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NE570DR2 Datasheet(PDF) 7 Page - ON Semiconductor

Part # NE570DR2
Description  Compandor
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Manufacturer  ONSEMI [ON Semiconductor]
Direct Link  http://www.onsemi.com
Logo ONSEMI - ON Semiconductor

NE570DR2 Datasheet(HTML) 7 Page - ON Semiconductor

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At very high frequencies, the response of the rectifier will
fall off. The roll−off will be more pronounced at lower input
levels due to the increasing amount of gain required to switch
between Q5 or Q6 conducting. The rectifier frequency
response for input levels of 0 dBm, −20 dBm, and −40 dBm
is shown in Figure 11. The response at all three levels is flat
to well above the audio range.
0
3
10 k
1 MEG
INPUT = 0 dBm
−20 dBm
−40 dBm
FREQUENCY (Hz)
Figure 11. Rectifier Frequency Response
vs. Input Level
VARIABLE GAIN CELL
Figure 12 is a diagram of the variable gain cell. This is a
linearized two−quadrant transconductance multiplier. Q1,
Q2 and the op amp provide a predistorted drive signal for the
gain control pair, Q3 and Q4. The gain is controlled by IG and
a current mirror provides the output current.
V+
V−
Q2
Q1
NOTE:
IOUT =
IG
I1
R2
20 k
W
VIN
IIN
I2 ( = 2 I1 )
280
mA
+
I1
140
mA
Q4
Q3
IG
IIN =
VIN
R2
IG
I1
Figure 12. Simplified
DG Cell Schematic
The op amp maintains the base and collector of Q1 at
ground potential (VREF) by controlling the base of Q2. The
input current IIN (= VIN/R2) is thus forced to flow through
Q1 along with the current I1, so IC1 = I1 + IIN. Since I2 has
been set at twice the value of I1, the current through Q2 is:
I2 * (I1 ) IIN) + I1 * IIN + IC2.
The op amp has thus forced a linear current swing between
Q1 and Q2 by providing the proper drive to the base of Q2.
This drive signal will be linear for small signals, but very
non−linear for large signals, since it is compensating for the
non−linearity of the differential pair, Q1 and Q2, under large
signal conditions.
The key to the circuit is that this same predistorted drive
signal is applied to the gain control pair, Q3 and Q4. When
two differential pairs of transistors have the same signal
applied, their collector current ratios will be identical
regardless of the magnitude of the currents. This gives us:
I
C1
I
C2
+
I
C4
I
C3
+
I
1 ) IIN
I
1 * IIN
plus the relationships IG = IC3 + IC4 and IOUT = IC4 − IC3
will yield the multiplier transfer function,
I
OUT +
I
G
I
1
I
IN +
V
IN
R
2
I
G
I
1
This equation is linear and temperature−insensitive, but it
assumes ideal transistors.
4
3
2
1
0.34
−6
0
+6
4 mV
3 mV
2 mv
1 mV
INPUT LEVEL (dBm)
VOS = 5 mV
Figure 13.
DG Cell Distortion vs. Offset Voltage
If the transistors are not perfectly matched, a parabolic,
non−linearity is generated, which results in second
harmonic distortion. Figure 13 gives an indication of the
magnitude of the distortion caused by a given input level and
offset voltage. The distortion is linearly proportional to the
magnitude of the offset and the input level. Saturation of the
gain cell occurs at a +8.0 dBm level. At a nominal operating
level of 0 dBm, a 1.0 mV offset will yield 0.34% of second
harmonic distortion. Most circuits are somewhat better than


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