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VCA610 Datasheet(PDF) 11 Page - Burr-Brown (TI)

[Old version datasheet] Texas Instruments acquired Burr-Brown Corporation.
Part # VCA610
Description  WIDEBAND VOLTAGE CONTROLLED AMPLIFIER
Download  12 Pages
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Manufacturer  BURR-BROWN [Burr-Brown (TI)]
Direct Link  http://www.burr-brown.com
Logo BURR-BROWN - Burr-Brown (TI)

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®
VCA610
11
FIGURE 10. Signal Drive of the VCA610 Gain Control Pin
Produces and Exponential Response, Re-ex-
panding Signal Companded by Figure 9.
R
2
330
VCA610
R
1
470
V
O = –VR10
–2 [R1 VIN /(R1 + R2) + 1]
V
IN
V
R
–10mV
V
C
FIGURE 11. This Voltage-Tuneable Low-Pass Filter Pro-
duces a Variable Cutoff Frequency with a
3,000:1 Range.
Finite loop gain and a signal swing limitation set perfor-
mance boundaries for the circuit. Both limitations occur
when the VCA610 attenuates rather than amplifies the
feedback signal. These two limitations reduce the circuit’s
utility at the lower extreme of the VCA610’s gain range. For
–1
≤ V
C ≤ 0, this amplifier produces attenuating gains in the
range from 0dB to –40dB. This directly reduces the net gain
in the circuit’s feedback loop, increasing gain error effects.
Also, this attenuation transfers an output swing limitation
from the OPA620 output to the overall circuit’s output. Note
that OPA620 output voltage, V
OA, relates to VO through the
expression V
O = GVOA. Thus, a G < 1 limits the maximum
V
O swing to a value less than the maximum VOA swing.
However, the circuit shown provides greater output swing
than the more common multiplier implementation. The latter
replaces the VCA610 of the figure with an analog multiplier
having a response of V
O = XY/10. Then, X = VOA and Y =
V
C, making the circuit output voltage VO = VOAVC/10. Thus,
the multiplier implementation amplifies V
OA by a gain of VC/
10. Circuit constraints require that V
C ≤ 10, making this gain
≤ 1. Thus, the multiplier performs only as a variable attenu-
ator and never provides amplification. As a result, the
voltage swing limitation of V
OA
restricts the V
O
swing
throughout most of the circuit’s control range. Replacing the
multiplier with the VCA610 shown permits equivalent gains
greater > 1. Then, operating the VCA610 with gains in the
range of one to 100 avoids the reduction in output swing
capability.
VOLTAGE-CONTROLLED HIGH-PASS FILTER
A circuit analogous to the above low-pass filter produces a
voltage-controlled high-pass response. The gain control pro-
vided by the VCA610 of Figure 12 varies this circuit’s
response zero from 1Hz to 10kHz according to the relation-
ship F
Z ≈ 1/2πGR1C where G = 10
–2 (V
C
+ 1)
.
f
P = G/2πR2C
G = 10 –2(VC + 1)
V
O
V
I
= –
R
2
R
1
1
1 + R
2Cs/G
VOLTAGE-CONTROLLED LOW-PASS FILTER
In the circuit of Figure 11, the VCA610 serves as the
variable gain element of a voltage-controlled low-pass filter.
As will be described, this implementation expands the circuit’s
voltage swing capability over that normally achieved with
the equivalent multiplier implementation. The circuit’s re-
sponse pole responds to control voltage V
C according to the
relationship f
P = G/2πR2C where G = 10
–2 (V
C
+ 1)
. With the
components shown, the circuit provides a linear variation of
the low-pass cutoff from 300Hz to 1MHz.
FIGURE 12. A Voltage-Tunable High-Pass Filter Pro-
duces a Response Zero Variable from 1Hz to
10kHz.
The response control results from amplification of the feed-
back voltage applied to R
2. Consider first the case where the
VCA610 produces G = 1. Then, the circuit performs as if
this amplifier were replaced by a short circuit. Visually
doing so leaves a simple voltage amplifier with a feedback
resistor bypassed by a capacitor. This basic circuit produces
a response pole at f
P = 1/2πR2C.
For G > 1, the circuit applies a greater voltage to R
2,
increasing the feedback current this resistor supplies to the
summing junction of the OPA620. The increased feedback
current produces the same result as if R
2 had been decreased
in value in the basic circuit described above. Decreasing the
effective R
2 resistance moves the circuit’s pole to a higher
frequency, producing the f
P = G/2πR2C response control.
OPA620
VCA610
V
C
V
O
V
OA
0.047µF
330
R
2
330
R
1
C
V
I
OPA620
VCA610
V
C
0.047µF
V
OA
CR
3
33
V
O
R
2
33k
R
1
33k
V
I
For R
3 << GR1 and f << 1/2πR3Cs,
V
O
V
I
R
2
R
1
(1 + GR
1Cs), fZ = 1/2πGR1C
where G = 10–2(VC + 1)
= –


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