:
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