NE570
http://onsemi.com
4
13
2, 15
4 1, 16
5, 12 8, 9
7, 10
6, 11
V
1
V
2
V
O
V
CC
= 15 V
V
REF
10 mF0.1 mF
200 pF
8.2 kW2.2 mF
+
30 kW
20 kW
DG
10 kW
20 kW
2.2 mF
3, 14
2.2 mF
Figure 3. Typical Test Circuit
INTRODUCTION
Much interest has been expressed in high performance
electronic gain control circuits. For non−critical applications,
an integrated circuit operational transconductance amplifier
can be used, but when high−performance is required, one has
to resort to complex discrete circuitry with many expensive,
well−matched components. This paper describes an
inexpensive integrated circuit, the NE570 Compandor, which
offers a pair of high performance gain control circuits
featuring low distortion (<0.1 %), high signal−to−noise ratio
(90 dB), and wide dynamic range (110 dB).
CIRCUIT BACKGROUND
The NE570 Compandor was originally designed to satisfy
the requirements of the telephone system. When several
telephone channels are multiplexed onto a common line, the
resulting signal−to−noise ratio is poor and companding is
used to allow a wider dynamic range to be passed through the
channel. Figure 4 graphically shows what a compandor can
do for the signal−to−noise ratio of a restricted dynamic range
channel. The input level range of +20 dB to80 dB is shown
undergoing a 2to−1 compression where a 2.0 dB input level
change is compressed into a 1.0 dB output level change by the
compressor. The original 100 dB of dynamic range is thus
compressed to a 50 dB range for transmission through a
restricted dynamic range channel. A complementary
expansion on the receiving end restores the original signal
levels and reduces the channel noise by as much as 45 dB.
The significant circuits in a compressor or expander are
the rectifier and the gain control element. The phone system
requires a simple full−wave averaging rectifier with good
accuracy, since the rectifier accuracy determines the (input)
output level tracking accuracy. The gain cell determines the
distortion and noise characteristics, and the phone system
specifications here are very loose. These specs could have
been met with a simple operational transconductance
multiplier, or OTA, but the gain of an OTA is proportional
to temperature and this is very undesirable. Therefore, a
linearized transconductance multiplier was designed which
is insensitive to temperature and offers low noise and low
distortion performance. These features make the circuit
useful in audio and data systems as well as in
telecommunications systems.
INPUT
LEVEL
COMPRESSION
EXPANSION
OUTPUT
LEVEL
NOISE
+20
0 dB
−40
−80
−20
0 dB
−40
−80
Figure 4. Restricted Dynamic Range Channel
NE570
http://onsemi.com
5
BASIC CIRCUIT HOOK−UP AND OPERATION
Figure 5 shows the block diagram of one half of the chip,
(there are two identical channels on the IC). The full−wave
averaging rectifier provides a gain control current, I
G
, for the
variable gain (DG) cell. The output of the DG cell is a current
which is fed to the summing node of the operational
amplifier. Resistors are provided to establish circuit gain and
set the output DC bias.
7, 10
OUTPUT
+
DG
R
2
20 kW
V
REF
1.8 V
5, 12
INV. INR3
6, 11
R
3
20 kW
R
4
30 kW
V
CC
: PIN 13
GND: PIN 4
I
G
C
RECT
1, 16
8, 9
THD_TRIM
R
1
10 kW
RECT_IN
2, 15
3, 14
DG_CELL_IN
Figure 5. Chip Block Diagram (1 of 2 Channels)
The circuit is intended for use in single power supply
systems, so the internal summing nodes must be biased at
some voltage above ground. An internal band gap voltage
reference provides a very stable, low noise 1.8 V reference
denoted V
REF
. The non−inverting input of the op amp is tied
to V
REF
, and the summing nodes of the rectifier and DG cell
(located at the right of R
1
and R
2
) have the same potential.
The THD_TRIM pin is also at the V
REF
potential.
Figure 6 shows how the circuit is hooked up to realize an
expander. The input signal, V
IN
, is applied to the inputs of
both the rectifier and the DG cell. When the input signal
drops by 6.0 dB, the gain control current will drop by a factor
of 2, and so the gain will drop 6 dB. The output level at V
OUT
will thus drop 12 dB, giving us the desired 2−to−1
expansion.
V
OUT
+
DG
R
4
V
REF
R
3
*C
RECT
R
2
R
1
V
IN
*C
IN1
*C
IN2
* EXTERNAL COMPONENTS
GAIN =
2 R
3
V
IN
(Avg.)
R
1
R
2
I
B
I
B
= 140 mA
NOTES:
Figure 6. Basic Expander
2
Figure 7 shows the hook−up for a compressor. This is
essentially an expander placed in the feedback loop of the op
amp. The DG cell is set−up to provide AC feedback only, so
a separate DC feedback loop is provided by the two R
DC
and
C
DC
. The values of R
DC
will determine the DC bias at the
output of the op amp. The output will bias to:
V
OUT
DC +
ǒ
1 )
R
DC1
) R
DC2
R
4
Ǔ
V
REF
V
OUT
DC +
ǒ
1 )
R
DC TOT
30 kW
Ǔ
1.8 V
The output of the expander will bias up to:
V
OUT
DC +
ǒ
1 )
R
3
R
4
Ǔ
V
REF
V
OUT
DC +
ǒ
1 )
20 kW
30 kW
Ǔ
1.8 V + 3.0 V
The output will bias to 3.0 V when the internal resistors
are used. External resistors may be placed in series with R3,
(which will affect the gain), or in parallel with R4 to raise the
DC bias to any desired value.
V
OUT
+
DG
R
4
V
REF
*R
DC
*C
DC
R
3
V
IN
*C
IN
* EXTERNAL COMPONENTS
GAIN =
I
B
= 140 mA
NOTES:
*R
DC
*C
RECT
R
1
R
2
*C
F
Figure 7. Basic Compressor
ǒ
R
1
R
2
I
B
2R
3
V
IN
(avg.)
Ǔ
1
2
NE570
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6
CIRCUIT DETAILS−RECTIFIER
Figure 8 shows the concept behind the full−wave
averaging rectifier. The input current to the summing node
of the op amp, V
IN
/R
1
, is supplied by the output of the op
amp. If we can mirror the op amp output current into a
unipolar current, we will have an ideal rectifier. The output
current is averaged by R
5
, C
R
, which set the averaging time
constant, and then mirrored with a gain of 2 to become I
G
,
the gain control current.
Figure 9 shows the rectifier circuit in more detail. The op
amp is a one−stage op amp, biased so that only one output
device is on at a time. The non−inverting input, (the base of
Q
1
), which is shown grounded, is actually tied to the internal
1.8 V V
REF
. The inverting input is tied to the op amp output,
(the emitters of Q
5
and Q
6
), and the input summing resistor
R1. The single diode between the bases of Q
5
and Q
6
assures
that only one device is on at a time. To detect the output
current of the op amp, we simply use the collector currents of
the output devices Q
5
and Q
6
. Q
6
will conduct when the
input swings positive and Q
5
conducts when the input
swings negative. The collector currents will be in error by the
α of Q
5
or Q
6
on negative or positive signal swings,
respectively. ICs such as this have typical NPN βs of 200
and PNP βs of 40. The αs of 0.995 and 0.975 will produce
errors of 0.5% on negative swings and 2.5% on positive
swings. The 1.5% average of these errors yields a mere
0.13 dB gain error.
At very low input signal levels the bias current of Q
2
,
(typically 50 nA), will become significant as it must be
supplied by Q
5
. Another low level error can be caused by DC
coupling into the rectifier. If an offset voltage exists between
the V
IN
input pin and the base of Q
2
, an error current of
V
OS
/R
1
will be generated. A mere 1.0 mV of offset will
cause an input current of 100 nA, which will produce twice
the error of the input bias current. For highest accuracy, the
rectifier should be coupled capacitively. At high input levels
the β of the PNP Q
6
will begin to suffer, and there will be an
increasing error until the circuit saturates. Saturation can be
avoided by limiting the current into the rectifier input to
250 mA. If necessary, an external resistor may be placed in
series with R
1
to limit the current to this value. Figure 10
shows the rectifier accuracy versus input level at a frequency
of 1.0 kHz.
+
R
1
V
IN
I = V
IN
/R
1
V+
I
G
R
5
10 kW
C
R
Figure 8. Rectifier Concept
R
5
10 kW
C
R
Q
8
Q
9
R
1
10 kW
V
IN
Q
5
Q
6
Q
7
Q
4
V+
V−
Q
2
Q
1
I
1
I
2
Q
3
NOTE:
I
G
= 2
D
1
V
IN
avg
R
1
Figure 9. Simplified Rectifier Schematic
ERROR GAIN dB
+1
0
−1
−40 −20 0
RECTIFIER INPUT dBm
Figure 10. Rectifier Accuracy

NE570DR2G

Mfr. #:
Manufacturer:
ON Semiconductor
Description:
Audio Amplifiers Dual Gain Compandor Commercial Temp
Lifecycle:
New from this manufacturer.
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