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參數(shù)資料
| 型號(hào)： | HCPL-2602 |
| 英文描述： | High CMR Line Receiver Optocouplers(高共態(tài)抑制線接收光耦器) |
| 中文描述： | 高CMR線接收光耦合器（高共態(tài)抑制線接收光耦器） |
| 文件頁數(shù)： | 14/16頁 |
| 文件大?。?/td> | 263K |
| 代理商： | HCPL-2602 |
14
different circuit configuration
could make t
< t
, in which
case NOR gates would be pre-
ferred. If it is not known whether
t
> t
or t
< t
, or if the
drive conditions may vary over
the boundary for these conditions,
the exclusive-OR flip-flop of
Figure (d) should be used.
RS-422 and RS-423
Line drivers designed for RS-422
and RS-423 generally provide
adequate voltage and current for
operating the HCPL-2602/12.
Most drivers also have
characteristics allowing the
HCPL-2602/12 to be connected
directly to the driver terminals.
Worst case drive conditions,
however, would require current
shunting to prevent overstress of
the HCPL-2602/12.
Propagation Delay, Pulse-
Width Distortion and
Propagation Delay Skew
Propagation delay is a figure of
merit which describes how
quickly a logic signal propagates
through a system. The propaga-
tion delay from low to high (t
)
is the amount of time required for
an input signal to propagate to
the output, causing the output to
change from low to high.
Similarly, the propagation delay
from high to low (t
) is the
amount of time required for the
input signal to propagate to the
output, causing the output to
change from high to low (see
Figure 6).
Pulse-width distortion (PWD)
results when t
and t
differ in
value. PWD is defined as the
difference between t
PLH
and t
PHL
and often determines the
maximum data rate capability of a
transmission system. PWD can be
expressed in percent by dividing
the PWD (in ns) by the minimum
pulse width (in ns) being
transmitted. Typically, PWD on
the order of 20-30% of the
minimum pulse width is tolerable;
the exact figure depends on the
particular application (RS232,
RS422, T-1, etc.).
Propagation delay skew, t
, is an
important parameter to consider
in parallel data applications where
synchronization of signals on
parallel data lines is a concern. If
the parallel data is being sent
through a group of optocouplers,
differences in propagation delays
will cause the data to arrive at the
outputs of the optocouplers at
different times. If this difference
in propagation delays is large
enough, it will determine the
maximum rate at which parallel
data can be sent through the
optocouplers.
Propagation delay skew is defined
as the difference between the
minimum and maximum
propagation delays, either t
PLH
or
t
, for any given group of
optocouplers which are operating
under the same conditions (i.e.,
the same drive current, supply
voltage, output load, and
operating temperature). As
illustrated in Figure 16, if the
inputs of a group of optocouplers
are switched either ON or OFF at
the same time, t
is the
difference between the shortest
propagation delay, either t
or
t
, and the longest propagation
delay, either t
PLH
or t
PHL
.
As mentioned earlier, t
can
determine the maximum parallel
data transmission rate. Figure 17
is the timing diagram of a typical
parallel data application with both
the clock and the data lines being
sent through optocouplers. The
figure shows data and clock
signals at the inputs and outputs
of the optocouplers. To obtain the
maximum data transmission rate,
both edges of the clock signal are
being used to clock the data; if
only one edge were used, the
clock signal would need to be
twice as fast.
Propagation delay skew
represents the uncertainty of
where an edge might be after
being sent through an
optocoupler. Figure 17 shows
that there will be uncertainty in
both the data and the clock lines.
It is important that these two
areas of uncertainty not overlap,
otherwise the clock signal might
arrive before all of the data
outputs have settled, or some of
the data outputs may start to
change before the clock signal
has arrived. From these
considerations, the absolute
minimum pulse width that can be
sent through optocouplers in a
parallel application is twice t
PSK
. A
cautious design should use a
slightly longer pulse width to
ensure that any additional
uncertainty in the rest of the
circuit does not cause a problem.
The t
specified optocouplers
offer the advantages of
guaranteed specifications for
propagation delays, pulse-width
distortion and propagation delay
skew over the recommended
temperature, input current, and
power supply ranges.
相關(guān)PDF資料 |
PDF描述 |
|---|---|
| HCPL-261A | HCMOS Compatible, High CMR, 10 MBd Optocouplers |
| HCPL-261N | High CMR, High Speed TTL Compatible Optocouplers |
| HCPL-2630 | High CMR, High Speed TTL Compatible Optocouplers |
| HCPL-2631 | High CMR, High Speed TTL Compatible Optocouplers |
| HCPL-263A | High CMR, High Speed TTL Compatible Optocouplers |
相關(guān)代理商/技術(shù)參數(shù) |
參數(shù)描述 |
|---|---|
| HCPL-2602#300 | 功能描述:高速光耦合器 1Ch 5mA 600mW RoHS:否 制造商:Avago Technologies 電流傳遞比: 最大波特率: 最大正向二極管電壓:1.75 V 最大反向二極管電壓:5 V 最大功率耗散:40 mW 最大工作溫度:+125 C 最小工作溫度:- 40 C 封裝 / 箱體:SOIC-5 封裝:Tube |
| HCPL-2602#500 | 功能描述:高速光耦合器 1Ch 5mA 600mW RoHS:否 制造商:Avago Technologies 電流傳遞比: 最大波特率: 最大正向二極管電壓:1.75 V 最大反向二極管電壓:5 V 最大功率耗散:40 mW 最大工作溫度:+125 C 最小工作溫度:- 40 C 封裝 / 箱體:SOIC-5 封裝:Tube |
| HCPL-2602-000E | 功能描述:高速光耦合器 1Ch 5mA 600mW RoHS:否 制造商:Avago Technologies 電流傳遞比: 最大波特率: 最大正向二極管電壓:1.75 V 最大反向二極管電壓:5 V 最大功率耗散:40 mW 最大工作溫度:+125 C 最小工作溫度:- 40 C 封裝 / 箱體:SOIC-5 封裝:Tube |
| HCPL2602300E | 制造商:Avago Technologies 功能描述: |
| HCPL-2602-300E | 功能描述:高速光耦合器 1Ch 5mA 600mW RoHS:否 制造商:Avago Technologies 電流傳遞比: 最大波特率: 最大正向二極管電壓:1.75 V 最大反向二極管電壓:5 V 最大功率耗散:40 mW 最大工作溫度:+125 C 最小工作溫度:- 40 C 封裝 / 箱體:SOIC-5 封裝:Tube |
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