Freelance Electronics Components Distributor
Closed Dec 25th-26th
800-300-1968
We Stock Hard to Find Parts

VCA810ID

Part # VCA810ID
Description SINGLE VOLTAGE CONTROL AMP -Rail/Tube
Category IC
Availability Out of Stock
Qty 0



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.

G
2 GR Cp
1
f
Z
f =
P
G
2 R Cp
2
f
Z
1
2 R Cp
1
f
Z
1
2 R GCp
1
Frequency (Hz)
10k 100k 1M 10M
V = 1.4V-
C
V = 2V-
C
V = 1.6V-
C
V = 1.8V-
C
3
0
3
6
9
12
15-
-
-
-
-
Gain (dB)
OPA846
VCA810
V
C
50W
50W
OPA820
V
OA
C
2 Fm
R
3
3W
V
O
R
2
750W
R
1
750W
V
I
f
Z
1
2 (GR + R C)p
1 3
with G = 10
-2
(V + 1)
C
VCA810
SBOS275F JUNE 2003REVISED DECEMBER 2010
www.ti.com
For G > 1, the circuit applies a greater voltage to R
2
, TUNABLE EQUALIZER
increasing the feedback current this resistor supplies
A circuit analogous to the above low-pass filter
to the summing junction of the OPA820. The
produces a voltage-controlled equalizer response.
increased feedback current produces the same result
The gain control provided by the VCA810 of
as if R
2
had been decreased in value in the basic
Figure 41 varies this circuit response zero from 1Hz
circuit described above. Decreasing the effective R
2
to 10kHz, according to the relationship of Equation 4:
resistance moves the circuit pole to a higher
(4)
frequency, producing the response
control.
To visualize the circuit’s operation, consider a circuit
condition and an approximation that permit replacing
Finite loop gain and a signal-swing limitation set
the VCA810 and R
3
with short circuits. First, consider
performance boundaries for the circuit. Both
the case where the VCA810 produces G = 1.
limitations occur when the VCA810 attenuates, rather
Replacing this amplifier with a short circuit leaves the
than amplifies, the feedback signal. These two
operation unchanged. In this shorted state, the circuit
limitations reduce the circuit’s utility at the lower
is simply a voltage amplifier with an R-C bypass
extreme of the VCA810 gain range. For 1 V
C
0,
around R
1
. The resistance of this bypass, R
3
, serves
this amplifier produces attenuating gains in the range
only to phase-compensate the circuit, and practical
from 0dB to 40dB. This range directly reduces the
factors make R
3
<< R
1
. Neglecting R
3
for the
net gain in the circuit’s feedback loop, increasing gain
moment, the circuit becomes just a voltage amplifier
error effects. Additionally, this attenuation transfers
with a capacitive bypass of R
1
. This circuit produces
an output swing limitation from the OPA820 output to
the overall circuit’s output. Note that OPA820 output
voltage, V
OA
, relates to V
O
through the expression,
a response zero at .
V
O
= G V
OA
. Thus, a G < 1 limits the maximum V
O
Adding the VCA810 as shown in Figure 41 permits
swing to a value less than the maximum V
OA
swing.
amplification of the signal applied to capacitor C, and
Figure 40 shows the low-pass frequency for different
produces voltage control of the frequency f
Z
.
control voltages.
Amplified signal voltage on C increases the signal
current conducted by the capacitor to the op amp
feedback network. The result is the same as if C had
been increased in value to G
C
. Replacing C with this
effective capacitance value produces the circuit
control expression .
Figure 40. Voltage-Controlled Low-Pass Filter
Frequency Response
Figure 41. Tunable Equalizer
16 Submit Documentation Feedback Copyright © 2003–2010, Texas Instruments Incorporated
Product Folder Link(s): VCA810
f
O
=
10
-
(V + 1)
C
2 RCp
Frequency (Hz)
1 10 100 1k 10k 100k 1M 10M 100M
G = +40dB
G = +15dB
G = 15dB-
G = 40dB-
A
OL
100
90
80
70
60
50
40
30
20
10
0
Gain (dB)
=
s +
2
+
G
R C
2 2
s
nRC
s
nRC
-
V
V
O
I
Q = n ·
10
-
(V + 1)
C
VCA810
www.ti.com
SBOS275F JUNE 2003REVISED DECEMBER 2010
Another factor limits the high-frequency performance VOLTAGE-CONTROLLED BAND-PASS
of the resulting high-pass filter: the finite bandwidth of FILTER
the op amp. This limits the frequency duration of the
The variable gain of the VCA810 also provides
equalizer response. Limitations such as bandwidth
voltage control over the center frequency of a
and stability are clearly shown in Figure 42.
band-pass filter. As shown in Figure 43, this filter
follows from the state-variable configuration with the
VCA810 replacing the inverter common to that
configuration. Variation of the VCA810 gain moves
the filter’s center frequency through a 100:1 range
following the relationship of Equation 5:
(5)
As before, variable gain controls a circuit time
constant to vary the filter response. The gain of the
VCA810 amplifies or attenuates the signal driving the
lower integrator of the circuit. This amplification alters
the effective resistance of the integrator time
constant, producing the response of Equation 6:
Figure 42. Amplifier Noise Gain and A
OL
for
Different Gain
(6)
Evaluation of this response equation reveals a
Other limitations of this circuit are stability versus
passband gain of A
O
= –1, a bandwidth of BW =
VCA810 gain and input signal level for the circuit.
Figure 42 also illustrates these two factors. As the
1/(2pRC), and a selectivity of . Note
VCA810 gain increases, the crossover slope between
that variation of control voltage V
C
alters Q but not
the A
OL
curve of the OPA846 and noise gain will be
bandwidth.
greater than 20dB/decade, rendering the circuit
The gain provided by the VCA810 restricts the output
unstable. The signal level for high gain of the
swing of the filter. Output signal V
O
must be
VCA810 will meet two limitations: the output voltage
constrained to a level that does not drive the VCA810
swings of both the VCA810 and the OPA846. The
output, V
OA
, into its saturation limit. Note that these
expression V
OA
= GV
I
relates these two voltages.
two outputs have voltage swings related by V
OA
=
Thus, an output voltage limit V
OAL
constrains the input
G
VO
. Thus, a swing limit V
OAL
imposes a circuit output
voltage to V
I
V
OAL
/G.
limit of V
OL
V
OAL
/G.
With the components shown, BW = 50kHz. This
See Figure 44 for the frequency response for two
bandwidth provides an integrator response duration
different gain conditions of the schematic shown in
of four decades of frequency for f
Z
= 1Hz, dropping to
Figure 43. In particular, notice the center frequency
one decade for f
Z
= 10kHz.
shift and the selectivity of Q changing as the gain is
increased.
Copyright © 2003–2010, Texas Instruments Incorporated Submit Documentation Feedback 17
Product Folder Link(s): VCA810
VCA810
nR
5kW
R
330W
nR
5kW
C
0.047 Fm
V
C
R
330W
50W
50W
V
OA
C
0.047 Fm
V
I
V
O
1/2
OPA2822
1/2
OPA2822
=
s +
2
+
G
R C
2 2
s
nRC
s
nRC
-
V
V
O
I
f
O
=
10
-
(V + 1)
C
2 RCp
BW =
1
2 RCp
(V + 1)
C
Q = n
-
·10
A = 1-
O
0
5
10
15
20
25
30
35
40
45
50
-
-
-
-
-
-
-
-
-
-
Gain (dB)
Frequency (Hz)
100 1k 10k 100k
VCA810
SBOS275F JUNE 2003REVISED DECEMBER 2010
www.ti.com
Figure 43. Tunable Band-Pass Filter
Figure 44. Tunable Band-Pass Filter Response
18 Submit Documentation Feedback Copyright © 2003–2010, Texas Instruments Incorporated
Product Folder Link(s): VCA810
PREVIOUS12345678910NEXT