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VCA810ID

Part # VCA810ID
Description SINGLE VOLTAGE CONTROL AMP -Rail/Tube
Category IC
Availability Out of Stock
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Technical Document


DISCLAIMER: The information provided herein is solely for informational purposes. Customers must be aware of the suitability of this product for their application, and consider that variable factors such as Manufacturer, Product Category, Date Codes, Pictures and Descriptions may differ from available inventory.

f =
W
1
2 R Cp
W W
VCA810
C
H
1 Fm
V-
OPA820
V
R
0.1 VDC
V = V
OPEAK R
V
O
R
3
1kW
HP5082
R
1
50kW
C
W1
4700pF
R
4
100W
R
2
50kW
R
W1
300W
R
W2
300W
C
W2
4700pF
C
C
10pF
f = 1/2 R Cp
W1 W1
V
C
R = R
W1 W2
C = C
W1 W2
VCA810
www.ti.com
SBOS275F JUNE 2003REVISED DECEMBER 2010
STABILIZED WEIN-BRIDGE OSCILLATOR magnitude of C
W
equals R
W
, and inspection of the
circuit shows that this condition produces a feedback
Adding Wein-bridge feedback to the above AGC
factor of 1/3. Thus, self-sustaining oscillation requires
amplifier produces an amplitude-stabilized oscillator.
a gain of three through the amplifier. The AGC
As Figure 34 shows, this alternative requires the
circuitry establishes this gain level. Following initial
addition of just two resistors (R
W1
, R
W2
) and two
circuit turn-on, R
1
begins charging C
H
negative,
capacitors (C
W1
, C
W2
).
increasing the amplifier gain from its minimum. When
this gain reaches three, oscillation begins at f
W
; the
Connecting the feedback network to the amplifier
continued charging effect of R
1
makes the oscillation
noninverting input introduces positive feedback to
amplitude grow. This growth continues until that
induce oscillation. The feedback factor displays a
amplitude reaches a peak value equal to V
R
. Then,
frequency dependence due to the changing
the AGC circuit counteracts the R
1
effect, controlling
impedances of the C
W
capacitors. As frequency
the peak amplitude at V
R
by holding the amplifier gain
increases, the decreasing impedance of the C
W2
at a level of three. Making V
R
an ac signal, rather
capacitor increases the feedback factor.
than a dc reference, produces amplitude modulation
Simultaneously, the decreasing impedance of the
of the oscillator output.
C
W1
capacitor decreases this factor. Analysis shows
that the maximum factor occurs at Hz,
making this the frequency most conducive to
oscillation. At this frequency, the impedance
Figure 34. Amplitude-Stabilized Oscillator
Copyright © 2003–2010, Texas Instruments Incorporated Submit Documentation Feedback 13
Product Folder Link(s): VCA810
G =
10
-2
(V + 1)
C
5
4
3
2
1
0
1
2
3
4
5
-
-
-
-
-
Output Voltage (V)
V /V
IN R
Voltage Ratio
0.001 0.01 0.1 1 10 100
I
II
III
R
1
470W
VCA810
R
2
330W
V
OL
V
R
-10mV
OPA820
V
IN
V = GV-
OA R
C
C
50pF
R
3
100W
V = 1 +- 1 + 0.5 Log( V /V )-
OL IN R
( )
V
C
R
R
1
2
10
-2
(V + 1)
C
V = V = V-
OA IN R
·
V =
C
R V
R + R
1 OL
1 2
·
V =
OL
-
1 +
R
R
2
1
(
(
1 + 0.5 log·
·
V
V
IN
R
(
(
-
VCA810
SBOS275F JUNE 2003REVISED DECEMBER 2010
www.ti.com
LOW-DRIFT WIDEBAND LOG AMP produces log-ratio operation. Either way, the log
term’s argument constrains the polarities of V
R
and
The VCA810 can be used to provide a 2.5MHz
V
IN
. These two voltages must be of opposite polarities
(–3dB) log amp with low offset voltage and low gain
to ensure a positive argument. This polarity
drift. The exponential gain-control characteristic of the
combination results when V
R
connects to the
VCA810 permits simple generation of a
inverting input of the VCA810. Alternately, switching
temperature-compensated logarithmic response.
V
R
to the amplifier noninverting input removes the
Enclosing the exponential function in an op-amp
minus sign of the log term argument. Then, both
feedback path inverts this function, producing the log
voltages must be of the same polarity in order to
response. Figure 35 shows the practical
produce a positive argument. In either case, the
implementation of this technique. A dc reference
positive polarity requirement of the argument restricts
voltage, V
R
, sets the VCA810 inverting input voltage.
V
IN
to a unipolar range. Figure 36 illustrates these
This configuration makes the amplifier output voltage
constraints.
V
OA
= GV
R
, where .
Figure 36. Test Result for LOG Amp for V
R
=
100mV
Figure 35. Temperature-Compensated Log
Response
The above V
OL
expression reflects a circuit gain
introduced by the presence of R
1
and R
2
. This feature
A second input voltage also influences V
OA
through
adds a convenient scaling control to the circuit.
control of gain G. The feedback op amp forces V
OA
to
However, a practical matter sets a minimum level for
equal the input voltage V
IN
connected at the op amp
this gain. The voltage divider formed by R
1
and R
2
inverting input. Any difference between these two
attenuates the voltage supplied to the V
C
terminal by
signals drops across R
3
, producing a feedback
the op amp. This attenuation must be great enough to
current that charges C
C
. The resulting change in V
OL
prevent any possibility of an overload voltage at the
adjusts the gain of the VCA810 to change V
OA
.
V
C
terminal. Such an overload saturates the VCA810
At equilibrium:
gain-control circuitry, reducing the amplifier’s gain.
For the feedback connection of Figure 35, this
(1)
overload condition permits a circuit latch. To prevent
this, choose R
1
and R
2
to ensure that the op amp
The op amp forces this equality by supplying the gain
cannot possibly deliver a more negative input than
2.5V to the V
C
terminal.
control voltage, .
Figure 36 exhibits three zones of operation described
Combining the last two expressions and solving for
below:
V
OL
yields the circuit’s logarithmic response:
Zone I: V
C
> 0V. The VCA810 is operating in full
attenuation (80dB). The noninverting input of the
OPA820 will see 0V. V
OL
is going to be the
(2)
integration of the input signal.
An examination of this result illustrates several circuit
Zone II: 2V < V
C
< 0V. The VCA810 is in its normal
characteristics. First, the argument of the log term,
operating mode, creating the log relationship in
V
IN
/V
R
, reveals an option and a constraint. In
Equation 2.
Figure 35, V
R
represents a dc reference voltage.
Optionally, making this voltage a second signal
14 Submit Documentation Feedback Copyright © 2003–2010, Texas Instruments Incorporated
Product Folder Link(s): VCA810
G
2 R Cp
2
f =
P
G =
10
-2
(V + 1)
C
R
2
330W
VCA810
R
1
470W
V
R
-10mV
V
C
500W 500W
OPA698
V
IN
V
L
V
I
-3.4V
+0.5V
V = V- x 10
OL R
-2
R V
R + R
1 IN
1 2
+1
(
(
OPA820
VCA810
V
C
V
O
V
OA
R
2
330W
R
1
330W
C
0.047 Fm
V
I
G
2 R Cp
2
f =
P
V
V
O
I
R
R
2
1
= -
R C
G
2 2
1 + s
1
·
G = 10
-2
(V + 1)
C
Input Voltage (V)
+3.0 +2.5 +2.0 +1.5 +1.0 +0.5 0
1
0.1
0.01
0.001
Output Voltage (V)
f =
P
G
2 R Cp
2
VCA810
www.ti.com
SBOS275F JUNE 2003REVISED DECEMBER 2010
Zone III: V
C
< 2V. The VCA810 control pin is out of
range, and some measure should be taken so that it
does not exceed –2.5V. A limiting action could be
VOLTAGE-CONTROLLED LOW-PASS FILTER
achieved by using a voltage limiting amplifier.
In the circuit of Figure 39, the VCA810 serves as the
variable-gain element of a voltage-controlled
LOW-DRIFT, WIDEBAND EXPONENTIAL AMP
low-pass filter. This section discusses how this
A common use of the log amp above involves signal implementation expands the circuit voltage swing
compounding. The inverse function, signal capability over that normally achieved with the
expanding, requires an exponential transfer function. equivalent multiplier implementation. The circuit
The VCA810 produces this latter response directly, response pole responds to control voltage V
C
as shown in Figure 37. DC reference V
R
again sets according to the relationship in Equation 3:
the amplifier input voltage, and the input signal V
IN
now drives the gain control point. Resistors R
1
and R
2
(3)
attenuate this drive to prevent overloading the gain
control input. Setting these resistors at the same
where
values as in the preceding log amp produces an
exponential amplifier with the inverse function of the
With the components shown, the circuit provides a
log amp.
linear variation of the low-pass cutoff from 300Hz to
1MHz.
Figure 37. Exponential Amplifier
Testing the circuit given in Figure 37 gives the
exponential response shown in Figure 38.
Figure 39. Tunable Low-Pass Filter
The response control results from amplification of the
feedback voltage applied to R
2
. First, consider the
case where the VCA810 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 .
Figure 38. Exponential Amplifier Response
Copyright © 2003–2010, Texas Instruments Incorporated Submit Documentation Feedback 15
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