LM1893 [NSC]

LM1893/LM2893 Carrier-Current Transceiver; LM1893 / LM2893载波电流收发器
LM1893
型号: LM1893
厂家: National Semiconductor    National Semiconductor
描述:

LM1893/LM2893 Carrier-Current Transceiver
LM1893 / LM2893载波电流收发器

文件: 总24页 (文件大小:576K)
中文:  中文翻译
下载:  下载PDF数据表文档文件
April 1995  
²
LM1893/LM2893 Carrier-Current Transceiver  
General Description  
Y
Output power easily boosted 10-fold  
50 to 300 kHz carrier frequency choice  
TTL and MOS compatible digital levels  
Regulated voltage to power logic  
Carrier-current systems use the power mains to transfer in-  
formation between remote locations. This bipolar carrier-  
current chip performs as a power line interface for half-du-  
plex (bi-directional) communication of serial bit streams of  
virtually any coding. In transmission, a sinusoidal carrier is  
FSK modulated and impressed on most any power line via a  
rugged on-chip driver. In reception, a PLL-based demodula-  
tor and impulse noise filter combine to give maximum range.  
A complete system may consist of the LM1893, a COPSTM  
controller, and discrete components.  
Y
Y
Y
Y
Drives all conventional power lines  
Applications  
Y
Energy management systems  
Y
Home convenience control  
Y
Inter-office communication  
Y
Appliance control  
Features  
Y
Y
Fire alarm systems  
Noise resistant FSK modulation  
Y
Security systems  
Y
User-selected impulse noise filtering  
Y
Telemetry  
Y
Up to 4.8 kBaud data transmission rate  
Y
Computer terminal interface  
Y
Strings of 0’s or 1’s in data allowed  
Y
Sinusoidal line drive for low RFI  
Typical Application  
TL/H/6750–1  
FIGURE 1. Block diagram of carrierÐcurrent chip with a complement of discrete components making a complete  
e
360 Baud transceiver. Use caution with this circuitÐdangerous line voltage is present.  
e
F
O
125 kHz, f  
DATA  
BI-LINETM and COPSTM are trademarks of National Semiconductor Corp.  
²
Carrier-Current Transceivers are also called Power Line Carrier (PLC) transceivers.  
C
1995 National Semiconductor Corporation  
TL/H/6750  
RRD-B30M115/Printed in U. S. A.  
Absolute Maximum Ratings  
If Military/Aerospace specified devices are required,  
please contact the National Semiconductor Sales  
Office/Distributors for availability and specifications.  
e
25 C,  
Maximum continuous dissipation, T  
plastic DIP N (Note 2): transmit mode  
§
A
1.66 W  
1.33 W  
receive mode  
b
Operating ambient temp. range  
Storage temperature range  
Lead temp., soldering, 7 seconds  
40 to 85 C  
§
Supply voltage  
Voltage on pin 12  
30 V  
55 V  
41 V  
40 V  
100 mA  
b
65 to 150 C  
260 C  
§
§
Voltage on pin 10 (Note 1)  
Voltage on pins 5 and 17  
5.6 V DC zener current  
Junction temperature: transmit mode  
receive mode  
Note: Absolute maximum ratings indicate limits beyond  
which damage to the device may occur. Electrical specifica-  
tions are not ensured when operating the device above  
guaranteed limits but below absolute maximum limits, but  
there will be no device degradation.  
150 C  
125 C  
§
§
Electro-Static Discharge (120 pF, 1500X)  
1KV  
General Electrical Characteristics  
O
(Note 3). The test conditions are: Va 18V and F  
e
e
125 kHz, unless otherwise noted.  
Test  
Limit  
(Note 4)  
Design  
Limit  
(Note 5)  
Limit  
Units  
Ý
Parameter  
5.6 V Zener voltage, V  
Conditions  
Typical  
e
Pin 11, I  
Z
1
2 mA  
5.6  
5.2  
5.9  
V min.  
V max.  
Z
@
(V 10 mA  
@
e
b
b
1 mA)/(10 mA 1 mA)  
2
3
5.6 V Zener resistance, R  
Pin 11, R  
V
5
X
Z
Z
Z
Z
Carrier I/O peak survivable  
transient voltage, V  
Pin 10, discharge 1 mF cap. charged to V  
OT  
80  
60  
V max.  
k
thru 1X  
OT  
Carrier I/O clamp voltage, V  
e
4
Pin 10, I 10 mA, RX mode  
OC  
2N2222 diode pin 8 to 9  
44  
41  
50  
V min.  
V max.  
OC  
e
5
6
7
8
Carrier I/O clamp resistance, R  
10  
Pin 10, I  
Pin 5  
10 mA  
20  
1.8  
2.2  
X
OC  
TX/RX low input voltage, V  
IL  
0.8  
2.8  
V max.  
V min.  
TX/RX high input voltage, V  
Pin 5 (Note 9)  
Pin 5 at 0.8 V  
IH  
b
b
20  
1
TX/RX low input current, I  
IL  
2
mA min.  
mA max.  
b
1
10  
9
TX/RX high input current, I  
IH  
Pin 5 at 40 V  
0
mA min.  
mA max.  
10b  
10  
2
4
b
RX TX switch-over time, T  
10  
11  
Time to develop 63% of full current drive thru pin 10  
ms  
RT  
b
TX RX switch-over time, T  
e
1/(2F  
DATA  
1 bit time, T  
). Time T is user  
TR  
bit  
TR  
B
controlled with C , see Apps. Info.  
M
e
F )/2  
2
e
6.65 kX, C  
O
12  
ICO initial accuracy of F  
TX mode, R  
e
560 pF  
125  
113  
137  
kHz min.  
kHz max.  
O
O
a
F
(F  
0
1
b
b
T )  
JMIN  
b
100  
13  
14  
ICO temperature coefficient of F  
TX or RX mode, (F  
F
)/(T  
PPM/ C  
§
% max.  
O
OMAX  
OMIN  
JMAX  
s
s
T
JMAX  
b
TX or RX mode, 40  
g
g
5.0  
Temperature drift of F  
T
J
2.0  
O
Transmitter Electrical Characteristics (Note 3). The test conditions are: Va 18 V and F 125 kHz  
e
e
O
unless otherwise noted. The transmit center frequency is F , FSK low is F , and FSK high is F .  
O
1
2
Test  
Limit  
(Note 4)  
Design  
Limit  
(Note 5)  
Limit  
Units  
Ý
Parameter  
Conditions  
Typical  
15  
Supply voltage, Va, range  
13  
40  
14  
24  
15  
23  
V min.  
V max.  
e
Meets test 17 spec. at T 25 C and:  
J
§
k
b
b
[
[
]
]
[
[
]
]
[
[
]
]
(F 14V  
F
18V )/F 18V  
0.01  
0.01  
l
l
1
(F 24V  
1
1
1
18V )/F 18V  
l
k
F
1
1
l
16  
Total supply current, I  
QT  
Pin 15. Pin 12 high. I is I through  
52  
79  
mA max.  
QT  
Q
pin 15 and the average current I  
Carrier I/O through pin 10  
of the  
ODC  
17  
18  
Carrier I/O output current, I  
100X load on pin 10  
70  
45  
mApp min.  
O
Carrier I/O lower swing limit, V  
ALC  
Pin 10. Set internally be ALC.  
2N2222 diode pin 8 to 9  
4.7  
4.0  
5.7  
V min.  
V max.  
19  
20  
THD of I (Note 6)  
O
Q of 10 tank driving 10X line  
100X load, no tank  
0.6  
5.5  
5.0  
9
% max.  
% max.  
b
b
(F F )/( F  
a
F
1
[
]
/2)  
FSK deviation, F  
F
4.4  
3.7  
5.2  
% min.  
% max.  
2
1
2
1
2
21  
22  
23  
Data In. low input voltage, V  
IL  
Pin 17  
1.7  
2.1  
0.8  
2.8  
V max.  
V min.  
Data In. high input voltage, V  
IH  
Pin 17 (Note 9)  
Pin 17 at 0.8 V  
b
b
10  
1
Data In. low input current, I  
IL  
1
mA min.  
mA max.  
b
1
10  
24  
Data In. high input current, I  
IH  
Pin 17 at 40 V  
0
mA min.  
mA max.  
10b  
4
2
Receiver Electrical Characteristics (Note 3). The test conditions are: Va 18 V, F 125 kHz, 2.2%  
e
e
g
O
e
e
100 mVpp, in the receive mode, unless otherwise noted.  
deviation FSK, F  
2.4 kHz, V  
IN  
DATA  
Test  
Limit  
(Note 4)  
Design  
Limit  
(Note 5)  
Limit  
Units  
Ý
Parameter  
Conditions  
Typical  
25  
26  
27  
28  
Supply voltage, Va, range  
Functional receiver (Note 7)  
12  
37  
13  
30  
13.5  
28  
V min.  
V max.  
Supply current, I  
QT  
I
is pin 15 (Va) plus pin 10  
11  
19.5  
10  
5
14  
mA min.  
mA max.  
QT  
(Carrier I/O) current. 2.4 kX Pin 13 to GND.  
Carrier I/O input resistance, R  
Pin 10  
14  
30  
kX min.  
kX max.  
10  
e
Max. data rate, F  
MD  
Functional receiver (Note 7), C  
e
2.4 kHz 4.8 kBaud  
100 pF,  
4.8  
2.4  
kBaud  
F
R
0X, no tank,  
F
e
e
e
e
e
g
g
g
g
g
10  
29  
30  
31  
PLL capture range, F  
C
C
100 pF, R  
0 X  
0 X  
40  
45  
15  
15  
% min.  
% min.  
C
F
F
F
F
PLL lock range, F  
100 pF, R  
L
Receiver input sensitivity, S  
IN  
For a functional receiver (Note 8)  
Referred to chip side (pin 10)  
1.8  
2.0  
1.4  
0.26  
0.29  
0.20  
10  
12  
mV  
RMS  
mV  
RMS  
e
e
of the line-coupling XFMR: F  
F
50 kHz  
300 kHz  
O
mV  
RMS  
mV  
RMS  
mV  
RMS  
mV  
RMS  
O
Referred to line side of XFMR:  
e
e
(assuming a 7.07:1 XFMR) F  
F
50 kHz  
300 kHz  
O
O
32  
Tolerable input dc voltage offset  
range, V  
Pin 10 lower than pin 15 by V  
2
0.1  
V max.  
INDC  
INDC  
Data Out. breakdown voltage  
Data Out. low output, V  
s
33  
34  
35  
Pin 12, leakage I 20 mA  
70  
55  
V min.  
V max.  
e
Pin 12, sat. voltage at I  
OL  
2 mA  
0.15  
0.4  
OL  
Impulse noise filter current, I  
g
g
g
Pin 13 charge and discharge current  
55  
45  
85  
mA min.  
mA max.  
I
36  
37  
38  
39  
40  
41  
42  
43  
Offset hold cap. bias voltage, V  
CM  
Pin 6  
2.0  
1.3  
3.5  
V min.  
V max.  
b
Pin 6. V(pin 3) V(pin 4)  
e
g
g
g
g
Offset hold capacitor max. drive  
current, I  
250 mV  
55  
25  
80  
mA min.  
mA max.  
MCM  
Offset hold bias current, I  
b
b
b
40  
40  
Pin 6, TX mode. Bias pin 6 as it self-  
biased during test 31.  
0.5  
20  
nA min.  
nA max.  
OHB  
Phase comparator current, I  
PC  
Bias pins 3 and 4 at 8.5 V  
a
100  
10  
50  
200  
mA min.  
mA max.  
e
I
I(pin 3)  
I(pin 4), TX mode  
PC  
Phase detector output resistance,  
Pins 3 and 4.  
@
6
18  
kX min.  
kX max.  
@
e
b
V
R
R
PD  
(V 100mA  
50mA)/(50mA)  
PD  
Phase detector demodulated output  
voltage, V  
Pin 3 to 4, measured after filtering  
out the 2F component  
100  
0.95  
80  
60  
180  
mVpp min.  
mVpp max.  
PD  
Fast offset cancel voltage ‘‘window’’  
-to-V ratio, V /V  
O
b
e
a
DC offset  
WINDOW  
g
V
PIN3  
V
PIN4  
V
0.70  
1.20  
V/V min.  
V/V max.  
g
Drive for 1 mA pin 6 current  
PD  
W
PD  
e
e
CMRR. 120 Hz  
Power supply rejection, PSRR  
C
L
0.1 mF. PSRR  
dB min.  
Note 1: More accurately, the maximum voltage allowed on pin 10 is V , and V  
OC  
ranges from 41 to 50V. Also, transients may reach above 60V; see the transient  
OC  
peak voltage characteristic curve.  
Note 2: The maximum power dissipation rating should be derated for device operation above 25 C to insure that the junction temperature remains below the  
§
maximum rating. Use a i of 75 C/W for the N package using a socket in still air (which is the worst case). Consult the Application Information section for more  
§
JA  
detail.  
e
e
25 C. Pin  
Note 3: The boldface values apply over the full junction temperature range for the specified supply voltage range. All other numbers apply at T  
T
§
A
J
numbers refer to LM1893. LM2893 tested by shorting Carrier In to Carrier Out and testing it as an LM1893.  
Note 4: Guaranteed and 100% production tested.  
Note 5: Guaranteed (but not 100% production tested) over the temperature and supply voltage ranges. These limits are not used to calculate outgoing quality  
levels.  
e
[
]
O
[
(all components at or above 2F ) / I  
]
(fundamental) .  
Note 6: Total harmonic distortion is measured using THD  
I
RMS  
RMS  
Note 7: Receiver function is defined as the error-free passage of 1 cycle of 50% duty-cycle 2.4 kHz square-wave data (2 sequential 208 mS bits), with the first bit  
g
g
being a ‘‘1.’’ All of the data transitions (edges) must fall within 10% ( 20.8 ms) of their noise-free positions. RX time delay is minimized by using no impulse noise  
filter cap. C for this test.  
I
e
Note 8: During the sensitivity check, note 7 requirements are followed with these exceptions: (1) data rate F  
g
approximately 6200 pF).  
1.2 kHz, (2) all of the data transitions must fall  
DATA  
g
within 20% ( 41.6 ms) of their noise-free positions, and (3), a time-domain filter capacitor (C ) is used. The time delay of C is (/2 bit, or 208 ms. (C is  
I
I
I
Note 9: For TTL compatibility use a pull-up resistor to increase min. V  
to above 2.8 V.  
OH  
3
Typical Performance Characteristics (Va 18V, F  
e
e
125 kHz, circuit ofFigure 1, pin numbers for  
O
LM1893)  
Total Current Consumption,  
, vs Supply Voltage  
Total Current Consumption,  
, vs Junction Temperature  
Chip Bias Current,  
i , vs Supply Voltage  
Q
I
I
QT  
QT  
n  
TL/H/675038  
4
Typical Performance Characteristics (Continued)  
Maximum Data Rate vs  
Junction Temperature  
Receiver Sensitivity vs  
Junction Temperature  
PLL Lock Range vs  
Junction Temperature and F  
O
Filter  
TL/H/675039  
5
Dual-In-Line Package  
Application Information*  
THE DATA PATH  
The BI-LINETM chip serves as a power line interface in the  
carrier-current transceiver (CCT) system of Figure 3. Figure  
4 shows the interface circuit now discussed. The controller  
may select either the transmit (TX) or receive (RX) mode.  
Serial data from the controller is used to generate a FSK-  
modulated 50 to 300 kHz carrier on the line in the TX mode.  
In the RX mode line signal passes through the coupling  
transformer into the PLL-based receiver. The recreated seri-  
al bit stream drives the controller.  
With the IC in the TX mode (pin 5 a logic high), baseband  
data to 5 kHz drive the modulator’s Data In pin to generate  
a switched 0.978I/1.022I control current to drive the low TC,  
TL/H/6750–2  
Top View  
g
triangle-wave, current-controlled oscillator to 2.2% devia-  
tion. The tri-wave passes through a differential attenuator  
and sine shaper which deliver a current sinusoid through an  
automatic level control (ALC) circuit to the gain of 200 cur-  
rent output amplifier. Drive current from the Carrier I/O de-  
Order Number LM1893N  
See NS Package Number N18A  
Small Outline & Dual-In-Line Package  
velops a voltage swing on T ’s (Figure 4) resonant tank  
1
proportional to line impedance, then passes through the  
step-down transformer and coupling capacitor C onto the  
C
line. Progressively smaller line impedances cause reduced  
signal swing, but never clipping-thus avoiding potential radio  
frequency interference. When large line impedances threat-  
en to allow excessive output swing on pin 10, the ALC  
shunts current away from the output amplifier, holding the  
voltage swing constant and within the amp’s compliance  
limit. The amplifier is stable with a load of any magnitude or  
phase angle.  
In the RX mode (pin 5 a logic low), the TX sections on the  
chip are disabled. Carrier signal, broad-band noise, transient  
spikes, and power line component impinge of the receiver’s  
TL/H/675041  
input highpass filter, made up of C and T , and the tank  
1
C
Top View  
bandpass filter. In-band carrier signal, band-limited noise,  
heavily attenuated line frequency component, and attenuat-  
ed transient energy pass through to produce voltage swing  
on the tank, swinging about the positive supply to drive the  
Carrier I/O receiver input. The balanced Norton-input limiter  
amplifier removes DC offsets, attenuates line frequency,  
performs as a bandpass filter, and limits the signal to drive  
the PLL phase detector differentially. The differential de-  
modulated output signal from the phase detector, contain-  
ing AC and DC data signal, noise, system DC offsets, and a  
large twice-the-carrier-frequency component, passes  
through a 3-stage RC lowpass filter to drive the offset can-  
cel circuit differentially. The offset cancelling circuit works  
Order Number LM2893M or LM2893N  
See NS Package Number M20B or N20A  
FIGURE 2. Connection Diagrams  
g
by insuring that the (fixed) 50 mV signal delivered to the  
data squaring (‘‘slicing’’) comparator is centered around the  
0 mV comparator switch point. Whenever the comparator  
signal plus DC offset and noise moves outside the carefully  
g
matched 50 mV voltage ‘‘window’’ of the offset cancel  
circuit, it adjusts its DC correction voltage in series with the  
differential signal to force the signal back into the window.  
g
While the signal is within the 50 mV window, the DC offset  
is stored on capacitor C . By grace of the highly non-linear  
M
offset hold capacitor charging during offset cancelling, the  
DC cancellation is done much more quickly than with an AC  
coupling capacitor normally used in place of the offset can-  
cel circuit. Since impulse noise spikes normally ring the sig-  
nal symmetrically around 0 V, the fully bilateral offset cancel  
topology affords excellent noise rejection. The switched cur-  
rent output of the comparator drives the impulse noise filter  
integrator capacitor that rejects all data pulses of less than  
the integrator charge time. Noise appears as duty-cycle jitter  
at the open collector serial data output.  
TL/H/6750–3  
FIGURE 3. The block diagram of a carrier-current  
system using the Bi-Line chip to interface digital  
controllers via the power line  
*Unless otherwise noted, all pin references refer to LM1893, but hold true  
for equivalent LM2893 pin.  
6
Application Information (Continued)  
7
Application Information (Continued)  
Recommended  
Value  
Effect of making the component value:  
Smaller Larger  
Ý
Purpose  
Notes  
g
2 k pot and 5.6 k fixed R.  
k
7.6 k not recommended. Poor F TC with 5.6 k R .  
O O  
C
R
560 pF  
6.2 kX  
Together, C and R Increases F  
O
Decreases F  
5% NPO ceramic. Use low TC  
O
O
O
O
O
set ICO F  
.
O
Increases F  
O
k
5.6 k not recommended.  
Decreases F  
O
l
C
R
0.047 mF  
3.3 kX  
PLL loop filter pole  
PLL loop filter zero  
Less noise immune, higher More noise immune, lower Depending on R value and  
F
F
f
PLL less stable, allows  
, more PLL stability.  
DATA  
f , less PLL stability.  
DATA  
PLL more stable, allows  
F , PLL unstable with large  
O
C . See Apps. Info. C  
F F  
F
less C . Less ringing.  
F
more C . More ringing.  
F
and R values not critical.  
F
t
250 V non-polar. Use 2C  
C
on hot and neutral for max.  
line isolation, safety.  
C
C
0.22 mF  
Couples F to line,  
C
Low TX line amplitude.  
and T low-pass Less 60 Hz T current.  
Drives lower line Z.  
O
More 60 Hz T current.  
1
More stored charge.  
C
1
attenuates 60 Hz.  
1
Less stored charge.  
g
Tank F down or decrease 100 V nonpolar, low TC, 10%  
O
C
0.033 mF  
Tank matches line Z, Tank F up or increase  
O
L of T for constant F  
Q
1
bandpass filters,  
isolates from line,  
recommended and attenuates  
.
L of T for constant F .  
O
Larger L: lower F or  
O
High large-signal Q needed.  
Optimize for low F line  
1
O
Smaller L: higher F or  
1
T
Use  
O
O
increase C ; decreased F decrease C ; increased F pull with control of F TC  
C O C O O  
XFMR  
transients.  
line pull.  
Noise spikes turn ALC off. Slower ALC response.  
Less stable ALC. More stable ALC.  
line pull.  
and Q.  
C
A
R
A
0.1 mF  
10 kX  
ALC pole  
ALC zero  
R
A
optional. ALC stable  
t
for C 100 pF.  
A
C
L
0.047 mF  
Limiter 50 kHz pole, Higher pole F, more 60 Hz Lower pole F, less 60 Hz  
reject, more noise BW.  
Any reasonably low TC cap.  
300 pF guarantees stability.  
60 Hz rejection.  
reject. F attenuation?  
O
g
C
M
0.47 mF  
Holds RX path V  
Less noise immune, shorter More noise immune, longer Low leakage 20% cap.  
OS  
V
OS  
sition, shorter preamble. sition, longer preamble.  
hold, faster V aqui- hold, slower V aqui- Scale with f  
V
.
OS OS DATA  
OS  
C
0.047 mF  
Rejects short pulses Less impulse reject, less More impulse reject, more C charge time (/2 bit nom.  
I
Must be 1 bit worst-case.  
I
k
like impulse noise.  
Open-col. pull-up  
5.6 V Zener bias  
delay, more pulse jitter.  
delay, less pulse jitter.  
t
R 1.5 kX on 5.6 V  
C
R
R
10 kX  
12 kX  
Less available sink I.  
Less available source I.  
C
k
k
30 mA recommended.  
(Chip power-up needs 5.6 V)  
Larger shunt current,  
more chip dissipation.  
Smaller shunt current,  
less Va current draw.  
1
I
Z
Z
t
k
Z
44 V BV  
60 V peak  
Transient clamp  
Z
failure, higher series  
Z costly, lower series  
T
Recommend Zener rated  
t
for 500 W for 1 ms.  
T
T
R-excess peak V, Zener  
and chip damage,  
less ruggedness.  
R gives enhanced  
transient clamp,  
more ruggedness.  
Excessive TX attenuation. Carbon comp. recommended.  
Costly IRF 11DQ05 or 1N5819  
R
D
4.7 X  
t
Transient I limit  
Over-drive Clamp  
Damage Z , pull up Va  
.
T
T
T
Failure on Transient  
44V BV  
b
Inadequate turn-off speed. Boost optional. Q F( 3 dB)  
B
R
Q
180 X  
Power NPN  
1.1 X  
Base bleed  
Boost gain device  
Current setting R  
Faster, lower THD I  
.
B
O
l
l
Excessive T and V  
.
More rugged, but costly.  
.
of 200 MHz. R  
B
24 Ohm.  
B
J
SAT  
More I , need higher h  
e
a
R
G
[
]
)/R mApp.  
G
R
G
.
Less I , lower min. h  
O
I
70 (10  
O
fe  
fe  
O
t
C
47 mF  
Supply bypass  
Transients destroy chip.  
Less supply spike.  
Va never over abs. max.  
B
A
Z
5.1V  
Stop ALC charge  
in RX mode  
Excess ALC  
current flow  
ALC RX charging  
not inhibited over T  
Z optional - 5.1V  
A
20% low leakage type  
g
J
FIGURE 5. A quick explanation of the external component function using the circuit ofFigure 4. Values given are for Va  
e
e
e
360 Baud (180 Hz), using a 115 V 60 Hz power line  
18 V, F  
125 kHz, f  
DATA  
O
Component Selection  
Assuming the circuit of Figure 4 is used with something oth-  
er than the nominal 125 kHz carrier frequency, 180 Hz data  
rate, 18V supply voltage, etcetera, the component values  
listed in Figure 5 will need changing. This section will help  
direct the CCT designer in finding the required component  
values with emphasis placed on look-up tables and charts. It  
is assumed that the designer has selected values for carrier  
ance considerations only, are: 1) the higher the F the bet-  
O
ter, 2) the lower the maximum data rate the better, and 3)  
the more time and frequency filtering the better.  
Use Figure 5 as a quick reference to the external compo-  
nent function.  
THE TRANSMITTER  
center frequency, F ; data rate, f  
; supply voltage, Va  
;
power line voltage, V ; and power line frequency, F . If one  
O
DATA  
C
O
L
L
Central to chip operation is the low TC of F emitter-cou-  
O
or more of those parameters is not defined, one may read  
the data sheet and make an educated guess.  
pled oscillator. With proper C , the F of the 2V  
BE  
ampli-  
O
O
tude triangle-wave oscillator output may vary from near DC  
to above 300 kHz. While C may have any value, C should  
Maxims to keep in mind, based on CCT electrical perform-  
O
O
8
Component Selection (Continued)  
be made above 10 pF so that parasitic capacitance is not  
dominant. Excessive or unbalanced common-mode-to-  
ground capacitance should be avoided. A low temperature  
T
1
At this point, the CCT system designer may choose to use  
one of the recommended transformers or to design custom  
T . Consult ‘‘The Coupling Transformer’’ section to help  
k
coefficient (TC) of capacitance ( 100 PPM/ C), such as a  
monolithic NPO ceramic multilayer type, preserves low TC  
§
1
with the design of T if a new or boost-capable transformer  
1
is needed. The recommended 125 kHz transformer func-  
of F . Figure 6 finds a C value given F .  
O
O
O
tions with an I of up to 600 mApp.  
O
R
O
It is recommended that CCT systems use the recommended  
Resistor R is used by the IC to generate a V /R related  
BE  
O
transformers, described in Figure 7, for T . The 3 transform-  
1
ers are optimized for use in the ranges of 50100 kHz, 100–  
current that is multiplied by 2 to produce the 200 mA ICO  
control current that sets F . The control current TC ‘‘bucks’’  
O
the V related tri-wave amplitude across C to effect a low  
200 kHz, and 200400 kHz with unloaded Q’s (Q ) of about  
U
BE  
O
35, and loaded Q’s (Q ) of about 12. Three secondary taps  
L
TC of F . Vary R to trim F , within limits. Raising F more  
O
O
O
O
are supplied with nominal 7.07, 10, and 14.1 turns ratios (N)  
to drive industrial and residential power line impedances of  
3.5, 7, and 14X respectively. All are inexpensive, all have  
the same pin-outs for easy exchange in a PC board, and all  
are small - on the order of 10 mm diameter at the base.  
than 20% above its untrimmed value by means of decreas-  
ing R more than 20% is not recommended. Low R , and  
so high control current, risks ICO saturation and poor TC  
O
O
under worst-case conditions. Raising R reduces the de-  
O
modulated signal amplitude from the phase detector; raising  
R
by more than a factor of 2 (1 octave) is not recommended.  
O
C
Q
Since lower TC pots are relatively costly, it is recommended  
k
Tank resonant frequency F must be correct to allow pas-  
Q
sage of transmitter signal to the line. Use Figure 8 to find  
that R be made up of a 5.6 k fixed ( 100 PPM/ C) resistor  
§
O
k
with a 2 kX ( 250 PPM/ C) series pot.  
§
C
ming slug. The inductance of T has a TC of 150 PPM/ C  
’s value. Trimming F to equal F is done with T ’s trim-  
Q Q O 1  
a
which may be cancelled by using a 150 PPM/ C cap such  
§
C
and R  
A
1
A
b
as polystyrene. Since circulating current in the tank is (/4  
§
Components C and R control the dynamic characteristics  
A
A
of the transmitter output envelope. Their values are not crit-  
ical. Use the values given in Figure 5. C and R are func-  
A
, C should have a low series resistance (a 1 X series  
RMS  
Q
A
A
resistance is too much). Polypropelene caps are excellent,  
‘‘orange drop’’ mylars are adequate, while many other my-  
lars are inadequate. A 100V rating is needed for transient  
protection.  
tions of loaded T tank Q, R , f  
, and line impulse  
DATA  
noise. Any changes made in C and R should be made  
1
O
A
A
based on empirical measurements of a CCT on the line.  
Roughly, C acts as an ALC pole and R an ALC zero.  
A
A
TL/H/675010  
TL/H/6750–5  
FIGURE 8. Find C ’s value given F  
O
FIGURE 6. Find C ’s value knowing F  
O
O
O
Bottom View  
TL/H/6750–7  
TL/H/6750–8  
TL/H/6750–9  
TL/H/6750–6  
125 kHz  
Toko 707VX-A042YUK  
50 kHz  
Toko 707VX-A043YUK  
300 kHz  
Toko 161XN-A207YUK  
FIGURE 7. The recommended T transformers, available through:  
1
Toko America, 1250 Feehanville Drive, Mount Prospect, IL, 60056, (312) 297-0070  
9
Component Selection (Continued)  
neous power of greater than 1 kW has been measured us-  
ing the recommended transformers). For self protection, the  
Carrier I/O has an internal 44V voltage clamp with a 20X  
series resistance. A parallel low impedance 44V external  
transient suppression diode will then conduct the lion’s  
share of any current when transients force the Carrier I/O to  
a high voltage.  
C
C
Capacitor C ’s primary function is to block the power line  
C
voltage from T ’s line-side winding. Also, C and T ’s line-  
1
C
1
side winding comprise a LC highpass filter. The self-induc-  
tance of T is far too low to support a direct line connection.  
1
C
C
must have a low enough impedance at F to allow T to  
O 1  
drive transmitted energy onto the line. To drive a 14X power  
line, the impedance of C should be below 14X.  
C
Use Figure 9 to find the reactive impedance of C to check  
C
that it is less than the line impedance. Then checkFigure 10  
to see that the power line current is small enough to keep  
T
1
well out of saturation; the recommended transformers  
can withstand a 10 Amp-turn magnetizing force (1 Amp  
through the worst-case 10 turn line-side winding).  
Caution is required when choosing C to avoid series reso-  
C
nance of the series combination of C , the transformer in-  
C
ductance, and the reflected tank impedance. The low resist-  
ance of the network under series resonance will load the  
line, possibly decreasing range. For your particular line cou-  
pling circuit, measure for series resonance using some ex-  
pected line impedance load.  
TL/H/675012  
FIGURE 10. The AC line-induced current passed by C  
C
R
B
This base-bleed resistor turns Q off quickly - important  
B
since the amplifier output swing is about 200V/ms. An R  
B
below about 24X will conduct excessive current and over-  
load the chip amplifier and is not recommended.  
TL/H/675013  
FIGURE 11. Output amplifier current and required min.  
versus gain-setting resistor R  
Q
B
h
fe  
G
TL/H/675011  
FIGURE 9. C ’s impedance should be,  
C
as a rule-of-thumb, smaller than the lowest  
expected line impedance  
R
G
This resistor, in parallel with the internal 10X resistor, fixes  
the current gain of the output amplifier, and so the output  
current amplitude. Figure 11 gives output current and mini-  
TL/H/675014  
FIGURE 12. Boost transistor power dissipation versus  
amplifier output current  
mum AC current gain h for Q when R is used to boost  
fe  
B
G
output current.  
Z
must be used unless some precaution is taken to protect  
the Carrier I/O pin from line transients or transients caused  
T
Q
B
The boost gain transistor Q must be fast. Double-diffused  
B
devices with 50 MHz F ’s work, slower transistors (epi-base  
when stored line energy in C is discharged by the random  
C
phase of power line connection and disconnection. Worst  
T
types) do not preserve a sinusoidal waveform when F is  
case, C may discharge a full peak-to-peak line voltage into  
C
the tuned circuit. Another way to reduce the need for Z is  
T
O
high or will cause the output amp. to oscillate. Q must have  
B
a certain minimum h for given boost levels, as shown in  
fe  
Figure 11. Figure 12 shows the power Q must dissipate  
by placing another magnetic circuit in the signal path that  
relies on a high, but easily saturated, permeability to couple  
a primary and secondary winding - a toroidal transformer for  
B
e
(R  
R ) must be 60V or greater and Q must have adequate  
continuously operating with a shorted output. BV  
CER  
example. Toroids cost more than Z .  
T
B
B
SOA for transient survival.  
Use an avalanche diode designed specifically for transient  
suppression Ð they have orders of magnitude higher pulse  
Z
T
Unfortunately, potentially damaging transient energy passes  
through transformer T onto the Carrier I/O pin (instanta-  
1
10  
Component Selection (Continued)  
power capability than standard avalanche diodes rated for  
equal DC dissipation. Metal oxide varistors have not proven  
useful because of their inferior clamping coefficient and are  
not recommended. Specifications for an example minimum  
diode are given in Figure 13.  
differential inputs of the Norton amp. equally, while the sin-  
gle-ended input signal swings only the positive input. Overall  
PSRR consists of the input CMRR (set by the input stage  
component matching) and the ripple-frequency attenuation  
of the input amplifier bandpass response that passes carrier  
frequency but stops low frequencies. A typical 1% resistor  
and 1 mV n-p-n mirror offsets give 26 dB of attenuation, the  
bandpass gives 54 dB 120 Hz attenuation, for an overall 80  
dB PSRR to allow tens of volts of ripple before impacting  
ultimate sensitivity.  
@
4449V 1 mA  
Breakdown Voltage  
@
Maximum Leakage  
1mA 40V  
@
300 pF BV  
Capacitance  
@
64.5V 7.8A  
Maximum Clamp Voltage  
Peak Non-Repetitive Pulse Power  
(REA Standard Exponential Pulse)  
Surge Current  
10 kW for 1 ms  
C
C
A value was chosen earlier. Knowing T ’s secondary induc-  
1
tance allows a check of LC line attenuation using Figure 14.  
70A for 1/120s  
FIGURE 13. Key specifications for a recommended  
transient suppressor Z available from General  
T
Semiconductor, 2001 West Tenth Place, Tempe, AZ  
85281, 602968-3101, part no. SA40A  
C
L
The Norton input limiter amplifier has a bandpass filter for  
enhanced receiver selectivity, noise immunity, and line fre-  
e
quency rejection. The nominal response curve for F  
50  
kHz is shown inFigure 15. The 300 kHz pole is fixed. The 50  
kHz pole is set by C ’s value. After C is found, the resulting  
O
R
T
L
L
R
acts as a voltage divider with Z , absorbing transient  
T
energy that attempts to pull the Carrier Input pin above 44V.  
Make the resistor a carbon composition 1/4W. When exper-  
T
line frequency attenuation is found for the bandpass filter.  
Use Figure 15 to find a C value given for F . The approxi-  
O
L
iments discharging C charged to the peak-to-peak 620V  
C
AC thru a 1X power line were carried out, film resistors blew  
open-circuit.  
mate line frequency attenuation of the bandpass filter may  
then be found in Figure 16. Figure 15 returns a value for C  
33% larger than nominal, giving a low frequency pole 33%  
low to allow for component tolerances.  
L
D
T
This Schottky diode is placed in parallel with the CCT chip’s  
substrate diode to pass the majority of the current drawn  
from ground when the Carrier Input or Carrier Output is  
pulled below ground by a larger-than-twice-the supply-swing  
on the tank. Note that Z is in parallel with the substrate  
T
diode, but is ineffective due to its high forward voltage drop  
and high diffusion capacitance caused by its low forward  
speed. Tests proved that a 1N5818 kept a receive-path  
functional with a 20X boost transmitter with a 7:1 transform-  
g
er attempted to swing the receiver’s Carrier I/O to 100V  
TL/H/675015  
(300 mA peak ground current in the receiver). Without D ,  
T
the receiver momentarily stops functioning at a 100 times  
lower ground current.  
FIGURE 14. The 60 Hz line rejection of the highpass  
filter made up of C and T ’s line-side winding  
C
1
(neglecting capacitive coupling)  
This diode is not needed if the Carrier I/O never swings  
below ground. If your CCT systems all run on the same  
regulated voltage with all matched transformers and turns  
ratios, it is not needed. Otherwise, it is.  
THE RECEIVER  
The receiver and transmitter share components C , T , C ,  
Q
C
1
R , Z , C , R , and peripheral supply and bias components  
T
T
O
O
that are not in need of change for RX mode operation. Val-  
ues for the balance of the components are now found.  
TL/H/675016  
Line-Frequency Rejection  
To use the ultimate sensitivity of the device, fully 110 dB of  
115 V, 60 Hz attenuation is required between the line and  
the limiter amplifier output. Using the circuit topology of Fig-  
ure 4, the combined attenuation of the C /T highpass, the  
1
C
tuned transformer, and the bandpass filter attenuation of  
the limiter amplifier give far more line rejection than the  
above-stated minimum. However, if some other CCT line  
coupling circuit is used, line rejection will become important  
to the system designer.  
Receiver input power supply rejection (PSRR) and common-  
mode rejection (CMRR) are one-in-the-same using the sup-  
ply-referenced signal input of Figure 4. Ripple swings both  
TL/H/675017  
FIGURE 15. Given F , C is found. Also shown is the  
L
input amplifier’s small signal amplitude response  
O
11  
Component Selection (Continued)  
obvious way out is to then reduce the unfiltered loop band-  
width. That bandwidth is approximately proportional to the  
value of C . For a fixed F , unfiltered loop bandwidth reduc-  
C
and R  
F
F
These phase-locked loop (PLL) loop filter components re-  
move some of the noise and most of the 2F components  
O
present in the demodulated differential output voltage signal  
from the phase detector. They affect the PLL capture range,  
loop bandwidth, damping, and capture time. Because the  
PLL has an inherent loop pole due to the integrator action of  
O
O
tion requires a larger C and larger control current. With this  
O
chip, changing the control current is not allowed. So one is  
forced to choose a C /R combination with some minimum  
F
F
g
capture range, say 20%, that is within some guardband  
from the point of loop instability. Happily, impulse noise  
tends to last only fractions of a millisecond so that the lack  
of low bandwidth loop response with low data rates is not a  
heavy penalty. As long as there is adequate capture range,  
the impulse noise filter performs admirably. Note that reduc-  
the ICO (via C ), the loop pole set by C and the zero set by  
R
O
F
gives the loop filter a classical 2nd-order response.  
F
ing F will reduce the no-filter loop bandwidth, and indeed  
O
the maximum data rate falls below the limit set by the RC  
lowpass filter as F falls below 100 kHz (Figure 19).  
O
The tuned transformer characteristics will affect the demod-  
ulated data waveform more than C and R at low data  
F
F
rates. Tank Q and off-tuning will affect overshoot during the  
FSK frequency steps. This is a property of tuned circuits.  
The maximum data rate of Figure 19 is measured from the  
receiver input to the Data Out and does not include the data  
TL/H/675018  
FIGURE 16. The Norton-input limiter amplifier bandpass  
filter line-frequency signal attenuation given C  
L
bandwidth reducing effects of T .  
I
C
M
Capacitor C stores a voltage corresponding to a correction  
M
factor required to cancel the phase detector differential out-  
put DC offsets. The stored voltage is ±/6 of the DC offset  
plus some bias level of about 2.2 V. A large C value in-  
M
creases the time required to bias-up the receive path at the  
beginning of transmission. A large C does filter well and  
M
store its bias voltage long. Because of the initial random  
charge of C , the receiver must be given a data transition to  
M
charge to the proper bias voltage. Therefore, reducing C ’s  
M
TL/H/675019  
FIGURE 17. Find C given F .Figure 19  
F
O
gives the maximum data rate  
value to one that may be charged in less than 2 bit-times will  
not save biasing time and is not recommended.  
No C and R give the most stable PLL with the fastest  
F
F
response. Large C ’s with a too-small R cause PLL loop  
F
F
instability leading to poor capture range and poor step re-  
sponse or oscillation.  
Calculation of C and R is quite difficult, involving not only  
F
F
the 2nd-order loop step response, but also the PLL non-  
dominant poles, the tuned transformer stepped-frequency  
response, and the RC lowpass step response (for data rates  
approaching 1 kHz). C and R values are best found em-  
F
F
pirically. Tolerance is not critical. Component values are se-  
lected to give the best possible impulse noise rejection  
TL/H/675020  
FIGURE 18. Find R given F with F  
DATA  
a parameter  
F
O
g
while preserving a 20% capture range and wide stability  
margin.Figures 17 and18 give C and R values versus F  
F
,
O
F
kk  
where ‘‘f  
MAX DATA RATE’’ means that f  
DATA  
DATA  
should be less than the maximum data rate, in kHz, from  
Figure 19 divided by 10.  
Note that C and R are a function of data rate only for high  
F
F
data rates and are not plotted against data rate - as one  
might expect. The reason for this is important to understand  
if the CCT system designer wishes to find C and R empiri-  
F
F
cally. Data signal is, loosely speaking, passed through the  
PLL loop and is therefore potentially attenuated if the loop  
bandwidth is on the order of the 3rd harmonic of the data  
rate, or less. Overall loop bandwidth is held as low as possi-  
ble for maximum noise rejection while passing the data.  
Loop bandwidth is roughly proportional to the geometric  
mean of the unfiltered loop bandwidth and the filter pole set  
TL/H/675021  
FIGURE 19. The maximum data rate versus F using  
O
loop filter components optimized for max. noise  
g
performance while retaining a min. 20% capture  
range (large signal)  
Use Figure 20 to find C ’s value knowing f  
M
, assuming  
DATA  
by C . Therefore, C is related to data rate. Unfortunately,  
F
F
the loop capture range falls to critically low values when  
the standard 2 bit receive charge time is desired. The cap.  
value and TC are not critical, but the capacitor should have  
low leakage.  
large enough values of C are used to reduce loop band-  
F
width down to the 100’s of Hz range, for low data rates. The  
12  
Component Selection (Continued)  
Z
A
The 5.1V silicon zener diode Z is required when a short  
A
RX-to-TX switch-over time is needed at the same time that  
the chip is operating in the RX mode with a pin 10 input  
signal swing approaching or exceeding twice the supply  
voltage. Predominant causes of these large swings imping-  
ing on the RX input are: 1) a transmitter’s supply voltage  
higher than the receiver’s supply voltage, 2) a TX and RX  
pair that are electrically close, or, 3) a higher RX T step-up  
1
turns ratio than the TX T step-down ratio.  
1
TL/H/675022  
Normally, when in the RX mode with small incoming signal  
on pin 10, the ALC remains off with pin 7 at a 6V  
FIGURE 20. Size C assuming a 2 bit-time  
M
receive bias time  
b
mode may then be selected with 6V on C allowing 100%  
(V  
2V ) bias voltage. C is then charged to 6V. TX  
BE A  
Z
A
C
I
TX power to pump T ’s tuned circuit, and so the AC line,  
1
quickly for fast RX-to-TX switch time. As TX output swing  
The impulse noise filter integrator capacitor C is used to  
I
disallow the passage of any pulse shorter than the integra-  
increases so that pin 10 swings below V  
ALC  
(4.7V typically),  
tor charge time. That charge time, set to a nominal (/2 bit  
g
that ALC activates to charge C to about 6.6V to reduce TX  
A
output drive. However, if in the RX mode pin 10 ever swings  
time, is the time required for a 50 mA charge current to  
swing C over a 2 V range. Charge time under worst case  
I
BE  
conditions must never be greater than a bit time since no  
below V  
, C will charge to above 6.6V. Now, when the  
A
ALC  
TX mode is selected with C at 6.6V, somewhere from 0 to  
A
g
signal could then pass. Using a 10% capacitor, full junc-  
tion temperature range, and full specified current range, a  
100% TX output drive is available to pump T ’s tuned circuit  
1
resulting in a slower rising line signal - effectively reducing  
the RX-to-TX switch time.  
maximum nominal charge time of (/2 bit is recommended.  
Figure 21 gives C versus data rate under those conditions.  
I
Use a 5.1V Z driven by a 0 to 0.8V logic low signal to  
A
R
C
guarantee over-temp. operation. R must be in series with  
A
Z
R
to limit current flow and should never fall below 1 kX. If  
is less than 1 kX, then put a 2 kX resistor in series with  
Z . Logic high voltages above 10V will cause current flow  
The collector pull-up resistor is sized to supply adequate  
pull-up current drive and speed while preserving adequate  
output low current drive.  
A
A
A
into pin 7 that must be limited to 1 mA (with R or a  
A
series R).  
Breadboarding Tips  
During CCT system evaluation, some techniques listed be-  
low will simplify certain measurements.  
Ð Use caution when working on this circuit - dangerous  
line voltages may be present.  
Ð When evaluating PLL operation, offset cancel circuit op-  
eration, and loop filter values, use the filter of Figure 22  
to view the demodulated signal minus the 2F and noise  
O
TL/H/675024  
components. This filter models the RC lowpass filter on  
chip.  
FIGURE 21. Impulse noise filter cap. C versus F  
I
where the charge time is (/2 bit time  
DATA  
TL/H/675025  
FIGURE 22. Circuit to view the differential demodulated data signal, minus the noise and 2F components,  
O
conveniently with a single-ended gain-of-one output  
13  
Breadboarding Tips (Continued)  
Ð When evaluating CCT system noise performance on a  
real power line, it is desirable to vary the signal ampli-  
tude to the receiver. This is not easy. An in-line line-  
proof L-pad is fine except that the line impedance is un-  
known and variable and so the L-pad will rarely match.  
Instead, the power output of a chip transmitter may be  
controlled using the circuit of Figure 23. This circuit con-  
trols the ALC.  
representing an average line impedance may be connected  
to the line side of T . The circuit of Figure 23 should then be  
1
used to defeat the leveling effect of the ALC.  
Ð It is sometimes desirable to place impulse noise on the  
line. A simple light dimmer with a 100 W light bulb load  
produces representative impulse noise.  
Ð Do not allow peak currents of over 1 A through the 5.6 V  
Zener. In other words, don’t short charged capacitors  
into this low-impedance device. Take care not to mo-  
mentarily short pins 10 and 11 - chip damage may result.  
TL/H/675026  
FIGURE 23. A means of transmitter output amplitude  
control is shown  
Ð Figure 24 shows some typical signals beginning with se-  
rial data transmitted to received signal.  
Thermal Considerations  
It is desirable to place the largest possible signal on the  
power line for maximum range, limited only by the chip pow-  
er dissipation and maximum junction temperature T . The  
Tuning Procedure  
This procedure applies to circuits similar toFigure 4 LM1893  
or LM2893 circuit.  
J
falling output power at elevated T allows a more optimal  
J
power output - high power at low T and lower power at high  
J
for chip self-protection. However, it is still possible to  
T
exceed the maximum T within the specified ambient tem-  
First, trim F by putting the chip in the TX mode, setting a  
O
logical high data input, and measuring the TX high frequen-  
J
J
e
perature limit (T  
85 C) under worst case conditions of  
cy, 1.022 F , on the Carrier I/O using these steps:  
O
§
A
100% TX duty cyle, high supply, shorted load, poor PC  
board layout (with small copper foil area), and an above  
nominal current part. Under those conditions, a part may  
e
dissipate 2140 mW, reaching a T  
mittedly a rare occurrence). Proper system design includes  
1. Take pin 17 to a logic low.  
2. Take pin 5 to a logic high.  
3. Place a counter on pin 10.  
170 C worst-case (ad-  
§
J
e
4. Adjust R on pin 18 for F  
O
1.022F .  
O
the measurement or calculation of T max. to guarantee  
J
Second, the line transformer is tuned. The chip is placed in  
the TX mode, a resistive line load is connected to disable  
the ALC by reducing tank voltage swing below its limit. FSK  
data is then passed through the tank so that the tank enve-  
lope may be adjusted for equal amplitude for high and low  
data frequency.  
function under worst-case operation. Like all devices with  
failure modes modeled by the Arrhenius model, the high  
chip reliability is further enhanced by keeping the die tem-  
perature mercifully below the absolute maximum rating.  
A direct method of measuring operating junction tempera-  
voltage on pin 18, which is al-  
ture is to measure the V  
BE  
ways available under all operating modes. The graph of Fig-  
ure 25 may be used to find T , knowing V at the operating  
1. Take pin 5 to a logic high.  
2. Place a logic-level square wave at or below the receiver’s  
maximum data rate on pin 17.  
J
BE  
e
e
by powering up a chip (in RX mode) that has been dissipat-  
point in question and V at T  
BE  
T
J
25 C. V is found  
BE  
§
A
3. Temporarily place a 330 X resistor across the tank.  
4. Place a scope on pin 10.  
ing zero power at some T for some time and measuring  
V
A
in less than 1 s (for better than 5 C accuracy).  
§
5. Adjust the transformer slug for the least envelope modu-  
lation.  
BE  
Alternately, T may be calculated using:  
J
e
a
i
In lieu of the 330 X resistive load, T may be coupled to the  
T
J
T
A
P
JA D  
(1)  
1
power line to better simulate actual load and tank pull condi-  
tions during tank tuning. Alternatively, a passive network  
where i is 75 C/W for the plastic (N) package using a  
socket. That i value is for a high confidence level; nomi-  
JA  
§
JA  
TL/H/675023  
FIGURE 24. Oscillogram revealing signals at several important nodes under weak signal (0.5 mV  
) conditions with  
RMS  
SCR spikes on an otherwise quiet 115 V, 60 Hz power line. The signals are: 1) transmitted data, 2) RX carrier on the  
tuned transformer, 3) demodulated signal from the PLL after passing thru circuit ofFigure 22, 4) signal after RC  
lowpass, 5) data at impulse noise filter integrator, and 6) received data. Horizontal scale is 10 ms per div.  
14  
g
mended C and R (47 nF and 6.2 kX) with a 4.4% DF  
(a  
F
F
O
Thermal Considerations (Continued)  
g
to take less than 50 cycles of F . That is a 0.40 ms delay  
100 mV DC offset on C and R ), lock was measured  
F F  
nal i for an N package is 60 C/W, lower with good PC  
§
board layout. Since P is a relatively strong function of T ,  
JA  
O
D
J
(proportional to 1/F ).  
O
an iterative solution process starting with an initial guess for  
is used. With the estimated T , find the total supply cur-  
rent found in the typical performance characteristics.  
Acquisition is incomplete until the second order PLL loop  
settles. For the above-mentioned C and R , the loop natu-  
T
J
J
F
F
and damping factor are found to be  
ral frequency  
2.3 kHz and 1.0 respectively. Settling to within 25 mV of  
F
N
g
the 100 mV DC offset change requires 2.7 periods of F  
g
or 1.2 ms (a function of C and R ).  
,
N
F
F
Third, the RC lowpass filter introduces a 0.12 ms delay.  
e
ing on the polarity of F . Borderline data squaring with zero  
g
Fourth, C must charge up to (±/6)100  
83 mV depend-  
M
O
noise immunity is possible with only (±/6) 50 mV of charg-  
g
ing. C charge current is an asymptotic function approxi-  
M
mated by assuming a 50 mA charge current and the full 83  
mV charge voltage. C charge time is then 1.7 ms (propor-  
M
TL/H/675027  
tional to 1/f  
).  
DATA  
FIGURE 25. T may be found by using the temperature  
J
Fifth, the impulse noise filter adds a (/2 bit-time delay. Total  
is 3.9 ms plus (/2 bit-time for a total of 1.9 bit-times at  
360 Baud.  
coefficient of pin 18 V if V is known at 25 C  
BE  
§
BE  
T
TR  
Transmit-To-Receive  
Switch-Over Time  
Receive-To-Transmit  
Switch-Over Time  
An important figure-of-merit for a half-duplex CCT link, af-  
.
fecting effective data rate, is the TX-to-RX switch time T  
TR  
Using the recommended component values gives this part a  
Assume the chip has been in the RX mode and the TX  
mode is now selected. In less than 10 ms, full output current  
is exponentially building tank swing. 50% of full swing is  
achieved in less than 10 cycles - or under 80 ms at 125 kHz.  
In the same 10 ms that the output amp went on, the phase  
detector and loop filter are disconnected and the modulator  
input is enabled. FSK modulation is produced in 10 ms after  
switching to TX mode.  
e
[
]
) over a wide  
nominal 2 bit-time (1 bit time  
range of operating conditions, where the receiver requires 1  
data transition. T cannot be decreased significantly but  
1/ 2f  
DATA  
TR  
does increase as noise filtering, especially via C , is in-  
M
creased. Impulse noise at switch, signals near the limiting  
sensitivity, poor F match between receiver and transmitter  
O
because of poor trim or worst-case conditions, and the sta-  
tistical nature of PLL signal acquisition may all contribute to  
Power Line Impedance  
Irrespective of how wide the limits on power line impedance  
increase T to possibly 4 bit-times.  
TR  
T
is lower when a pair of LM1893’s handshake rapidly.  
TR  
The receiver was designed to ‘‘remember’’ the RX-mode  
DC operating points on C and C while in the TX mode.  
Z
are placed, there are no guarantees. However, since the  
CCT design requires an estimate of the lowest expected line  
L
M
F
impedance Z encountered for the most efficient transmit-  
LN  
ter-to-line coupling, line impedance should be measured  
Under noisy worst case conditions, C will discharge to the  
M
point of false operation after 35 bit-times in the TX mode  
and Z limits fixed to a given confidence level. Reasonable  
L
values for T turns ratio, loaded Q, and tank resonant fre-  
1
quency pull F may be found to enable a CCT system de-  
Q
e
(1400 bit times with no noise and a nominal part, f  
DATA  
is about 0.8 ms (proportional to the selected  
180 Hz). T  
TR  
F
) plus (/2 bit-time.  
O
sign that functions with the overwhelming majority of power  
lines.  
The major components of T  
TR  
nominal 125 kHz F , 180 Hz f  
are described below for a  
, lightly-loaded tank with  
O
DATA  
A limited sampling of Z was made, during the LM1893 de-  
L
a Q of 20, and the circuit of Figure 4. The remote CCT has  
been operating in the TX mode with a 26.6 V tank swing  
PP  
and is now selected as a receiver. An incoming signal re-  
quiring the ultimate receiver sensitivity immediately is placed  
on the line.  
sign, of residential and commercial 115V 60 Hz power line.  
Data was also drawn from the research of Nicholson and  
Malack (reference 1), among others, to produce Figures 26  
and 27. All measured impedances are contained within the  
shaded portions of Figure 27. A nominal 3.5, 7.0 and 14 X  
First, the tank stored energy at the transmit frequency must  
decay to a level below the 2.8 mV swing caused by the  
PP  
Z
is used throughout the application information with a  
LN  
nominal 45 phase angle (0 is sometimes used for simplici-  
ty).  
§
§
0.14 mV  
incoming line signal containing the information  
RMS  
to be received.  
Q
V
V
1
e
e
decay time  
ln  
qF  
O
# J  
O
20  
26.6  
e
ln  
0.466 ms  
(2)  
c
q
125 000  
0.0028  
# J  
That is 0.47 ms of delay (proportional to I/F and Q).  
O
Second, the PLL must acquire the signal; it must lock and  
settle. Acquisition time is statistical and may take any length  
of time, but average acquisition time depends on the loop  
TL/H/675028  
FIGURE 26. Measured line impedance range for  
residential and commercial 115V, 60 Hz lines  
filter components C and R and the difference in center  
F
frequencies, DF , of the TX/RX pair. Using the recom-  
F
O
15  
Power Line Impedance (Continued)  
TL/H/675029  
TL/H/675030  
TL/H/675031  
e
a
jX  
FIGURE 27. Complex-plane plots of measured 115V, 60 Hz line impedance where Z  
R
L
L
L
Power Line Attenuation  
The wiring in most US buildings is a flat 3 conductor cable  
T with a stable resonant frequency, F , that is little affect-  
1 Q  
called Amerflex, BX, or Romex. All referenced line imped-  
ances refer to hot-to-neutral impedances with a grounded  
center conductor. The cable has a 100 X characteristic im-  
pedance, a 125 kHz quarter-wavelength of 600 m (250 m at  
300 kHz), and a measured 7 dB attenuation for a 50 m run  
with a 10 X termination. Generally, line loads may be treat-  
ed as lumped impedances. Instrument line cords exhibit  
about 0.7 mH and 30 pF per meter.  
ed by the de-tuning effect of the line impedance Z , and of  
L
2) building a tightly line-coupled transformer for transmitted  
carrier with loose coupling for transients, are somewhat mu-  
tually exclusive. The tradeoffs are exposed in the following  
example for the CCT designer attempting a new boost-ca-  
pable, or different core, transformer design.  
The compromises are eased by separating the TX output  
and RX input in the LM2893. An untuned TX coupling trans-  
former with only core coupling (not air-coupled solenoid  
windings) would employ a high permeability, high magnetic  
field, low loss, square saturating, toroidal core. The reso-  
nant RX path would be isolated from line-pull problems by a  
unilateral amplifier that operates at line voltages with much  
more than 110 dB of dynamic range, or by a capacitively  
coupled pulse transformer driving a unilateral amplifier and  
filter, for increased selectivity. See the LM2893-specific ap-  
plications section.  
Limited tests of CCT link range using this chip show exten-  
sive coverage while remaining on one phase of a distribu-  
tion transformer (100’s of m), with link failure often occuring  
across transformer phases or through transformers unless  
coupling networks are utilized. Total line attenuation allowed  
from full signal to limiting sensitivity is more than 70 dB.  
Typically, signal is coupled across transformer phases by  
parasitic winding capacitance, typically giving 40 dB attenu-  
ation between phased 115 V windings. Coupling capacitors  
may be installed for improved link operation across phases.  
Power factor correcting capacitor banks on industrial lines  
or filter capacitors across the power lines of some electronic  
gear short carrier signal and should be isolated with induc-  
tors. Increasing range is sometimes accomplished by elect-  
ing to install the isolating inductors (Figure 28) and coupling  
capacitors, as well as by electing to use the boost option.  
Frequency translating or time division multiplexed repeaters  
will also increase range.  
For a LM1893-style transformer application, first, choose  
the turns ratio N based on an estimated lowest Z likely  
L
encountered, Z . Figure 29 shows graphically how N af-  
LN  
fects line signal. N should be as large as possible to drive  
Z
with full signal. If T has an unloaded Q, Q , of well less  
1 U  
LN  
than 35, a guess of N somewhat high should be used and  
later checked for accuracy. The recommended transformers  
e
have secondary taps giving a choice of N 7.07, 10, and  
14.1 (nominally) for driving Z ’s of 14, 7.0, and 3.5 X re-  
LN  
a e  
e
e
35).  
spectively (at T  
25 C, V  
18V, and Q  
§
J
U
The resonating inductance of the tuned primary, L , is  
1
sought. Note that, while standard transformer design gives a  
transformer self-inductance with an impedance at operating  
frequency well above load impedance, the tuned transform-  
er requires a low L for adequate Q and minimum line pull.  
1
U
Result: relatively poor mutual coupling.  
TL/H/675040  
FIGURE 28. An isolation network to prevent: 1) noise  
from some device from polluting the AC line, and 2) to  
R
e
L
(3)  
1
2qF  
Q
O
e
It is known that resonant frequency F  
minimum bandwidth, or maximum Q, will be required to pass  
signal under full load conditions.  
F
O
and some  
Q
stop some low impedance device (measured at F )  
o
from shorting carrier signal. Component values given  
e
residential power lines  
as an example for F  
125 kHz on  
o
R
Z
O
LN Ê  
Q
Q
ll l  
l
L
e
L
(4)  
1
2q F  
Z
resistance R models all transformer losses and sets Q  
is the reflected Z , Q is the loaded Q, and parallel  
L
The Coupling Transformer  
The design arrived at for T is the result of an unhappy  
LN Ê  
l
l
LN  
.
O
Q
1
compromise - but a workable one. The goals of 1) building  
R
Z
LN Ê  
l
is found knowing that it absorbs full rated power.  
Q
ll l  
16  
The Coupling Transformer (Continued)  
Line pull DF was calculated (reference 3) for a Z magni-  
Q
L
b
tude of 14X and up with any phase angle from 90 to 90 .  
§
§
DF was 6.4% - well above the 3.3% estimate. Referring to  
Q
(11), an 11.8% bandwidth is required, forcing L to be re-  
1
duced to reduce Q. That fix was not implemented; some  
signal attenuation under worst-case drift and DF is al-  
Q
lowed. L is already so small that the 31 gauge winding  
circulating current.  
1
conducts a (/4 A  
RMS  
Line Carrier Detection  
While the addition of a carrier detection circuit (for a mute or  
squelch function) will only decrease receiver ultimate sensi-  
tivity, there is sometimes good reason to employ it to free  
the controller from watching for RX signal when no carrier is  
incoming, or to employ it to reduce the probability of line  
collisions (when multiple transmitters operate simultaneous-  
ly to cause one or more transmissions to fail). Unless the  
detector is heavily filtered or uses a high carrier amplitude  
threshold, there will be false outputs that force the controller  
to have Data Out data checking capability just as is required  
when using no carrier detector. If false triggering is mini-  
mized, the probability of line collisions is increased due to  
the inability to sense low carrier amplitudes and because of  
sense delay. The property of the LM1893 to change output  
state infrequently (although the polarity is undefined) when  
in the RX mode, with no incoming carrier, reduces the desire  
to implement carrier detection and preserves the full ulti-  
mate sensitivity. Also, many impulse-noise insensitive trans-  
mission schemes, like handshaking, are easily modified to  
recover from line collisions.  
TL/H/675032  
FIGURE 29. Impressed line voltage for a given Z  
for each of the 3 taps available  
L
on the recommended transformers  
b
a
b
a
I
2(  
V
V
)
(
4.7  
V )I  
a
a
OPP  
ALC  
O
e
e
V
O O  
e
P
I
(5)  
O
2
2
2
2
4
0
Ð
0
(
where I is in amps peak-to-peak at an elevated T  
O
J
b
(18 4.7) 0.06  
e
e
b
P
0.200 W  
(6)  
(7)  
O
4
2
a
V
O
(
V
V
) 2  
a 0  
ALC  
e
e
e
442 X  
R
R
Z
LN Ê  
l
Q
Q
ll l  
P
I
O
O
is found using Z and the value for N found when as-  
LN  
e
suming Q  
35.  
U
2
N
2
(7.07) 13.9  
e
e
Z
LN  
e
Z
695 X  
(8)  
(9)  
LN Ê  
l
l
1
1
e
e
e
1210 X  
R
Q
1
1
1
1
Regarding this, it should be stated that for very complicated  
industrial systems with long signal runs and high line noise  
levels, it is probably wise to use a protocol which is inherent-  
ly collision free so that no carrier detect hardware or soft-  
ware is needed. A token passing protocol is an example of  
such a system.  
b
e
b
R
Q
Z
Z
442 695  
LN Ê  
l
LN Ê  
ll l  
R
l
l
1210  
Q
e
e
1 X  
R
(10)  
QS  
2
2
a
a
35  
1
Q
1
U
Only Q remains to be found to calculate L . Q is related to  
L
L
the 3 dB (half-power) bandwidth by  
1
b
Figure 30 shows a low cost carrier amplitude detection cir-  
cuit.  
1
e
Q
(11)  
L
BW (% of F  
)
O
Audio Transmission  
An iterative solution is forced where line pull, DF , must be  
Q
guessed to find Q and L . L is then used to check the line  
The LM1893 is designed to allow analog data transmission  
and reception. Base-band audio-bandwidth signals FM  
modulate the carrier passing through the tuned transformer  
(placing a limit on the usable percent modulation) onto the  
power line to be linearly demodulated by the receiver PLL.  
Because the receiver data path beyond the phase detector  
will pass only digital signal, external audio filtering and am-  
plification is required. Figure 31 shows a simple audio trans-  
mitter and receiver circuit utilizing a carrier detection mute  
circuit. A single LM339 quad. comparator may be used to  
build the carrier detect and mute. Filter bandwidth is held to  
a minimum to minimize noise, especially line-related corre-  
lated noise.  
L
1
1
pull guess; a large error requires a new guess. Try a BW of  
8.7% - that is 4.4% for deviation, 1% for TC of F , and  
O
e
3.3% for DF - giving Q  
11.5.  
Q
L
442  
e
e
49.0 mH  
L
1
(12)  
c
c
2q 125 000 11.5  
Knowing the core inductance per turn, L, and L , the num-  
1
ber of turns is found.  
L
49.0 mH  
1
e
e
e
49 (/2 turns  
T
(13)  
1
L
20 nH/T  
0 0  
T is normally an integer, but these transformers require so  
few turns that half-turns are specified, remembering that the  
remaining (/2 turn is completed on the P.C. board and is  
loosely coupled. The secondary turns are calculated  
Communication and System  
Protocols  
The development of communication and system protocols  
has historically been the single most time consuming ele-  
ment in design of carrier current systems. The protocols are  
defined as the following:  
T
49.5  
7.07  
1
e
e
e
e
7.00 7 turns  
T
(15)  
2
N
giving an L of 0.98 mH. Note that the recommended 125  
2
kHz transformer mirrors these specifications. The resonat-  
ing capacitor is  
1. Communication protocol: a software method of encoding  
and decoding data that remains constant for every transmis-  
1
b
9
e
33 nF  
e
e
c
33.1 10  
C
(16)  
Q
2
) L  
1
(2qF  
Q
17  
TL/H/675033  
FIGURE 30. A simple carrier amplitude detector with output low when carrier is detected  
TL/H/675034  
FIGURE 31. A simple linear analog audio transmitter and receiver are shown.  
The carrier and 1.6V inputs are derived from the carrier detector ofFigure 30.  
The remaining 2 LM339 comparators may be used to build the carrier detector circuit.  
Communication and System  
Protocols (Continued)  
sion in a system. Its first purpose is to put data in a base-  
band digital form that is more easily recognized as a real  
message at the receive end. Secondly, it incorporates en-  
coding techniques to ensure that noise induced errors do  
not easily occur; and when they do, they can always be  
detected. Lastly, the software algorithms that are used on  
the receive end to decode incoming data prevent the recep-  
tion of noise induced ‘‘phantom’’ messages, and insure the  
recovery of real messages from an incoming bit stream that  
has been altered by noise.  
ensure message retransmission to correct errors (hand-  
shake). Secondly it coordinates messages for maximum uti-  
lization and efficiency on the network. Lastly, it ensures that  
messages do not collide on the network. Common system  
protocols include master-slave, carrier detect multiple ac-  
cess, and token passing. Token passing and master slave  
have been found to be the most useful since they are inher-  
ently collision free.  
Both protocols usually reside as software in a single micro-  
controller that is connected to the LM1893/2893 I/O. In any  
case, some sort of intelligence is needed to process incom-  
ing and outgoing messages. UARTs have no usefulness in  
2. System protocol: the manner in which messages are co-  
ordinated between nodes in a system. Its first purpose is to  
18  
transmission, using a random number of bits delay or a de-  
lay based on each transmitter’s address, since each trans-  
ceiver has a unique address.  
Communication and System  
Protocols (Continued)  
carrier current applications since they do not have the intelli-  
gence needed to distinguish between real messages and  
noise induced phantoms.  
An example of a simple transmission data packet is shown  
in Figure 32. The 8 bit 50% duty-cycle preamble is long  
enough to allow receiver biasing with enough bits left over  
to allow the receiver controller to detect the square-wave  
that signals the start of a transmission. If there had been no  
transmission for some time, the receiver would simply need  
to note that a data transition had occurred and begin its  
watch for a square-wave. If the receive controller detected  
the alternating-polarity data square-wave it would then use  
the sync. bit to signal that the address and data were imme-  
diately following. The address data would then be loaded,  
assuming the fixed format, and tested against its own. If the  
address was correct, the receiver would then load and store  
the data. If the address was not correct, either the transmis-  
sion was not meant for this receiver or noise has fooled the  
receiver. In the former case, when the transmission was not  
meant for the receiver, the controller should immediately  
return to watching the incoming data for its address. If the  
later case were true, then the receive controller would con-  
tinue to detect edges, tieing itself up by loading false data  
and being forced to handshake. The square-wave detection  
and address load and check routines should be fast to mini-  
mize the time spent in loops after being false-triggered by  
noise. If the controller detects an error (a received data bit  
that does not conform to the pre-defined encoding format) it  
should immediately resume watching the LM1893’s Data  
Out for transmissions, the next bit would be shifted in and  
the process repeated.  
The difficulty in designing special protocols arises out of the  
special nature of the AC line, an environment laden with the  
worst imaginable noise conditions. The relatively low data  
rates possible over the AC line (typically less than 9600  
baud) make it even more imperative that systems utilize the  
most sophisticated means available to ensure network effi-  
ciency.  
With these facts in mind, the designer is referred to a publi-  
cation intended to aid in the development of carrier current  
Ý
systems. This is literature 570075 The Bi-Line Carrier Cur-  
rent Networking System, a 200 pp. book that functions as  
the ‘‘bible’’ of Bi-Line system design. It has sections on  
LM1893 circuit optimization, protocol design, evaluation kit  
usage, critical component selection, and the Datachecker/  
DTS case study.  
Basic Data Encoding (please refer to the pre-  
viously mentioned publications for advanced techniques)  
At the beginning of a received transmission, the first 0 to 2  
bits may be lost while the chip’s receiver settles to the DC  
bias point required for the given transmitter/receiver pair  
carrier frequency offset. With proper data encoding,  
dropped start bits can be tolerated and correct communica-  
tion can take place. One simple data encoding scheme is  
now discussed.  
A line-synchronous CCT system passing 3 bits per half-cy-  
cle may replace the long 8 bit preamble and sync pulse with  
a 2 bit start-of-transmission bias preamble. The receive con-  
troller might then assume that preamble always starts after  
bit 1 (the first bit after zero-crossing) so that any data tran-  
sition at a zero crossing must be the start of the address bits  
and is tested as such. The line synchronous receiver oper-  
ates with a simpler controller than an asynchronous system.  
Generally, a CCT system consists of many transceivers that  
normally listen to the line at all times (or during predeter-  
mined time windows), waiting for a transmission that directs  
one or more of the receivers to operate. If any receiver finds  
its address in the transmitted data packet, further action  
such as handshaking with the transmitter is initiated. The  
receiver might tell the transmitter, via retransmission, that it  
received this data, waiting for acknowledgement before act-  
ing on the received command. Error detecting and correct-  
ing codes may be employed throughout. The transmitter  
must have the capability to retransmit after a time if no re-  
sponse from the receiver is heard - under the assumption  
that the receiver didn’t detect its address because of noise,  
or that the response was missed because of noise or a line  
collision. (A line collision happens when more than 1 trans-  
mitter operates at one time - causing one or more of the  
communications to fail). After many re-transmissions the  
transmitter might choose to give up. Collision recovery is  
achieved by waiting some variable amount of time before re-  
Discussion has assumed that the controller has always  
known when the Data Out is high or low. The controller  
must sample at the proper time to check the Data Out state.  
Since noise shows itself as pulse width jitter, symmetrically  
placed about the no-noise switch-points, optimum Data Out  
sampling is done in the center of the received data pulse.  
The receive data path has a time delay that, at low data  
rates, is dominated by the impulse noise filter integrator and  
is nominally (/2 bit. At a 2 kHz data rate, an additional delay  
of approximately (/10 bit is added because of the cumulative  
delay of the remainder of the receiver. Figure 33 shows that  
Data Out sampling occurs conveniently at the transmitted  
TL/H/675035  
FIGURE 32. A simple encoded data packet, generated by the transmit controller is shown.  
The horizontal axis is time where 1 bit time is 1/(2f  
)
DATA  
19  
Because the coupling transformer is used as a filter, the  
LM1893 circuit is susceptible to pulling of the center fre-  
quency under conditions of changing line impedances or  
when several LM1893 circuits are close in proximity on the  
AC line. Because the tuned transformer has a high value of  
‘‘Q’’, ringing also occurs in the presence of impulsive noise.  
This ringing occurs at the center frequency and increases  
the error rate of transmissions, especially at relatively high  
Basic Data Encoding (Continued)  
l
data rates ( 2000 baud). Because it is the only tuned circuit  
in the system, the selectivity characteristics leave a lot to be  
desired.  
The LM2893, having separate receive input and transmit  
output pins, removes the limitations on coupling transformer  
design, allowing the design of circuits devoid of the previous  
limitations.  
TL/H/675036  
FIGURE 33. Operating waveforms of a line-  
synchronized transceiver pair are shown. The diagram  
shows how the transmitted data transitions may be  
used as received data sampling points  
The first enhancement that can be made with the LM2893  
circuit is the use of a high permeability ferrite toroid for line  
coupling along with a separate filter. The transformer would  
be of broadband design (untuned) with two secondaries,  
one for coupling to the transmit output and one for coupling  
to the receive input. This allows impedance matching of  
both the transmitter and receiver, with the result of quite a  
bit more receive sensitivity.  
data edges for the line synchronous data transmission  
scheme mentioned in the previous paragraph. With the  
asynchronous system suggested, the receive controller  
must sample the Data Out pin often to determine, with sev-  
eral bits of accuracy, where the square-wave data tran-  
Because of the increased signal and separate receive signal  
path, a 3 or 6 db pad can be used before the selective  
stages to eliminate pulling of the center frequency due to  
changes in line impedance.  
sitions take place, average their positions assuming  
a
known data rate, and calculate where the center of the data  
bits are and will continue to be as the address and data are  
read. A long preamble is helpful. Software that continuously  
updates the center-of-bit time estimate, as address and  
data are received, works even better. Alternatively, a coding  
scheme employing an embedded clock can be used.  
Another advantage of the toroidal transformer is that it can  
be designed for use at very low line impedances due to its  
inherent tight coupling.  
SEPARATE FILTER  
LM2893 Application Hints  
Because of the separate receive path of the LM2893, a rela-  
tively high quality bandpass filter can be used for selectivity.  
Inexpensive ceramic filters are available that have band-  
pass and center frequency characteristics compatible with  
carrier current operation. Futhermore, the use of these fil-  
ters allows multichannel operation, previously made difficult  
by the single tuned network of the LM1893. These filters are  
easily cascaded for even more off-frequency rejection. If the  
pad is added before the filter, there will be negligible pulling  
due to changes in line impedance reflected through the cou-  
pling transformer.  
The LM2893 is intended for advanced applications where  
special circuitry is used in the transmit and receive paths.  
The LM2893 makes this possible by featuring separate  
transmit output and receive input pins.  
Examples of enhancements that can be added to the basic  
LM1893/2893 circuit include separate transmit and receive  
windings on the coupling transformer, high quality ceramic  
or LC filters in the receive path, and simple impulse noise  
blanking circuits.  
In many applications, the additional performance to be  
gained outweighs the extra cost of the additional circuitry.  
More than likely, high performance industrial applications  
such as building energy management will fit into this catego-  
ry, since they require the utmost in reliability.  
Alternatively, a Butterworth/Chebyshev bandpass LC filter  
or an active filter can be used in place of the ceramic filter.  
IMPULSE NOISE BLANKER  
Although the LM2893 has adequate impulse noise rejection  
for most applications, there is reason to employ impulse  
blanking to improve error rates in severe AC line environ-  
ments. Typically, errors occur due to pulse jitter in the  
LM1893/2893 data output that originates when the internal  
time domain filter smooths out an incoming noise pulse.  
Because of the specialized nature of individual LM2893 ap-  
plications, it is not possible to give one circuit that will satisfy  
all requirements for performance and cost effectiveness.  
Therefore no specific application examples will be given.  
Instead the subsequent text describes in general terms the  
types of circuits that can be used to increase performance  
along with their advantages and disadvantages. It is intend-  
ed to be a springboard for ideas.  
The solution involves removing the impulse completely and  
not simply trying to filter it. Moreover, the pulse should be  
removed in the receive signal path before the selective por-  
tions of the circuit to eliminate ringing. This also allows the  
receiver filter to smooth out the blanks that also occur in the  
desired incoming carrier signal.  
LM2893 COUPLING NETWORKS  
The main disadvantages of the typical LM1893 coupling  
network are that it functions as the bandpass filter, has  
loose coupling between primary and secondary, and has a  
single secondary. The LM1893 coupling network was de-  
signed this way mainly because of the restraint that the car-  
rier input and output are tied together.  
If a carrier detect circuit is desired in conjunction with the  
LM2893 it can be located after the filter and impulse blank-  
er. Because impulse noise is removed, the false triggering  
that plagues these circuits will be greatly reduced.  
20  
Simplified Schematic  
21  
References  
4. FCC, ‘‘Notice of Proposed Rule Making,’’ Docket 20780,  
adopted Apr. 14, 1976, (Proposed regulation)  
1. Nicholson, J.R. and J.A. Malack; ‘‘RF Impedance of Pow-  
er Lines and Line Impedance Stabilization Network in  
Conducted Interference Measurements;’’ IEEE Transac-  
tions on Electromagnetic Compatibility; May 1973; (line  
impedance data)  
5. Monticelli, Dennis M. and Michael E. Wright; ‘‘A Carrier  
Current Transceiver IC for Data Transmission Over the  
AC Power Lines;’’ IEEE J. Solid-State Circuits; vol. SC-17;  
Dec. 1982; pp. 1158-1165; (LM1893 circuit description)  
2. Southwick, R.A.; ‘‘Impedance Characteristics of Single-  
Phase Power Lines;’’ Conference Rec.; 1973 IEEE Int.  
Symp. on Electromagnetic Compatibility; (line impedance  
data)  
6. Lee, Mitchell; ‘‘A New Carrier Current Transceiver IC;’’  
IEEE Trans. on Consumer Electronics; vol. CE-28; Aug.  
1982; pp. 409414; (Application of LM1893)  
3. Hayt, William H. Jr. and Jack E. Kemmerly; ‘‘Engineering  
Circuit Analysis;’’ McGraw-Hill Books; 1971; pp. 447–  
453; (linear transformer reflected impedance)  
22  
Physical Dimensions inches (millimeters)  
Molded Small Outline Package (M)  
Order Part LM2893M  
NS Package Number M20B  
Molded Dual-In-Line Package (N)  
Order Part LM1893N  
NS Package Number N18A  
23  
Ý
Lit. 107664  
Physical Dimensions inches (millimeters) (Continued)  
Molded Dual-In-Line Package (N)  
Order Part LM2893N  
NS Package Number N20A  
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systems which, (a) are intended for surgical implant  
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failure to perform, when properly used in accordance  
with instructions for use provided in the labeling, can  
be reasonably expected to result in a significant injury  
to the user.  
2. A critical component is any component of a life  
support device or system whose failure to perform can  
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