TI VCA2614

VCA
VCA810
810
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SBOS275F – JUNE 2003 – REVISED DECEMBER 2010
High Gain Adjust Range, Wideband,
VARIABLE GAIN AMPLIFIER
Check for Samples: VCA810
FEATURES
Operating from ±5V supplies, the gain control voltage
for the VCA810 will adjust the gain from –40dB at 0V
input to +40dB at –2V input. Increasing the control
voltage above ground will attenuate the signal path to
greater than 80dB. Signal bandwidth and slew rate
remain constant over the entire gain adjust range.
This 40dB/V gain control is accurate within ±1.5dB
(±0.9dB for high grade), allowing the gain control
voltage in an AGC application to be used as a
Received Signal Strength Indicator (RSSI) with
±1.5dB accuracy.
1
•
•
•
•
•
•
•
•
•
2
HIGH GAIN ADJUST RANGE: ±40dB
DIFFERENTIAL IN/SINGLE-ENDED OUT
LOW INPUT NOISE VOLTAGE: 2.4nV/√Hz
CONSTANT BANDWIDTH vs GAIN: 35MHz
HIGH dB/V GAIN LINEARITY: ±0.3dB
GAIN CONTROL BANDWIDTH: 25MHz
LOW OUTPUT DC ERROR: < ±40mV
HIGH OUTPUT CURRENT: ±60mA
LOW SUPPLY CURRENT: 24.8mA
(max for −40°C to +85°C temperature range)
Excellent
common-mode
rejection
and
common-mode
input
range
at
the
two
high-impedance inputs allow the VCA810 to provide a
differential receiver operation with gain adjust. The
output signal is referenced to ground. Zero differential
input voltage gives a 0V output with a small dc offset
error. Low input noise voltage ensures good output
SNR at the highest gain settings.
APPLICATIONS
•
•
•
•
•
•
•
OPTICAL RECEIVER TIME GAIN CONTROL
SONAR SYSTEMS
VOLTAGE-TUNABLE ACTIVE FILTERS
LOG AMPLIFIERS
PULSE AMPLITUDE COMPENSATION
AGC RECEIVERS WITH RSSI
IMPROVED REPLACEMENT FOR VCA610
In applications where pulse edge information is
critical, and the VCA810 is being used to equalize
varying channel loss, minimal change in group delay
over gain setting will retain excellent pulse edge
information.
+5V
6
V+
V-
VCA810
1
8
Gain
Adjust
+
X1
5
VOUT
An improved output stage provides adequate output
current to drive the most demanding loads. While
principally intended to drive analog-to-digital
converters (ADCs) or second-stage amplifiers, the
±60mA
output
current
will
easily
drive
doubly-terminated 50Ω lines or a passive post-filter
stage over the ±1.7V output voltage range.
VCA810 RELATED PRODUCTS
2
VC
DUALS
GAIN
ADJUST
RANGE
(dB)
VCA811
—
80
2.4
80
—
VCA2612
45
1.25
80
—
VCA2613
45
1
80
—
VCA2614
45
3.6
40
—
VCA2616
45
3.3
40
VCA2618
45
5.5
30
3
SINGLES
0 ® -2V
-40dB ® +40dB Gain
7
-5V
DESCRIPTION
The VCA810 is a dc-coupled, wideband, continuously
variable, voltage-controlled gain amplifier. It provides
a differential input to single-ended output conversion
with a high-impedance gain control input used to vary
the gain over a –40dB to +40dB range linear in dB/V.
INPUT
NOISE
(nV/√Hz)
SIGNAL
BANDWIDTH
(MHz)
1
2
Please be aware that an important notice concerning availability, standard warranty, and use in critical applications of Texas
Instruments semiconductor products and disclaimers thereto appears at the end of this data sheet.
All trademarks are the property of their respective owners.
PRODUCTION DATA information is current as of publication date.
Products conform to specifications per the terms of the Texas
Instruments standard warranty. Production processing does not
necessarily include testing of all parameters.
Copyright © 2003–2010, Texas Instruments Incorporated
VCA810
SBOS275F – JUNE 2003 – REVISED DECEMBER 2010
www.ti.com
This integrated circuit can be damaged by ESD. Texas Instruments recommends that all integrated circuits be handled with
appropriate precautions. Failure to observe proper handling and installation procedures can cause damage.
ESD damage can range from subtle performance degradation to complete device failure. Precision integrated circuits may be more
susceptible to damage because very small parametric changes could cause the device not to meet its published specifications.
ORDERING INFORMATION (1)
SPECIFIED
TEMPERATURE
RANGE
PACKAGE
MARKING
PRODUCT
PACKAGE-LEAD
PACKAGE
DESIGNATOR
VCA810ID
SO-8
D
–40°C to +85°C
VCA810
VCA810AID
SO-8
D
–40°C to +85°C
VCA810A (2)
(1)
(2)
ORDERING
NUMBER
TRANSPORT
MEDIA, QUANTITY
VCA810ID
Rails, 75
VCA810IDR
Tape and Reel, 2500
VCA810AID
Rails, 75
VCA810AIDR
Tape and Reel, 2500
For the most current package and ordering information see the Package Option Addendum at the end of this document, or see the
device product folder at www.ti.com.
The A indicating high grade appears opposite the pin 1 marking indicator.
ABSOLUTE MAXIMUM RATINGS (1)
Over operating free-air temperature range, unless otherwise noted.
Power supply
Internal power dissipation
VCA810
UNIT
±6.5
V
See Thermal Analysis section
Differential input voltage
±VS
Input common-mode voltage range
Storage temperature range, D package
Junction temperature (TJ)
Human body model (HBM)
V
±VS
V
–65 to +125
°C
+150
°C
2000
V
ESD ratings Charge device model (CDM)
1500
V
Machine model
200
V
(1)
Stresses above these ratings may cause permanent damage. Exposure to absolute maximum conditions for extended periods may
degrade device reliability. These are stress ratings only, and functional operation of the device at these or any other conditions beyond
those specified is not implied.
PIN CONFIGURATIONS
D PACKAGE
SO-8
(TOP VIEW)
A
-In
-VS
8
7
+VS VOUT
6
5
(1)
VCA810
1
+In
2
(1)
High grade version indicator.
(2)
NC = Not connected.
2
3
4
GND Gain NC
Control,
VC
(2)
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SBOS275F – JUNE 2003 – REVISED DECEMBER 2010
ELECTRICAL CHARACTERISTICS: VS = ±5V
Boldface limits are tested at +25°C.
At RL = 500Ω, and VIN = single-ended input on V+ with V− at ground,, unless otherwise noted.
VCA810
MIN/MAX OVER
TEMPERATURE
TYP
PARAMETER
CONDITIONS
+25°C
+25°C (2)
0°C to
+70°C (3)
–40°C to
+85°C (3)
UNITS
MIN/
MAX
TEST
LEVEL (1)
AC PERFORMANCE
−2V ≤ VC ≤ 0V
35
30
29
29
MHz
min
B
VO = 2VPP, −2 ≤ VC ≤ −1
35
30
29
29
MHz
min
B
VO < 500mVPP, −2V ≤ VC ≤ 0V
0.1
0.5
0.5
0.5
dB
min
B
VO = 3.5V Step, −2 ≤ VC ≤ −1, 10% to 90%
350
300
300
295
V/ms
min
B
Settling time to 0.01%
VO = 1V Step, −2 ≤ VC ≤ −1
30
40
41
41
ns
min
B
Rise-and-fall time
VO = 1V Step, −2 ≤ VC ≤ −1
10
12
12.1
12.1
ns
min
B
G = 0dB, VC=−1V, f = 5MHz, VO = 500mVPP
6.2
ns
typ
C
VO < 500mVPP, −2V ≤ VC ≤ 0V, f = 5MHz
3.5
ns
typ
C
Second harmonic
VO = 1VPP, f = 1MHz, VC = −1V, G = 0dB
–71
–51
–50
–49
dBc
min
B
Third harmonic
VO = 1VPP, f = 1MHz, VC = −1V, G = 0dB
−35
–34
–32
–29
dBc
min
B
Input voltage noise
VC = −2V
2.4
2.8
3.4
3.5
nV/√Hz
max
B
Input current noise
−2V ≤ VC ≤ 0V
1.4
1.8
2.0
2.1
pA/√Hz
max
B
f ≤ 1MHz, VC > +200mV
−80
−70
dB
max
B
VIN = 2V to 0V, VC = −2V, G = 40dB
100
150
ns
min
B
−2V ≤ VC ≤ 0V
±4
±22
±30
±32
mV
max
A
±125
±125
V/°C
max
B
Both inputs grounded
±0.1
±0.25
±0.30
±0.35
mV
max
A
±1
±1.2
mV/°C
max
B
−12
−14
mA
max
A
±25
±30
nA/°C
max
B
±700
±800
nA
max
A
±1.4
±2.2
nA/°C
max
B
A
Small-signal bandwidth (see Figure 29)
Large-signal bandwidth
Frequency response peaking
Slew rate
Group delay
Group delay variation
Harmonic distortion
Fully attenuated feedthrough
Overdrive recovery
DC PERFORMANCE
Output offset voltage (both inputs
grounded) (4)
Single-ended or differential input
Output offset voltage drift
Input offset voltage (4)
input offset voltage drift
Input bias current
−2V ≤ VC ≤ 0V
−6
–10
Input bias current drift
Input offset current
−2V ≤ VC ≤ 0V
±100
±600
Input offset current drift
INPUT
Common-mode input range
±2.4
±2.3
±2.3
±2.2
V
min
VCM = 0.5V, VC = −2V, Input-referred
95
85
83
80
dB
min
A
VCM = 0V, Single-ended
1|| 1
MΩ || pF
typ
C
VCM = 0V, Differential
> 10 || < 2
MΩ || pF
typ
C
VC = 0V, VCM = 0V
3
VPP
typ
C
VC = −2V, RL = 100Ω
±1.8
±1.7
±1.4
±1.3
V
min
A
VC = −2V, RL = 100Ω
±1.7
±1.6
±1.3
±1.2
V
min
A
Output current
VO = 0V
±60
±40
±35
±32
mA
min
A
Output short-circuit current
VO = 0V
±120
mA
typ
C
VO = 0V, f < 100kHz
0.2
Ω
typ
C
Common-mode rejection ratio
Input impedance
Differential input range (5)
OUTPUT
Voltage output swing
Output impedance
(1)
(2)
(3)
(4)
(5)
Test levels: (A) 100% tested at +25°C. Over temperature limits set by characterization and simulation. (B) Limits set by characterization
and simulation. (C) Typical value; only for information.
Junction temperature = ambient for +25°C tested specifications.
Junction temperature = ambient at low temperature limit; junction temperature = ambient +30°C at high temperature limit for over
temperature specifications.
Total output offset is: (Output Offset Voltage ± Input Offset Voltage x Gain).
Maximum input at minimum gain for < 1dB gain compression.
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VCA810
SBOS275F – JUNE 2003 – REVISED DECEMBER 2010
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ELECTRICAL CHARACTERISTICS: VS = ±5V (continued)
Boldface limits are tested at +25°C.
At RL = 500Ω, and VIN = single-ended input on V+ with V− at ground,, unless otherwise noted.
VCA810
MIN/MAX OVER
TEMPERATURE
TYP
PARAMETER
GAIN CONTROL (VC, Pin 3)
CONDITIONS
+25°C
+25°C (2)
0°C to
+70°C (3)
–40°C to
+85°C (3)
UNITS
MIN/
MAX
TEST
LEVEL (1)
Single-ended or differential input
ΔVC/ΔdB = 25mV/dB
±40
dB
typ
C
Maximum control voltage
G = −40dB
0
V
typ
C
Minimum control voltage
G = +40dB
–2
V
typ
C
−1.8V ≤ VC ≤ −0.2V
±0.4
±1.5
±2.5
±3.5
dB
max
A
VC < −1.8V, VC > −0.2V
±0.5
±2.2
±3.7
±4.7
dB
max
A
−1.8V ≤ VC ≤ −0.2V
±0.02
±0.03
dB/°C
max
B
VC < −1.8V, VC > −0.2V
±0.03
±0.04
dB/°C
max
B
db/V
typ
C
Specified gain range
Gain accuracy
Gain drift
Gain control slope
–40
Gain control linearity (6)
−1.8V ≤ VC ≤ 0V
±0.3
±1
±1.1
±1.2
dB
max
A
VC < −1.8V
±0.7
±1.6
±2.5
±3.2
dB
max
A
25
20
19
19
MHz
min
B
dB/ns
typ
C
Gain control bandwidth
Gain control slew rate
80dB Gain Step
900
Gain settling time
1%, 80dB Step
0.8
ms
typ
C
Input bias current
VC = −1V
–1.5
–3.5
–4.5
–8
mA
max
A
Gain + Power-supply rejection ratio
VC = −2V, G = +40dB, +VS = 5V ±0.5V
0.5
1.5
1.8
2
dB/V
max
A
Gain – Power-supply rejection ratio
VC = −2V, G = +40dB, –VS = –5V ±0.5V
0.7
1.5
1.8
2
dB/V
max
A
V
typ
C
Minimum operating voltage
±4
±4
±4
V
min
A
Maximum operating voltage
±6
±6
±6
V
max
A
POWER SUPPLY
Specified operating voltage
±5
Positive supply quiescent current
Maximum quiescent current
+VS = +5V, G = −40dB
10
12.5
12.6
12.7
mA
min
A
Minimum quiescent current
+VS = +5V, G = −40dB
10
7.5
7.2
7.1
mA
max
A
Maximum quiescent current
+VS = +5V, G = +40dB
18
20.5
22
22.3
mA
min
A
Minimum quiescent current
+VS = +5V, G = +40dB
18
15.5
14.5
13.5
mA
max
A
Maximum quiescent current
−VS = −5V, G = −40dB
12
14.5
14.6
14.7
mA
max
A
Minimum quiescent current
−VS = −5V, G = −40dB
12
9.5
9.4
9.3
mA
min
A
Maximum quiescent current
−VS = −5V, G = +40dB
20
22.5
24.5
24.8
mA
max
A
Minimum quiescent current
−VS = −5V, G = +40dB
20
17.5
16.5
16
mA
min
A
Positive power-supply rejection ratio (+PSRR)
Input-referred, VC = −2V
90
75
75
73
dB
min
A
Negative power-supply rejection ratio
(–PSRR)
Input-referred, VC = −2V
85
70
70
68
dB
min
A
–40 to +85
°C
typ
C
80
°C/W
typ
C
Negative supply quiescent current (7)
THERMAL CHARACTERISTICS
Specified operating range, ID package
Thermal resistance, q JA
D
(6)
(7)
4
SO-8
Junction-to-ambient
Maximum deviation from best line fit.
Magnitude.
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SBOS275F – JUNE 2003 – REVISED DECEMBER 2010
HIGH GRADE DC SPECIFICATIONS: VS = ±5V (VCA810AID)
Boldface limits are tested at +25°C.
At RL = 500Ω, and VIN = single-ended input on V+ with V− at ground,, unless otherwise noted.
VCA810AID
MIN/MAX OVER
TEMPERATURE
TYP
PARAMETER
CONDITIONS
DC PERFORMANCE
Single-ended or differential input
Output offset voltage
−2V < VC < 0V
+25°C
+25°C (2)
0°C to
+70°C (3)
–40°C to
+85°C (3)
UNITS
MIN/
MAX
TEST
LEVEL (1)
±4
±14
±24
±26
mV
max
A
Input offset voltage
±0.1
±0.2
±0.25
±0.3
mV
max
A
Input offset current
±100
±500
±600
±700
mA
max
A
GAIN CONTROL (VC, Pin 3)
Single-ended or differential input
−1.8V ≤ VC ≤ −0.2V
±0.4
±0.9
±1.9
±2.9
dB
max
A
VC < −1.8V, VC > −0.2V
±0.5
±1.5
±3.0
±4.0
dB
max
A
−1.8V ≤ VC ≤ 0V
±0.3
±0.6
±0.7
±0.8
dB
max
A
VC < −1.8V
±0.7
±1.1
±1.9
±2.7
dB/V
max
A
Maximum quiescent current
+VS = +5V, G = −40dB
10
11.5
11.6
11.7
mA
min
A
Minimum quiescent current
+VS = +5V, G = −40dB
10
8.5
8.2
8.1
mA
max
A
Maximum quiescent current
+VS = +5V, G = +40dB
18
19.5
21
21.3
mA
min
A
Minimum quiescent current
+VS = +5V, G = +40dB
18
16.5
15.5
14.5
mA
max
A
Maximum quiescent current
−VS = −5V, G = −40dB
12
14
14.1
14.2
mA
min
A
Minimum quiescent current
−VS = −5V, G = −40dB
12
10
9.9
9.8
mA
max
A
Maximum quiescent current
−VS = −5V, G = +40dB
20
22
24
24.3
mA
min
A
Minimum quiescent current
−VS = −5V, G = +40dB
20
18
17
16.5
mA
max
A
Gain accuracy
Gain control linearity (4)
POWER SUPPLY
Positive supply quiescent current
Negative supply quiescent current (5)
(1)
(2)
(3)
(4)
(5)
Test levels: (A) 100% tested at +25°C. Over temperature limits set by characterization and simulation. (B) Limits set by characterization
and simulation. (C) Typical value; only for information.
Junction temperature = ambient for +25°C tested specifications.
Junction temperature = ambient at low temperature limit; junction temperature = ambient +30°C at high temperature limit for over
temperature specifications.
Maximum deviation from best line fit.
Magnitude.
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TYPICAL CHARACTERISTICS: VS = ±5V
At RL = 500Ω and VIN = single-ended input on V+ with V− at ground, unless otherwise noted.
SMALL−SIGNAL FREQUENCY RESPONSE
GAIN CONTROL FREQUENCY RESPONSE
60
3
Gain (dB)
20
RL = 500W
VIN = 10mVPP, VOUT = 1VPP
0
VIN = 100mVPP, VOUT = 1VPP
-3
Gain (dB)
40
VIN = 1VPP, VOUT = 1VPP
0
VOUT = 2VPP, VIN = 200mVPP
-6
-9
-20
-12
VOUT = 2VPP, VIN = 20mVPP
-40
-15
-60
VC = -1VDC + 10mVPP
-18
1
10
100
1000
1
10
Frequency (MHz)
Figure 1.
Figure 2.
ATTENUATED PULSE RESPONSE
HIGH GAIN PULSE RESPONSE
0.6
150
G = +40dB
VIN = 2VPP
G = -20dB
50
G = -40dB
0
-50
0.2
G = +20dB
0
-0.2
-0.4
-100
-0.6
-150
Time (20ns/div)
Time (20ns/div)
Figure 3.
Figure 4.
GAIN CONTROL PULSE RESPONSE
1.2
GAIN vs CONTROL VOLTAGE
60
G = 0dB to -40dB, VIN = 1VDC
Specified Operating Range
40
1.0
20
0.8
Gain (dB)
Output Voltage (V)
VIN = 10mVPP
0.4
Output Voltage (V)
Output Voltage (mV)
100
100
Frequency (MHz)
0.6
0.4
0.2
0
-20
-40
Output Disabled for
+0.15V £ VC £ +2V
-60
0
G = 0dB to +40dB, VIN = 10mVDC
-0.2
-80
-100
Time (20ns/div)
0.5
0
-0.5
-1.0
-1.5
-2.0
-2.5
Control Voltage, VC (V)
Figure 5.
6
Figure 6.
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TYPICAL CHARACTERISTICS: VS = ±5V (continued)
At RL = 500Ω and VIN = single-ended input on V+ with V− at ground, unless otherwise noted.
HARMONIC DISTORTION vs FREQUENCY
VO = 1VPP
RL = 500W
Harmonic Distortion (dBc)
-35
HARMONIC DISTORTION vs RLOAD
-20
G = 0dB, Third Harmonic
G = 0dB, Third Harmonic
Harmonic Distortion (dBc)
-30
-40
-45
-50
G = +40dB, Third Harmonic
-55
G = +40dB, Second Harmonic
-60
-65
-70
-30
-40
G = +40dB, Third Harmonic
-50
-60
G = +40dB, Second Harmonic
f = 1MHz
VO = 1VPP
RL = 500W
-70
G = 0dB, Second Harmonic
-75
G = 0dB, Second Harmonic
-80
0.1
1
10
100
1000
Frequency (MHz)
Load (W)
Figure 7.
Figure 8.
HARMONIC DISTORTION vs OUTPUT VOLTAGE
f = 1MHz
RL = 500W
Harmonic Distortion (dBc)
-30
HARMONIC DISTORTION vs GAIN
-20
G = 0dB, Third Harmonic
Harmonic Distortion (dBc)
-20
-40
G = +40dB, Second Harmonic
-50
-60
-70
-80
G = +40dB, Third Harmonic
-90
Third Harmonic
-40
-50
-60
Second Harmonic
-70
G = 0dB, Second Harmonic
-100
-80
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
0
1
5
10
15
Figure 9.
35
40
HARMONIC DISTORTION vs ATTENUATION
Output
Limited
Max Useful
Input Voltage Range
Max Useful
Output Voltage
Range
0.1
Resulting
Output Voltage
30
-20
Harmonic Distortion (dBc)
Input/Output Voltage (VPP)
Input
Limited
25
Figure 10.
INPUT/OUTPUT RANGE vs GAIN
10
20
Gain (dB)
Output Voltage (VPP)
1
f = 1MHz
VO = 1VPP
RL = 500W
-30
Resulting
Input Voltage
f = 1MHz
VIN = 1VPP
RL = 500W
-30
Third Harmonic
-40
-50
-60
Second Harmonic
-70
Input and Output Measured at 1dB Compression
-80
0.01
-40
-30
-20
-10
0
10
20
30
40
-40
-35
-30
-25
-20
-15
-10
-5
0
Attenuation (dB)
Gain (dB)
Figure 11.
Figure 12.
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TYPICAL CHARACTERISTICS: VS = ±5V (continued)
At RL = 500Ω and VIN = single-ended input on V+ with V− at ground, unless otherwise noted.
NOISE DENSITY vs CONTROL VOLTAGE
10000
Input-Referred Voltage Noise Density
INPUT VOLTAGE AND CURRENT NOISE
10
RS = 20W
on Each Input
en (nV/?Hz)
in (pA/?Hz)
en (nV/?Hz)
eO (nV/?Hz)
1000
100
Differential Input
Voltage Noise (2.4nV/ÖHz)
Output-Referred Voltage Noise Density
10
Current Noise (1.8pA/ÖHz)
Each Input
1
1
0
100
-0.2 -0.4 -0.6 -0.8 -1.0 -1.2 -1.4 -1.6 -1.8 -2.0
1k
10k
100k
1M
Control Voltage (V)
Frequency (Hz)
Figure 13.
Figure 14.
FULLY ATTENUATED ISOLATION vs FREQUENCY
OUTPUT OFFSET VOLTAGE
TOTAL ERROR BAND vs GAIN
0
10M
50
40
Output Offset Error (mV)
-20
Isolation (dB)
VC = +0.1V
-40
-60
VC = +0.2V
-80
-100
30
Maximum Error Band
20
10
Typical Devices
0
-10
-20
-30
-40
-120
-50
1M
10M
100M
-40
-30
-20
-10
Frequency (Hz)
Figure 15.
TYPICAL GAIN ERROR PLOT
20
30
40
OUTPUT OFFSET VOLTAGE DISTRIBUTION
250
Deviation from -40dB/V Gain Slope
Total Tested = 1462
G = +40dB
200
0.2
0.1
0
Count
Gain Error (dB)
10
Figure 16.
0.4
0.3
0
Gain (dB)
-0.1
150
100
-0.2
-0.3
50
-0.4
0
-0.5
-1
Control Voltage (V)
-1.5
-2
<-50
<-45
<-40
<-35
<-30
<-25
<-20
<-15
<-10
<-5
<0
<5
<10
<15
<20
<25
<30
<35
<40
<45
<50
>50
0
-0.5
Output Offset Voltage (mV)
Figure 17.
8
Figure 18.
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TYPICAL CHARACTERISTICS: VS = ±5V (continued)
At RL = 500Ω and VIN = single-ended input on V+ with V− at ground, unless otherwise noted.
GROUP DELAY vs GAIN
GROUP DELAY vs FREQUENCY
10
10
9
8
8
Group Delay (ns)
Group Delay (ns)
VO = 1VPP
RL = 500W
VO = 1VPP
RL = 500W
1MHz
7
6
5MHz
5
G = 0dB
6
G = +40dB
4
2
10MHz
4
0
-40
-30
-20
0
-10
10
20
30
1
40
Figure 19.
Figure 20.
OVERDRIVE RECOVERY AT MAXIMUM GAIN
OVERDRIVE RECOVERY AT MAXIMUM ATTENUATION
15
VOUT
1.5
1.0
10x VIN
0.5
0
-0.5
-1.0
-1.5
5
VIN
0
200
-5
-10
-15
-20
-2.0
-25
-2.5
Time (100ns/div)
Time (100ns/div)
Figure 21.
Figure 22.
COMMON−MODE REJECTION RATIO AND
POWER−SUPPLY REJECTION RATIO vs GAIN
COMMON−MODE REJECTION RATIO AND
POWER−SUPPLY REJECTION RATIO vs FREQUENCY
110
Input-Referred
100
90
80
CMRR (dB)
PSRR (dB)
70
60
50
PSRR
40
CMRR,
G = ±40dB
90
CMRR
80
CMRR (dB)
PSRR (dB)
VOUT
10
Input/Output Voltage (mV)
Input/Output Voltage (V)
2.0
100
100
Frequency (MHz)
2.5
110
10
Gain (dB)
70
60
50
30
30
20
20
10
10
0
CMRR,
G = 0dB
40
PSRR, G = 0dB
PSRR,
G = +40dB
0
-40
-30
-20
-10
0
10
20
30
40
0.1
Gain (dB)
1
10
100
Frequency (MHz)
Figure 23.
Figure 24.
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TYPICAL CHARACTERISTICS: VS = ±5V (continued)
At RL = 500Ω and VIN = single-ended input on V+ with V− at ground, unless otherwise noted.
GAIN CONTROL −PSRR AT MAX GAIN
6
5
5
4
4
Gain (dB)
Gain (dB)
GAIN CONTROL +PSRR AT MAX GAIN
6
3
2
2
1
1
0
0
1k
10k
100k
1M
10M
100M
1k
Figure 26.
20
20
19
10
8
5
6
0
4
-5
10x Input Offset Current (IOS)
17
16
14
13
-10
0
-15
11
-20
10
0
25
50
75
100
125
Quiescent Current
for -VS
15
2
-2
12
Quiescent Current
for +VS
0
-0.5
-1.0
-1.5
-2.0
Control Voltage (V)
Temperature (°C)
Figure 27.
10
100M
18
Supply Current (mA)
Input Bias Current (IB)
Output Offset Voltage (mA)
10
10M
TYPICAL SUPPLY CURRENT vs CONTROL VOLTAGE
25
15
-25
1M
Figure 25.
12
-50
100k
Frequency (Hz)
Output Offset Voltage (VOS)
14
10k
Frequency (Hz)
TYPICAL DC DRIFT vs TEMPERATURE
16
Input Bias and Offset Current (mA)
3
Figure 28.
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APPLICATION INFORMATION
CIRCUIT DESCRIPTION
The VCA810 is a high gain adjust range, wideband,
voltage amplifier with a voltage-controlled gain, as
shown in Figure 29. The circuit’s basic voltage
amplifier responds to the control of an internal
gain-control amplifier. At its input, the voltage
amplifier presents the high impedance of a differential
stage, permitting flexible input impedance matching.
To preserve termination options, no internal circuitry
connects to the input bases of this differential stage.
For this reason, the user must provide dc paths for
the input base currents from a signal source, either
through a grounded termination resistor or by a direct
connection to ground. The differential input stage also
permits rejection of common-mode signals. At its
output, the voltage amplifier presents a low
impedance, simplifying impedance matching. An
open-loop design produces wide bandwidth at all gain
settings. A ground-referenced differential to
single-ended conversion at the output retains the low
output offset voltage.
+5V
6
V+
V-
VCA810
1
8
Gain
Adjust
+
X1
5
Thus, G(dB) varies linearly over the specified −40dB to
+40dB range as VC varies from 0V to −2V. Optionally,
making VC slightly positive (≥ +0.15V) effectively
disables the amplifier, giving greater than 80dB of
signal path attenuation at low frequencies.
Internally, the gain-control circuit varies the amplifier
gain by varying the transconductance, gm, of a bipolar
transistor using the transistor bias current. Varying
the bias currents of differential stages varies gm to
control the voltage gain of the VCA810. A gm-based
gain adjust normally suffers poor thermal stability.
The VCA810 includes circuitry to minimize this effect.
VCA810 OPERATION
Figure 30 shows the circuit configuration used as the
basis of the Electrical Characteristics and Typical
Characteristics. Voltage swings reported in the
specifications are taken directly at the input and
output pins. For test purposes, the input impedance is
set to 50Ω with a resistance to ground. A 25Ω
resistance (RT) is included on the V− input to get bias
current cancellation. Proper supply bypassing is
shown in Figure 30, and consists of two capacitors on
each supply pin: one large electrolytic capacitor
(2.2mF to 6.8mF), effective at lower frequencies, and
one
small
ceramic
capacitor
(0.1mF)
for
high-frequency decoupling. For more information on
decoupling, refer to the Board Layout section.
VOUT
+5V -5V
2
VC
0.1mF
0.1mF
6.8mF
+
6.8mF
+
3
0 ® -2V
-40dB ® +40dB Gain
7
-5V
Figure 29. Block Diagram of the VCA810
A gain control voltage, VC, controls the amplifier gain
magnitude through a high-speed control circuit. Gain
polarity can be either inverting or noninverting,
depending upon the amplifier input driven by the input
signal. The gain control circuit presents the high-input
impedance of a noninverting op amp connection. The
control voltage pin is referred to ground as shown in
Figure 29. The control voltage VC varies the amplifier
gain according to the exponential relationship:
G(V/V) = 10
1
VI
50W
Source
RS
50W
8
RT
25W
6
7
2
VCA810
5
3
VO
RL
500W
RC
VC
Figure 30. Variable Gain, Specification and Test
Circuit
-2 (VC + 1)
This translates to the log gain relationship:
G(dB) = –40 ● (VC + 1)dB.
Notice that both inverting and noninverting inputs are
connected to ground with a resistor (RS and RT).
Matching the dc source impedance looking out of
each input will minimize input offset voltage error.
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RANGE-FINDING TGC AMPLIFIER
The block diagram in Figure 31 illustrates the
fundamental configuration common to pulse-echo
range finding systems. A photodiode preamp
provides an initial gain stage to the photodiode.
20W
OPA657
VCA810
ADC
and DSP
20kW
20W
VC
charging the holding capacitor. This charge drives the
capacitor voltage in a positive direction, reducing the
amplifier gain. R3 and the CH largely determine the
attack time of this AGC correction. Between gain
corrections, resistor R1 charges the capacitor in a
negative direction, increasing the amplifier gain. R1,
R2, and CH determine the release time of this action.
Resistor R2 forms a voltage divider with R1, limiting
the maximum negative voltage developed on CH. This
limit prevents input overload of the VCA810 gain
control circuit.
Figure 33 shows the AGC response for the values
shown in Figure 32.
CF
VC
-VB
0
t
VIN
-2V
Time-Gain Compensated Control Voltage
RSSI
Port
2mV to 2V
100kHz
VO
VCA810
VC
R3
1kW HP5082
OPA820
Figure 31. Typical Range-Finding Application
WIDE-RANGE AGC AMPLIFIER
The voltage-controlled gain feature of the VCA810
makes this amplifier ideal for precision AGC
applications with control ranges as large as 60dB.
The AGC circuit of Figure 32 adds an op amp and
diode for amplitude detection, a hold capacitor to
store the control voltage and resistors R1 through R3
that determine attack and release times. Resistor R4
and capacitor CC phase-compensate the AGC
feedback loop. The op amp compares the positive
peaks of output VO with a dc reference voltage, VR.
Whenever a VO peak exceeds VR, the OPA820
output swings positive, forward-biasing the diode and
12
R1
50kW
R2
50kW
R4
100W
VR
CH
0.1mF
CC
47pF
0.1 VDC
V-
Figure 32. 60dB Input Range AGC
0.15
Output Voltage (50mV/div)
The control voltage VC varies the amplifier gain for a
basic signal-processing requirement: compensation
for distance attenuation effects, sometimes called
time-gain
compensation
(TGC).
Time-gain
compensation increases the amplifier gain as the
signal moves through the air to compensate for signal
attenuation. For this purpose, a ramp signal applied
to the VCA810 gain control input linearly increases
the dB gain of the VCA810 with time.
VOUT PEAK = VR
0.10
0.05
VIN = 1VPP
VIN = 100mVPP
0
-0.05
-0.10
VIN = 10mVPP
-0.15
-0.20
Time (5ms/div)
Figure 33. AGC Output Voltage for 100kHz
Sinewave at 10mVPP, 100mVPP, and 1VPP
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STABILIZED WEIN-BRIDGE OSCILLATOR
Adding Wein-bridge feedback to the above AGC
amplifier produces an amplitude-stabilized oscillator.
As Figure 34 shows, this alternative requires the
addition of just two resistors (RW1, RW2) and two
capacitors (CW1, CW2).
Connecting the feedback network to the amplifier
noninverting input introduces positive feedback to
induce oscillation. The feedback factor displays a
frequency dependence due to the changing
impedances of the CW capacitors. As frequency
increases, the decreasing impedance of the CW2
capacitor
increases
the
feedback
factor.
Simultaneously, the decreasing impedance of the
CW1 capacitor decreases this factor. Analysis shows
1
fW =
2
p
R
WCW Hz,
that the maximum factor occurs at
making this the frequency most conducive to
oscillation. At this frequency, the impedance
RW2
300W
CW1
4700pF
magnitude of CW equals RW, and inspection of the
circuit shows that this condition produces a feedback
factor of 1/3. Thus, self-sustaining oscillation requires
a gain of three through the amplifier. The AGC
circuitry establishes this gain level. Following initial
circuit turn-on, R1 begins charging CH negative,
increasing the amplifier gain from its minimum. When
this gain reaches three, oscillation begins at fW; the
continued charging effect of R1 makes the oscillation
amplitude grow. This growth continues until that
amplitude reaches a peak value equal to VR. Then,
the AGC circuit counteracts the R1 effect, controlling
the peak amplitude at VR by holding the amplifier gain
at a level of three. Making VR an ac signal, rather
than a dc reference, produces amplitude modulation
of the oscillator output.
CW2
4700pF
f = 1/2pRW1CW1
RW1 = RW2
CW1 = CW2
RW1
300W
VO
VCA810
VC
VOPEAK = VR
R3
1kW
HP5082
OPA820
R1
50kW
R2
50kW
CH
1mF
R4
100W
VR
0.1 VDC
CC
10pF
V-
Figure 34. Amplitude-Stabilized Oscillator
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LOW-DRIFT WIDEBAND LOG AMP
The VCA810 can be used to provide a 2.5MHz
(–3dB) log amp with low offset voltage and low gain
drift. The exponential gain-control characteristic of the
VCA810
permits
simple
generation
of
a
temperature-compensated
logarithmic
response.
Enclosing the exponential function in an op-amp
feedback path inverts this function, producing the log
response.
Figure
35
shows
the
practical
implementation of this technique. A dc reference
voltage, VR, sets the VCA810 inverting input voltage.
This configuration makes the amplifier output voltage
VOA = −GVR, where G = 10
-2 (VC + 1)
produces log-ratio operation. Either way, the log
term’s argument constrains the polarities of VR and
VIN. These two voltages must be of opposite polarities
to ensure a positive argument. This polarity
combination results when VR connects to the
inverting input of the VCA810. Alternately, switching
VR to the amplifier noninverting input removes the
minus sign of the log term argument. Then, both
voltages must be of the same polarity in order to
produce a positive argument. In either case, the
positive polarity requirement of the argument restricts
VIN to a unipolar range. Figure 36 illustrates these
constraints.
.
5
4
VR
-10mV
VOA = -GVR
3
VC
(
VOL = - 1 +
R1
470W
R1
R2
R2
330W
VOL
OPA820
) 1 + 0.5 Log(-V
Output Voltage (V)
VCA810
IN/VR)
-2
III
0.01
0.1
1
10
100
Figure 36. Test Result for LOG Amp for VR =
−100mV
At equilibrium:
-2 (VC + 1)
(1)
The op amp forces this equality by supplying the gain
R1 · VOL
VC =
R 1 + R2 .
control voltage,
Combining the last two expressions and solving for
VOL yields the circuit’s logarithmic response:
( · 1 + 0.5·log ( - VV (
IN
R
(2)
An examination of this result illustrates several circuit
characteristics. First, the argument of the log term,
−VIN/VR, reveals an option and a constraint. In
Figure 35, VR represents a dc reference voltage.
Optionally, making this voltage a second signal
14
II
I
VIN/VR Voltage Ratio
A second input voltage also influences VOA through
control of gain G. The feedback op amp forces VOA to
equal the input voltage VIN connected at the op amp
inverting input. Any difference between these two
signals drops across R3, producing a feedback
current that charges CC. The resulting change in VOL
adjusts the gain of the VCA810 to change VOA.
R2
R1
-1
-5
0.001
Figure 35. Temperature-Compensated Log
Response
(
0
-4
CC
50pF
VOL = - 1 +
1
-3
R3
100W
VIN
VOA = VIN = -VR · 10
2
The above VOL expression reflects a circuit gain
introduced by the presence of R1 and R2. This feature
adds a convenient scaling control to the circuit.
However, a practical matter sets a minimum level for
this gain. The voltage divider formed by R1 and R2
attenuates the voltage supplied to the VC terminal by
the op amp. This attenuation must be great enough to
prevent any possibility of an overload voltage at the
VC terminal. Such an overload saturates the VCA810
gain-control circuitry, reducing the amplifier’s gain.
For the feedback connection of Figure 35, this
overload condition permits a circuit latch. To prevent
this, choose R1 and R2 to ensure that the op amp
cannot possibly deliver a more negative input than
−2.5V to the VC terminal.
Figure 36 exhibits three zones of operation described
below:
Zone I: VC > 0V. The VCA810 is operating in full
attenuation (−80dB). The noninverting input of the
OPA820 will see ∼0V. VOL is going to be the
integration of the input signal.
Zone II: −2V < VC < 0V. The VCA810 is in its normal
operating mode, creating the log relationship in
Equation 2.
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Zone III: VC < −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
achieved by using a voltage limiting amplifier.
LOW-DRIFT, WIDEBAND EXPONENTIAL AMP
A common use of the log amp above involves signal
compounding.
The
inverse
function,
signal
expanding, requires an exponential transfer function.
The VCA810 produces this latter response directly,
as shown in Figure 37. DC reference VR again sets
the amplifier input voltage, and the input signal VIN
now drives the gain control point. Resistors R1 and R2
attenuate this drive to prevent overloading the gain
control input. Setting these resistors at the same
values as in the preceding log amp produces an
exponential amplifier with the inverse function of the
log amp.
VR
-10mV
VCA810
VOL = -VR x 10
+0.5V
VI
R2
330W
-2
(
VOLTAGE-CONTROLLED LOW-PASS FILTER
In the circuit of Figure 39, the VCA810 serves as the
variable-gain element of a voltage-controlled
low-pass filter. This section discusses how this
implementation expands the circuit voltage swing
capability over that normally achieved with the
equivalent multiplier implementation. The circuit
response pole responds to control voltage VC
according to the relationship in Equation 3:
G
fP =
2pR2C
(3)
where G = 10
With the components shown, the circuit provides a
linear variation of the low-pass cutoff from 300Hz to
1MHz.
R2
330W
(
R1VIN
+1
R1 + R2
VC
C
0.047mF
R1
330W
VI
OPA698
R1
470W
VL
OPA820
-3.4V
500W
-2 (VC + 1)
500W
VOA
VO
VCA810
VIN
Figure 37. Exponential Amplifier
VC
Testing the circuit given in Figure 37 gives the
exponential response shown in Figure 38.
1
VO = - R 2
·
R1
VI
fP =
1
1+s
R 2C 2
G
G
2pR2C
-2 (VC + 1)
Output Voltage (V)
G = 10
0.1
Figure 39. Tunable Low-Pass Filter
0.01
0.001
+3.0
+2.5
+2.0
+1.5
+1.0
+0.5
Input Voltage (V)
Figure 38. Exponential Amplifier Response
0
The response control results from amplification of the
feedback voltage applied to R2. 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
G
fP =
2
p
R2C .
pole at
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For G > 1, the circuit applies a greater voltage to R2,
increasing the feedback current this resistor supplies
to the summing junction of the OPA820. The
increased feedback current produces the same result
as if R2 had been decreased in value in the basic
circuit described above. Decreasing the effective R2
resistance moves the circuit pole to a higher
G
fP =
2
p
R2C response
frequency, producing the
control.
Finite loop gain and a signal-swing limitation set
performance boundaries for the circuit. Both
limitations occur when the VCA810 attenuates, rather
than amplifies, the feedback signal. These two
limitations reduce the circuit’s utility at the lower
extreme of the VCA810 gain range. For −1 ≤ VC ≤ 0,
this amplifier produces attenuating gains in the range
from 0dB to −40dB. This range directly reduces the
net gain in the circuit’s feedback loop, increasing gain
error effects. Additionally, this attenuation transfers
an output swing limitation from the OPA820 output to
the overall circuit’s output. Note that OPA820 output
voltage, VOA, relates to VO through the expression,
VO = G ● VOA. Thus, a G < 1 limits the maximum VO
swing to a value less than the maximum VOA swing.
Figure 40 shows the low-pass frequency for different
control voltages.
3
0
VC = -2V
Gain (dB)
-3
VC = -1.4V
TUNABLE EQUALIZER
A circuit analogous to the above low-pass filter
produces a voltage-controlled equalizer response.
The gain control provided by the VCA810 of
Figure 41 varies this circuit response zero from 1Hz
to 10kHz, according to the relationship of Equation 4:
G
fZ ≈
2pGR1C
(4)
To visualize the circuit’s operation, consider a circuit
condition and an approximation that permit replacing
the VCA810 and R3 with short circuits. First, consider
the case where the VCA810 produces G = 1.
Replacing this amplifier with a short circuit leaves the
operation unchanged. In this shorted state, the circuit
is simply a voltage amplifier with an R-C bypass
around R1. The resistance of this bypass, R3, serves
only to phase-compensate the circuit, and practical
factors make R3 << R1. Neglecting R3 for the
moment, the circuit becomes just a voltage amplifier
with a capacitive bypass of R1. This circuit produces
1
fZ ≈
2
p
R
1C .
a response zero at
Adding the VCA810 as shown in Figure 41 permits
amplification of the signal applied to capacitor C, and
produces voltage control of the frequency fZ.
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 GC. Replacing C with this
effective capacitance value produces the circuit
1
fZ ≈
2
p
R
1GC .
control expression
-6
VC = -1.6V
VC = -1.8V
R1
750W
-9
R2
750W
OPA820
VI
50W
-12
VCA810
-15
10k
100k
1M
VOA
C
2 mF
R3
3W
OPA846
10M
VO
Frequency (Hz)
50W
VC
Figure 40. Voltage-Controlled Low-Pass Filter
Frequency Response
fZ ≈
1
2p(GR1 + R3C)
with G = 10
-2 (VC + 1)
Figure 41. Tunable Equalizer
16
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Another factor limits the high-frequency performance
of the resulting high-pass filter: the finite bandwidth of
the op amp. This limits the frequency duration of the
equalizer response. Limitations such as bandwidth
and stability are clearly shown in Figure 42.
100
AOL
90
G = +40dB
80
Gain (dB)
70
G = +15dB
VOLTAGE-CONTROLLED BAND-PASS
FILTER
The variable gain of the VCA810 also provides
voltage control over the center frequency of a
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:
60
10-(V + 1)
2pRC
C
fO =
50
40
G = -15dB
30
20
G = -40dB
10
0
1
10
100
1k
10k
100k
1M
10M
100M
Frequency (Hz)
Figure 42. Amplifier Noise Gain and AOL for
Different Gain
Other limitations of this circuit are stability versus
VCA810 gain and input signal level for the circuit.
Figure 42 also illustrates these two factors. As the
VCA810 gain increases, the crossover slope between
the AOL curve of the OPA846 and noise gain will be
greater than 20dB/decade, rendering the circuit
unstable. The signal level for high gain of the
VCA810 will meet two limitations: the output voltage
swings of both the VCA810 and the OPA846. The
expression VOA = GVI relates these two voltages.
Thus, an output voltage limit VOAL constrains the input
voltage to VI ≤ VOAL/G.
With the components shown, BW = 50kHz. This
bandwidth provides an integrator response duration
of four decades of frequency for fZ = 1Hz, dropping to
one decade for fZ = 10kHz.
(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:
- s
VO
nRC
=
VI
G
s
s2 + nRC + 2 2
RC
(6)
Evaluation of this response equation reveals a
passband gain of AO = –1, a bandwidth of BW =
- (VC + 1)
1/(2pRC), and a selectivity of Q = n · 10
. Note
that variation of control voltage VC alters Q but not
bandwidth.
The gain provided by the VCA810 restricts the output
swing of the filter. Output signal VO must be
constrained to a level that does not drive the VCA810
output, VOA, into its saturation limit. Note that these
two outputs have voltage swings related by VOA =
GVO. Thus, a swing limit VOAL imposes a circuit output
limit of VOL ≤ VOAL/G.
See Figure 44 for the frequency response for two
different gain conditions of the schematic shown in
Figure 43. In particular, notice the center frequency
shift and the selectivity of Q changing as the gain is
increased.
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VCA810
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C
0.047mF
nR
5kW
nR
5kW
VO
=
VI
VI
R
330W
s
nRC
G
s
s2 + nRC + 2 2
RC
-
10-(V + 1)
2pRC
C
1/2
OPA2822
fO =
VO
C
0.047mF
BW =
50W
R
330W
1/2
OPA2822
VOA
1
2pRC
Q = n·10
-(VC + 1)
VCA810
AO = -1
50W
VC
Figure 43. Tunable Band-Pass Filter
0
-5
-10
Gain (dB)
-15
-20
-25
-30
-35
-40
-45
-50
100
1k
10k
100k
Frequency (Hz)
Figure 44. Tunable Band-Pass Filter Response
18
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DESIGN-IN TOOLS
MACROMODELS AND APPLICATIONS
SUPPORT
DEMONSTRATION BOARDS
A printed circuit board (PCB) is available to assist in
the initial evaluation of circuit performance using the
VCA810. This evaluation board (EVM) is available
free, as an unpopulated PCB delivered with
descriptive documentation. The summary information
for this board is shown in Table 1.
Table 1. EVM Ordering Information
PRODUCT
PACKAGE
BOARD PART
NUMBER
VCA810ID
SO-8
DEM-VCA-SO-1A
LITERATURE
REQUEST
NUMBER
SBOU025
Computer simulation of circuit performance using
SPICE is often useful when analyzing the
performance of analog circuits and systems. This is
particularly true for video and RF amplifier circuits
where parasitic capacitance and inductance can play
a major role in circuit performance. A SPICE model
for the VCA810 is available through the TI web page.
The applications group is also available for design
assistance. The models available from TI predict
typical small-signal ac performance, transient steps,
dc performance, and noise under a wide variety of
operating conditions. The models include the noise
terms found in the electrical specifications of the
relevant product data sheet.
Go to the Texas Instruments website (www.ti.com) to
request an evaluation board through the VCA810
product folder.
OPERATING SUGGESTIONS
INPUT/OUTPUT RANGE
The VCA810’s 80dB gain range allows the user to
handle an exceptionally wide range of input signal
levels. If the input and output voltage range
specifications are exceeded, however, signal
distortion and amplifier overdrive will occur. The
VCA810 maximum input and output voltage range is
best illustrated in the Typical Characteristics plot,
Input/Output Range vs Gain (Figure 11). This chart
plots input and output voltages versus gain in dB.
The maximum input voltage range is the largest at full
attenuation (−40dB) and decreases as the gain
increases. Similarly, the maximum useful output
voltage range increases as the input decreases. We
can distinguish three overloading issues as a result of
the operating mode: high attenuation, mid-range
gain-attenuation, and high gain.
From –40dB to –10dB, gain overdriving the input
stage is the only method to overdrive the VCA810.
Preventing this type of overdrive is achieved by
limiting the input voltage range.
From –10dB to +40dB, overdriving can be prevented
by limiting the output voltage range. There are two
limiting mechanisms operating in this situation. From
–10dB to +10dB, an internal stage is the limiting
factor; from +10dB to +40dB, the output stage is the
limiting factor.
Output overdriving occurs when either the maximum
output voltage swing or output current is exceeded.
The VCA810 high output current of ±60mA ensures
that virtually all output overdrives will be limited by
voltage swing rather than by current limiting. Table 2
summarizes these overdrive conditions.
Table 2. Output Signal Compression
GAIN RANGE
LIMITING
MECHANISM
TO PREVENT, OPERATE
DEVICE WITHIN:
−40dB < G <
−10dB
Input Stage
Overdrive
Input Voltage Range
−10dB < G <
+10dB
Internal Stage
Overdrive
Output Voltage Range
+5dB < G <
+40dB
Output Stage
Overdrive
Output Voltage Range
OVERDRIVE RECOVERY
As shown in the Typical Characteristics plot,
Input/Output Range vs Gain (Figure 11), the onset of
overdrive occurs whenever the actual output begins
to deviate from the ideal expected output. If possible,
the user should operate the VCA810 within the linear
regions shown in order to minimize signal distortion
and overdrive delay time. However, instances of
amplifier overdrive are quite common in automatic
gain control (AGC) circuits, which involve the
application of variable gain to input signals of varying
levels. The VCA810 design incorporates circuitry that
allows it to recover from most overdrive conditions in
200ns or less. Overdrive recovery time is defined as
the time required for the output to return from
overdrive to linear operation, following the removal of
either an input or gain-control overdrive signal. The
overdrive plots for maximum gain and maximum
attenuation are shown in the Typical Characteristics.
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OUTPUT OFFSET ERROR
OFFSET ADJUSTMENT
Several elements contribute to the output offset
voltage error; among them are the input offset
voltage, the output offset voltage, the input bias
current and the input offset current. To simplify the
following analysis, the output offset voltage error is
dependent only on the output-offset voltage of the
VCA810 and the input offset voltage. The output
offset error can then be expressed as Equation 7:
Where desired, the offset of the VCA810 can be
removed as shown in Figure 46. This circuit simply
presents a dc voltage to one of the amplifier inputs to
counteract the offset error voltage. For best offset
performance, the trim adjustment should be made
with the amplifier set at the maximum gain of the
intended application. The offset voltage of the
VCA810 varies with gain as shown in Figure 45,
limiting the complete offset cancellation to one
selected gain. Selecting the maximum gain optimizes
offset performance for higher gains where high
amplification of the offset effects produces the
greatest output offset. Two features minimize the
offset control circuit noise contribution to the amplifier
input circuit. First, making the resistance of R2 a low
value minimizes the noise directly introduced by the
control circuit. This approach reduces both the
thermal noise of the resistor and the noise produced
by the resistor with the amplifier input noise current. A
second noise reduction results from capacitive
bypass of the potentiometer output. This reduction
filters out power-supply noise that would otherwise
couple to the amplifier input.
G
(
(
+ 10 20 · V
dB
VOS = VOSO
(7)
IOS
Where:
• VOS = Output offset error
• VOSO = Output offset voltage
• GdB = VCA810 gain in dB
• VIOS = Input offset voltage
This is shown in Figure 45.
50
Output Offset Error (mV)
40
30
Maximum Error Band
20
10
V+
Typical Devices
R1 VIN
10kW
0
RV
100kW
-10
-20
-30
V-
-40
1 mF
VCA810
R2
10W
VO
VC
-50
-40
-30
-20
-10
0
10
20
30
40
Gain (dB)
Figure 46. Optional Offset Adjustment
Figure 45. Output Offset Error versus Gain
The histogram Output Offset Voltage at Maximum
Gain (Figure 18) in the Typical Characteristics curves
shows the distribution for the output offset voltage at
maximum gain.
20
This filtering action diminishes as the wiper position
approaches either end of the potentiometer, but
practical conditions prevent such settings. Over its full
adjustment range, the offset control circuit produces a
±5mV input offset correction for the values shown.
However, the VCA810 only requires one-tenth of this
range for offset correction, assuring that the
potentiometer wiper will always be near the
potentiometer center. With this setting, the resistance
seen at the wiper remains high, which stabilizes the
filtering function.
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GAIN CONTROL
NOISE PERFORMANCE
The VCA810 gain is controlled by means of a
unipolar negative voltage applied between ground
and the gain control input, pin 3. If use of the output
disable feature is required, a ground-referenced
bipolar voltage is needed. Output disable occurs for
+0.15V ≤ VC ≤ +2V, and produces greater than 80dB
of attenuation. The control voltage should be limited
to +2V in disable mode, and –2.5V in gain mode in
order to prevent saturation of internal circuitry. The
VCA810 gain-control input has a –3dB bandwidth of
25MHz and varies with frequency, as shown in the
Typical Characteristics curves. This wide bandwidth,
although useful for many applications, can allow
high-frequency noise to modulate the gain control
input. In practice, this can be easily avoided by
filtering the control input, as shown in Figure 47. RP
should be no greater than 100Ω so as not to
introduce gain errors by interacting with the gain
control input bias current of 6mA.
The VCA810 offers 2.4nV/√Hz input-referred voltage
noise and 1.8 pA/√Hz input-referred current noise at
a gain of +40dB. The input-referred voltage noise,
and the input-referred current noise terms, combine
to give low output noise under a wide variety of
operating conditions. Figure 48 shows the op amp
noise analysis model with all the noise terms
included. In this model, all noise terms are taken to
be noise voltage or current density terms in either
nV/√Hz or pA/√Hz.
+5V
IBN
*
RS
ERS
4kTRS
IBI
-
*
EO
VC
RT
*
VO
VCA610
VCA810
ENI
-5V
4kTRT
CP
f-3dB =
1
2pRPCP
Figure 48. VCA810 Noise Analysis Model
RP
VC
Figure 47. Control Line Filtering
GAIN CONTROL AND TEEPLE POINT
When the VCA810 control voltage reaches −1.5V,
also referred to as the Teeple point, the signal path
undergoes major changes. From 0V to the Teeple
point, the gain is controlled by one bank of amplifiers:
a low-gain VCA. As the Teeple point is passed, the
signal path is switched to a higher gain VCA. This
gain-stage switching can be seen most clearly in the
Noise Density vs Control Voltage Typical
Characteristics curve (Figure 13). The output-referred
voltage noise density increases proportionally to the
control voltage and reaches a maximum value at the
Teeple point. As the gain increases and the internal
stages switch, the output-referred voltage noise
density drops suddenly and restarts its proportional
increase with the gain.
The total output spot noise voltage can be computed
as the square root of the sum of all squared output
noise voltage contributors. Equation 8 shows the
general form for the output noise voltage using the
terms shown in Figure 48.
EO = G(V/V)·
2
2
2
ENI + (IBIRT) + (IBNRS) + 4kT(RS + RT)
(8)
Dividing this expression by the gain will give the
equivalent input-referred spot-noise voltage at the
noninverting input as shown by Equation 9.
EN =
2
ENI2 + (IBIRT)2 + (IBNRS) + 4kT(RS + RT)
(9)
Evaluating these two equations for the VCA810 circuit
and component values shown in Figure 30
(maximizing gain) will give a total output spot-noise
voltage of 272.3nV√Hz and a total equivalent
input-referred spot-noise voltage of 2.72nV√Hz. This
total input-referred spot-noise voltage is higher than
the 2.4nV√Hz specification for the VCA810 alone.
This reflects the noise added to the output by the
input current noise times the input resistance RS and
RT. Keeping input impedance low is required to
maintain low total equivalent input-referred spot-noise
voltage.
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VCA810
SBOS275F – JUNE 2003 – REVISED DECEMBER 2010
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THERMAL ANALYSIS
The VCA810 will not require heatsinking or airflow in
most applications. Maximum desired junction
temperature would set the maximum allowed internal
power dissipation as described in this section. In no
case should the maximum junction temperature be
allowed to exceed +150°C.
Operating junction temperature (TJ) is given by
Equation 10:
TJ = TA + PD ´ qJA
(10)
The total internal power dissipation (PD) is the sum of
quiescent power (PDQ) and additional power
dissipated in the output stage (PDL) to deliver load
power. Quiescent power is simply the specified
no-load supply current times the total supply voltage
across the part. PDL depends on the required output
signal and load; for a grounded resistive load,
however, it is at a maximum when the output is fixed
at a voltage equal to one-half of either supply voltage
(for equal bipolar supplies). Under this worst-case
condition, PDL = VS.2/(4 ● RL), where RL is the
resistive load.
Note that it is the power in the output stage and not in
the load that determines internal power dissipation.
As a worst-case example, compute the maximum TJ
using an VCA810ID (SO-8 package) in the circuit of
Figure 30 operating at maximum gain and at the
maximum specified ambient temperature of +85°C.
PD = 10V(24.8mA) + 52/(4 ● 500Ω) = 260.5mW
Maximum TJ = +85°C + (0.260W ● +125°C/W)
= 117.6°C
This maximum operating junction temperature is well
below most system level targets. Most applications
will be lower since an absolute worst-case output
stage power was assumed in this calculation of VS/2
which is beyond the output voltage range for the
VCA810.
BOARD LAYOUT
Achieving
optimum
performance
with
a
high-frequency amplifier such as the VCA810
requires careful attention to board layout parasitic and
external component types. Recommendations that
will optimize performance include:
a) Minimize parasitic capacitance to any ac ground
for all of the signal I/O pins. This includes the ground
pin (pin 2). Parasitic capacitance on the output can
cause instability: on both the inverting input and the
noninverting input, it can react with the source
impedance to cause unintentional band limiting. To
22
reduce unwanted capacitance, a window around the
signal I/O pins should be opened in all of the ground
and power planes around those pins. Otherwise,
ground and power planes should be unbroken
elsewhere on the board. Place a small series
resistance (> 25Ω) with the input pin connected to
ground to help decouple package parasitic.
b) Minimize the distance (less than 0.25” or
6.35mm)
from
the
power-supply
pins
to
high-frequency 0.1mF decoupling capacitors. At the
device pins, the ground and power plane layout
should not be in close proximity to the signal I/O pins.
Avoid narrow power and ground traces to minimize
inductance between the pins and the decoupling
capacitors. The power-supply connections should
always be decoupled with these capacitors. Larger
(2.2mF to 6.8mF) decoupling capacitors, effective at
lower frequencies, should also be used on the main
supply pins. These capacitors may be placed
somewhat farther from the device and may be shared
among several devices in the same area of the PCB.
c) Careful selection and placement of external
components will preserve the high-frequency
performance of the VCA810. Resistors should be a
very low reactance type. Surface-mount resistors
work best and allow a tighter overall layout. Metal-film
and carbon composition, axially-leaded resistors can
also provide good high-frequency performance.
Again, keep the leads and PCB trace length as short
as possible. Never use wire-wound type resistors in a
high-frequency application. Since the output pin is the
most sensitive to parasitic capacitance, always
position the series output resistor, if any, as close as
possible to the output pin. Other network
components, such as inverting or noninverting input
termination resistors, should also be placed close to
the package.
d) Connections to other wideband devices on the
board may be made with short direct traces or
through onboard transmission lines. For short
connections, consider the trace and the input to the
next device as a lumped capacitive load. Relatively
wide traces (50mils to 100mils, or 1.27mm to
2.54mm) should be used, preferably with ground and
power planes opened up around them.
e) Socketing a high-speed part like the VCA810 is
not recommended. The additional lead length and
pin-to-pin capacitance introduced by the socket can
create an extremely troublesome parasitic network,
which can make it almost impossible to achieve a
smooth, stable frequency response. Best results are
obtained by soldering the VCA810 onto the board.
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INPUT AND ESD PROTECTION
The VCA810 is built using a very high-speed
complementary bipolar process. The internal junction
breakdown voltages are relatively low for these very
small geometry devices. These breakdowns are
reflected in the Absolute Maximum Ratings table.
All pins on the VCA810 are internally protected from
ESD by means of a pair of back-to-back,
reverse-biased diodes to either power supply, as
shown in Figure 49. These diodes begin to conduct
when the pin voltage exceeds either power supply by
about 0.7V. This situation can occur with loss of the
amplifier power supplies while a signal source is still
present. The diodes can typically withstand a
continuous current of 30mA without destruction. To
ensure long-term reliability, however, diode current
should be externally limited to 10mA whenever
possible.
+VS
ESD Protection diodes internally
connected to all pins.
External
Pin
Internal
Circuitry
-VS
Figure 49. Internal ESD Protection
REVISION HISTORY
NOTE: Page numbers for previous revisions may differ from page numbers in the current version.
Changes from Revision E (August, 2008) to Revision F
Page
•
Updated document format to current standards ................................................................................................................... 1
•
Deleted lead temperature specification from Absolute Maximum Ratings table .................................................................. 2
•
Corrected typo in Figure 30 ................................................................................................................................................ 11
Changes from Revision D (February, 2006) to Revision E
Page
•
Changed rails quantity from 100 to 75. ................................................................................................................................. 2
•
Changed storage temperature minimum value in Absolute Maximum Ratings table from –40°C to –65°C ........................ 2
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PACKAGE OPTION ADDENDUM
www.ti.com
28-Sep-2010
PACKAGING INFORMATION
Orderable Device
Status
(1)
Package Type Package
Drawing
Pins
Package Qty
Eco Plan
(2)
Lead/
Ball Finish
MSL Peak Temp
(3)
Samples
(Requires Login)
VCA810AID
ACTIVE
SOIC
D
8
75
Green (RoHS
& no Sb/Br)
CU NIPDAU Level-2-260C-1 YEAR
Request Free Samples
VCA810AIDG4
ACTIVE
SOIC
D
8
75
Green (RoHS
& no Sb/Br)
CU NIPDAU Level-2-260C-1 YEAR
Request Free Samples
VCA810AIDR
ACTIVE
SOIC
D
8
2500
Green (RoHS
& no Sb/Br)
CU NIPDAU Level-2-260C-1 YEAR
Purchase Samples
VCA810AIDRG4
ACTIVE
SOIC
D
8
2500
Green (RoHS
& no Sb/Br)
CU NIPDAU Level-2-260C-1 YEAR
Purchase Samples
VCA810ID
ACTIVE
SOIC
D
8
75
Green (RoHS
& no Sb/Br)
CU NIPDAU Level-2-260C-1 YEAR
Request Free Samples
VCA810IDG4
ACTIVE
SOIC
D
8
75
Green (RoHS
& no Sb/Br)
CU NIPDAU Level-2-260C-1 YEAR
Request Free Samples
VCA810IDR
ACTIVE
SOIC
D
8
2500
Green (RoHS
& no Sb/Br)
CU NIPDAU Level-2-260C-1 YEAR
Purchase Samples
VCA810IDRG4
ACTIVE
SOIC
D
8
2500
Green (RoHS
& no Sb/Br)
CU NIPDAU Level-2-260C-1 YEAR
Purchase Samples
(1)
The marketing status values are defined as follows:
ACTIVE: Product device recommended for new designs.
LIFEBUY: TI has announced that the device will be discontinued, and a lifetime-buy period is in effect.
NRND: Not recommended for new designs. Device is in production to support existing customers, but TI does not recommend using this part in a new design.
PREVIEW: Device has been announced but is not in production. Samples may or may not be available.
OBSOLETE: TI has discontinued the production of the device.
(2)
Eco Plan - The planned eco-friendly classification: Pb-Free (RoHS), Pb-Free (RoHS Exempt), or Green (RoHS & no Sb/Br) - please check http://www.ti.com/productcontent for the latest availability
information and additional product content details.
TBD: The Pb-Free/Green conversion plan has not been defined.
Pb-Free (RoHS): TI's terms "Lead-Free" or "Pb-Free" mean semiconductor products that are compatible with the current RoHS requirements for all 6 substances, including the requirement that
lead not exceed 0.1% by weight in homogeneous materials. Where designed to be soldered at high temperatures, TI Pb-Free products are suitable for use in specified lead-free processes.
Pb-Free (RoHS Exempt): This component has a RoHS exemption for either 1) lead-based flip-chip solder bumps used between the die and package, or 2) lead-based die adhesive used between
the die and leadframe. The component is otherwise considered Pb-Free (RoHS compatible) as defined above.
Green (RoHS & no Sb/Br): TI defines "Green" to mean Pb-Free (RoHS compatible), and free of Bromine (Br) and Antimony (Sb) based flame retardants (Br or Sb do not exceed 0.1% by weight
in homogeneous material)
(3)
MSL, Peak Temp. -- The Moisture Sensitivity Level rating according to the JEDEC industry standard classifications, and peak solder temperature.
Addendum-Page 1
PACKAGE OPTION ADDENDUM
www.ti.com
28-Sep-2010
Important Information and Disclaimer:The information provided on this page represents TI's knowledge and belief as of the date that it is provided. TI bases its knowledge and belief on information
provided by third parties, and makes no representation or warranty as to the accuracy of such information. Efforts are underway to better integrate information from third parties. TI has taken and
continues to take reasonable steps to provide representative and accurate information but may not have conducted destructive testing or chemical analysis on incoming materials and chemicals.
TI and TI suppliers consider certain information to be proprietary, and thus CAS numbers and other limited information may not be available for release.
In no event shall TI's liability arising out of such information exceed the total purchase price of the TI part(s) at issue in this document sold by TI to Customer on an annual basis.
Addendum-Page 2
PACKAGE MATERIALS INFORMATION
www.ti.com
14-Jul-2012
TAPE AND REEL INFORMATION
*All dimensions are nominal
Device
Package Package Pins
Type Drawing
SPQ
Reel
Reel
A0
Diameter Width (mm)
(mm) W1 (mm)
B0
(mm)
K0
(mm)
P1
(mm)
W
Pin1
(mm) Quadrant
VCA810AIDR
SOIC
D
8
2500
330.0
12.4
6.4
5.2
2.1
8.0
12.0
Q1
VCA810IDR
SOIC
D
8
2500
330.0
12.4
6.4
5.2
2.1
8.0
12.0
Q1
Pack Materials-Page 1
PACKAGE MATERIALS INFORMATION
www.ti.com
14-Jul-2012
*All dimensions are nominal
Device
Package Type
Package Drawing
Pins
SPQ
Length (mm)
Width (mm)
Height (mm)
VCA810AIDR
SOIC
D
8
2500
367.0
367.0
35.0
VCA810IDR
SOIC
D
8
2500
367.0
367.0
35.0
Pack Materials-Page 2
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