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LTC490C Datasheet

  • LTC490C

  • Linear Technology [Differential Driver and Receiver Pair]

  • LINER

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LTC490
APPLICATI
S I FOR ATIO
Cable Termination
The proper termination of the cable is very important.
If the cable is not terminated with its characteristic
impedance, distorted waveforms will result. In severe
cases, distorted (false) data and nulls will occur.
A quick look at the output of the driver will tell how well the
cable is terminated. It is best to look at a driver connected
to the end of the cable, since this eliminates the possibility
of getting reflections from two directions. Simply look at
the driver output while transmitting square wave data. If
the cable is terminated properly, the waveform will look
like a square wave (Figure 9). If the cable is loaded
excessively (47鈩?, the signal initially sees the surge
impedance of the cable and jumps to an initial amplitude.
The signal travels down the cable and is reflected back out
of phase because of the mistermination. When the re-
flected signal returns to the driver, the amplitude will be
lowered. The width of the pedestal is equal to twice the
electrical length of the cable (about 1.5ns/foot). If the
cable is lightly loaded (470鈩?, the signal reflects in phase
and increases the amplitude at the driver output. An input
frequency of 30kHz is adequate for tests out to 4000 feet
of cable.
PROBE HERE
Rt
DX
DRIVER
RECEIVER
RX
Rt = 120鈩?/div>
Rt = 47鈩?/div>
Rt = 470鈩?/div>
LTC490 鈥?TA10
Figure 9. Termination Effects
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 represen-
tation that the interconnection of its circuits as described herein will not infringe on existing patent rights.
U
AC Cable Termination
Cable termination resistors are necessary to prevent un-
wanted reflections, but they consume power. The typical
differential output voltage of the driver is 2V when the
cable is terminated with two 120鈩?resistors, causing
33mA of DC current to flow in the cable when no data is
being sent. This DC current is about 60 times greater than
the supply current of the LTC490. One way to eliminate the
unwanted current is by AC coupling the termination resis-
tors as shown in Figure 10.
120鈩?/div>
C
RECEIVER
RX
C = LINE LENGTH (FT)
16.3pF
LTC490 鈥?TA11
W
U
UO
Figure 10. AC Coupled Termination
The coupling capacitor must allow high frequency energy
to flow to the termination, but block DC and low frequen-
cies. The dividing line between high and low frequency
depends on the length of the cable. The coupling capacitor
must pass frequencies above the point where the line
represents an electrical one-tenth wavelength. The value
of the coupling capacitor should therefore be set at 16.3pF
per foot of cable length for 120鈩?cables.
With the coupling capacitors in place, power is consumed
only on the signal edges, and not when the driver output
is idling at a 1 or 0 state. A 100nF capacitor is adequate for
lines up to 4000 feet in length. Be aware that the power
savings start to decrease once the data rate surpasses
1/(120鈩?/div>
C).
Fault Protection
All of LTC鈥檚 RS485 products are protected against ESD
transients up to 2kV using the human body model (100pF,
1.5k鈩?. However, some applications need more
protection. The best protection method is to connect a
bidirectional TransZorb
from each line side pin to ground
(Figure 11). A TransZorb
is a silicon transient voltage
TransZorb
is a registered trademark of General Instruments, GSI
7

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