10
LT1713/LT1714
Figure 2. Various Configurations for Introducing Hysteresis
+
50k
V
IN
50
Q
Q
V
+
= 5V
V
= –5V
V
HYST
= 5mV
(ALL 3 CASES)
Q
Q
+
50k
V
IN
V
REF
50
Q
Q
+
100k
100k
V
IN
+
V
IN
50
50
171314 F02
LT1713
LT1713 LT1713
Hysteresis
Another useful technique to avoid oscillations is to provide
positive feedback, also known as hysteresis, from the
output to the input. Increased levels of hysteresis, how-
ever, reduce the sensitivity of the device to input voltage
levels, so the amount of positive feedback should be
tailored to particular system requirements. The
LT1713/LT1714 are completely flexible regarding the ap-
plication of hysteresis, due to rail-to-rail inputs and the
complementary outputs. Specifically, feedback resistors
can be connected from one or both outputs to their
corresponding inputs without regard to common mode
considerations. Figure 2 shows several configurations.
APPLICATIO S I FOR ATIO
WUUU
11
LT1713/LT1714
TYPICAL APPLICATIO S
U
Simultaneous Full Duplex 75Mbaud Interface
with Only Two Wires
The circuit of Figure 3 shows a simple, fully bidirectional,
differential 2-wire interface that gives good results to
75Mbaud, using the LT1714. Eye diagrams under condi-
tions of unidirectional and bidirectional communication
are shown in Figures 4 and 5. Although not as pristine as
the unidirectional performance of Figure␣ 4, the perfor-
mance under simultaneous bidirectional operation is still
excellent. Because the LT1714 input voltage range ex-
tends 100mV beyond both supply rails, the circuit works
with a full ±3V (one whole V
S
up or down) of ground
potential difference.
The circuit works well with the resistor values shown, but
other sets of values can be used. The starting point is the
characteristic impedance, Z
O
, of the twisted-pair cable.
The input impedance of the resistive network should
match the characteristic impedance and is given by:
RR
RRR
RRRR
IN O
O
=
+
++
[]
2
123
2123
••
||( )
•||( )
This comes out to 120 for the values shown. The
Thevenin equivalent source voltage is given by:
VV
RRR
RRR
R
RRRR
TH S
O
O
=
+
++
++
[]
(–)
()
•||( )
231
231
2123
+
1/2
LT1714
TxD
RxD
7
8
9
LE
6
5
49.9
750k
750k
100k
100k
49.9
2
1
15
3
16
13
14
3V
3V
4
11
12
R2A
2.55k
R3A
124
R
OA
140
R
OB
140
R1B
499
6-FEET
TWISTED PAIR
Z
O
120
R1D
499
R1C
499
R3B
124
R2C
2.55k
3V
100k
5
11
2
1
12
6
10
9
8
7
171314 F03
14
3
15
16
13
4
TxD
RxD
3V
R3C
124
R3D
124
R2D
2.55k
R2B
2.55k
R1A
499
10
+
1/2
LT1714
LE
+
750k
750k
49.9
49.9
100k
+
LE
1/2
LT1714
LE
1/2
LT1714
3V 3V
DIODES: BAV99
×4
Figure 3. 75Mbaud Full Duplex Interface on Two Wires
12
LT1713/LT1714
TYPICAL APPLICATIO S
U
Figure 4. Performance of Figure 3’s Circuit When
Operated Unidirectionally. Eye is Wide Open
171112 F04
Figure 5. Performance When Operated Simultaneous
Bidirectionally (Full Duplex). Crosstalk Appears as Noise.
Eye is Slightly Shut But Performance is Still Excellent
171112 F05
This amounts to an attenuation factor of 0.0978 with the
values shown. (The actual voltage on the lines will be cut
in half again due to the 120 Z
O
.) The reason this
attenuation factor is important is that it is the key to
deciding the ratio between the R2-R3 resistor divider in
the receiver path. This divider allows the receiver to reject
the large signal of the local transmitter and instead sense
the attenuated signal of the remote transmitter. Note that
in the above equations, R2 and R3 are not yet fully
determined because they only appear as a sum. This
allows the designer to now place an additional constraint
on their values. The R2-R3 divide ratio should be set to
equal half the attenuation factor mentioned above or:
R3/R2 = 1/2 • 0.0976
1
.
Having already designed R2 + R3 to be 2.653k (by allocat-
ing input impedance across R
O
, R1 and R2 + R3 to get the
requisite 120), R2 and R3 then become 2529 and
123.5 respectively. The nearest 1% value for R2 is 2.55k
and that for R3 is 124.
Voltage-Tunable Crystal Oscillator
The front page application is a variant of a basic crystal
oscillator that permits voltage tuning of the output fre-
quency. Such voltage-controlled crystal oscillators (VCXO)
are often employed where slight variation of a stable
carrier is required. This example is specifically intended to
provide a 4× NTSC sub-carrier tunable oscillator suitable
for phase locking.
The LT1713 is set up as a crystal oscillator. The varactor
diode is biased from the tuning input. The tuning network
is arranged so a 0V to 5V drive provides a reasonably
symmetric, broad tuning range around the 14.31818MHz
center frequency. The indicated selected capacitor sets
tuning bandwidth. It should be picked to complement loop
response in phase locking applications. Figure 6 is a plot
of tuning input voltage versus frequency deviation. Tuning
deviation from the 4× NTSC 14.31818MHz center fre-
quency exceeds ±240ppm for a 0V to 5V input.
1
Using the design value of R2 + R3 = 2.653k rather than the implementation value of 2.55k +
124 = 2.674k.
INPUT VOLTAGE (V)
0
FREQUENCY DEVIATION (kHz)
2
4
5
9
8
7
6
5
4
3
2
1
0
171112 F06
13
14.314.0MHz
14.31818MHz
14.3217MHz
Figure 6. Control Voltage vs Output Frequency for the First Page
Application Circuit. Tuning Deviation from Center Frequency
Exceeds ±240ppm

LT1713IMS8#PBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
Analog Comparators 1x, 7ns, L Pwr, 3V/5V/ 5V R2R Comps
Lifecycle:
New from this manufacturer.
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