TI OPA690

 OPA2890
OP
A2
89
0
OPA
2890
SBOS364A – DECEMBER 2007 – REVISED DECEMBER 2007
Low-Power, Wideband, Voltage-Feedback
OPERATIONAL AMPLIFIER with Disable
FEATURES
1
• FLEXIBLE SUPPLY RANGE:
+3V to +12V Single Supply
±1.5V to ±6V Dual Supplies
• UNITY-GAIN STABLE
• WIDEBAND +5V OPERATION: 90MHz
(G = 2V/V)
• OUTPUT VOLTAGE SWING: ±4.1V
• HIGH SLEW RATE: 400V/µs
• LOW QUIESCENT CURRENT: 1.1mA/ch
• LOW DISABLE CURRENT: 30µA/ch
DESCRIPTION
APPLICATIONS
The low 1.1mA/ch supply current of the OPA2890 is
precisely trimmed at +25°C. This trim, along with low
temperature drift, ensures lower maximum supply
current than competing products. System power may
be reduced further using the optional disable control
pin (MSOP-10 package only). Leaving this disable pin
open, or holding it high, operates the OPA2890
normally. If pulled low, the OPA2890 supply current
drops to less than 30µA/ch while the output goes into
a high-impedance state.
2
•
•
•
•
•
•
•
The OPA2890 represents a major step forward in
unity-gain stable, voltage-feedback op amps. A new
internal architecture provides slew rate and full-power
bandwidth previously found only in wideband,
current-feedback op amps. These capabilities give
exceptional single-supply operation. Using a single
+5V supply, the OPA2890 can deliver a 0.9V to 4.1V
output swing with over 30mA drive current and
210MHz bandwidth. This combination of features
makes the OPA2890 an ideal RGB line driver or
single-supply analog-to-digital converter (ADC) input
driver.
VIDEO LINE DRIVING
xDSL LINE DRIVERS/RECEIVERS
HIGH-SPEED IMAGING CHANNELS
ADC BUFFERS
PORTABLE INSTRUMENTS
TRANSIMPEDANCE AMPLIFIERS
ACTIVE FILTERS
1kW
50W
0V ® 4V
500pF
200W
+5V
+6V
ADS8472
VI
1/2
OPA2890
16W
RELATED
OPERATIONAL AMPLIFIER
PRODUCTS
-6V
200W
SINGLES
750W
0.01mF
16-Bit
1MSPS
SAR ADC
750W
375W
16W
Voltage-feedback amplifier
with disable (1800V/µs)
DUALS
TRIPLES
OPA890
Very low-power
voltage-feedback with disable
+6V
1/2
OPA2890
Low-power voltage-feedback
with disable
OPA2889
OPA690
OPA2690
OPA3690
VREF/2
-6V
500kHz LP
Pole
Low Power, DC-Coupled, Single-to-Differential
Driver for ≤100kHz Inputs
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 © 2007, Texas Instruments Incorporated
OPA2890
www.ti.com
SBOS364A – DECEMBER 2007 – REVISED DECEMBER 2007
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
OPA2890
SO-8
D
–40°C to +85°C
OPA2890
OPA2890
MSOP-10
DGS
–40°C to +85°C
BPQ
(1)
ORDERING
NUMBER
TRANSPORT
MEDIA, QUANTITY
OPA2890ID
Rail, 75
OPA2890IDR
Tape and Reel, 2500
OPA2890IDGST
Tape and Reel, 250
OPA2890IDGSR
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 TI
web site at www.ti.com.
ABSOLUTE MAXIMUM RATINGS (1)
Over operating free-air temperature range, unless otherwise noted.
OPA2890
UNIT
±6.5
V
Power supply
Internal power dissipation
See Thermal Characteristics
Input voltage range
±VS
V
–40 to +125
°C
Lead temperature (soldering, 10s)
+260
°C
Maximum junction temperature (TJ)
+150
°C
Minimum junction temperature: continuous operation, long-term reliability
+140
°C
Human body model (HBM)
2000
V
Charge device model (CDM)
1500
V
Machine model (MM)
200
V
Storage temperature range
ESD Rating:
(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
SO-8
Top View
Out A
2
1
-In A
2
+In A
3
-VS
4
A
B
MSOP-10
Top View
8
+VS
+In A
1
10
-In A
7
Out B
DIS A
2
9
Out A
6
-In B
-VS
3
8
+VS
5
+In B
DIS B
4
7
Out B
+In B
5
6
-In B
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Copyright © 2007, Texas Instruments Incorporated
Product Folder Link(s): OPA2890
OPA2890
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SBOS364A – DECEMBER 2007 – REVISED DECEMBER 2007
ELECTRICAL CHARACTERISTICS: VS = ±5V
At TA = +25°C, RF = 0Ω, G = +1V/V, and RL = 200Ω, unless otherwise noted.
OPA2890ID, IDGS
TYP
MIN/MAX OVER TEMPERATURE
+25°C (2)
0°C to
+70°C (3)
–40°C to
+85°C (3)
100
60
50
45
G = +10V/V, VO = 100mVPP
12
8
7
G > +20V/V
120
90
80
G = +2V/V, VO = 100mVPP
15
PARAMETER
CONDITIONS
+25°C
G = +1V/V, VO = 100mVPP, RF = 0Ω
250
G = +2V/V, VO = 100mVPP
MIN/
MAX
TEST
LEVEL (1)
MHz
typ
C
MHz
min
B
6.5
MHz
min
B
78
MHz
min
B
MHz
typ
C
UNITS
AC PERFORMANCE
Small-signal bandwidth
Gain bandwidth product
Bandwidth for 0.1dB flatness
Peaking at a gain of +1V/V
Large-signal bandwidth
Slew rate
VO < 100mVPP
0.2
dB
typ
C
G = +2V/V, VO = 2VPP
110
MHz
typ
C
G = +2V/V, VO = 2V step
400
V/µs
min
B
0.2V step
3.5
ns
typ
C
G = +1V/V, VO = 2V step
16
ns
typ
C
10
ns
typ
C
Rise-and-fall time
Settling time to 0.02%
Settling time to 0.1%
Harmonic distortion
300
275
270
G = +2V/V, f = 1MHz, VO = 2VPP
2nd harmonic
RL = 200Ω
84
73
69
68
dBc
max
B
RL ≥ 500Ω
100
83
81
80
dBc
max
B
RL = 200Ω
89
84
81
80
dBc
max
B
RL ≥ 500Ω
94
90
87
86
dBc
max
B
Input voltage noise
f > 100kHz
8
9
10
11
nV/√Hz
max
B
Input current noise
f > 100kHz
1
1.3
1.7
1.9
pA/√Hz
max
B
Differential gain
G = +2V/V, VO = 1.4VPP, RL = 150Ω
0.05
%
typ
C
Differential phase
G = +2V/V, VO = 1.4VPP, RL = 150Ω
0.03
°
typ
C
f = 5MHz, Input-referred
–68
dB
typ
C
VO = 0V, RL = 100Ω
62
57
56
54
dB
min
A
VCM = 0V
±2
±5
±6.6
±7.1
mV
max
A
±35
±35
µV/°C
max
B
±1.8
±2
µA
max
A
±5
±6
nA/°C
max
B
±450
±500
nA
max
A
±2.5
±2.5
nA/°C
max
B
3rd harmonic
Channel-to-channel crosstalk
DC PERFORMANCE (4)
Open-loop voltage gain (AOL)
Input offset voltage
Average offset voltage drift
VCM = 0V
Input bias current
VCM = 0V
Average input bias current drift
±0.1
±1.6
VCM = 0V
Input offset current
VCM = 0V
Average input offset current drift
±70
±350
VCM = 0V
INPUT
Common-mode input range (CMIR) (5)
±3.9
±3.8
±3.7
±3.6
V
min
A
VCM = 0V, Input-referred
66
60
57
56
dB
min
A
Differential
VCM = 0V
190 || 0.6
kΩ || pF
typ
C
Common-mode
VCM = 0V
3.2 || 0.9
MΩ || pF
typ
C
Common-mode rejection ratio (CMRR)
Input impedance
OUTPUT
Output voltage swing
No load
±4.0
±3.9
±3.8
±3.7
V
min
A
RL = 100Ω
±3.6
±3.1
±3.05
±2.9
V
min
A
VO = 0V
±40
±35
±33
±30
mA
min
A
Output shorted to ground
±75
mA
typ
C
G = +2V/V, f = 100kHz
0.04
Ω
typ
C
Output current, sourcing, sinking
Peak output current
Closed-loop 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 +4°C at high temperature limit for over
temperature specifications.
Current is considered positive out-of-node. VCM is the input common-mode voltage.
Tested < 3dB below minimum specified CMRR at ±CMIR limits
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Copyright © 2007, Texas Instruments Incorporated
Product Folder Link(s): OPA2890
3
OPA2890
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SBOS364A – DECEMBER 2007 – REVISED DECEMBER 2007
ELECTRICAL CHARACTERISTICS: VS = ±5V (continued)
At TA = +25°C, RF = 0Ω, G = +1V/V, and RL = 200Ω, unless otherwise noted.
OPA2890ID, IDGS
TYP
MIN/MAX OVER TEMPERATURE
+25°C
+25°C (2)
0°C to
+70°C (3)
–40°C to
+85°C (3)
UNITS
MIN/
MAX
VDIS = 0, Both channels
60
110
120
150
µA
max
A
VIN = 1VDC
7
µs
typ
C
Enable time
VIN = 1VDC
200
ns
typ
C
Off isolation
G = +2V/V, f = 5MHz
70
dB
typ
C
4
pF
typ
C
PARAMETER
CONDITIONS
DISABLE (MSOP-10 ONLY)
TEST
LEVEL (1)
Disablelow
Power-down supply current (+VS)
Disable time
Output capacitance in disable
Enable voltage
3.0
3.2
3.4
3.8
V
min
A
Disable voltage
1.4
1.1
1.0
0.8
V
max
A
15
30
35
40
µA
max
A
Control pin input bias current (VDIS)
VDIS = 0V, Each channel
POWER SUPPLY
Specified operating voltage
±5
V
typ
C
Minimum operating voltage
1.5
V
typ
C
Maximum operating voltage
±6.0
±6.0
±6.0
V
max
A
Maximum quiescent current
VS = ±5V, Both channels
2.25
2.4
2.45
2.5
mA
max
A
Minimum quiescent current
VS = ±5V, Both channels
2.25
2.1
2.05
2.0
mA
min
A
+VS = 4.5V to 5.5V
68
60
58
56
dB
min
A
°C
typ
C
Power-supply rejection ratio
(+PSRR)
THERMAL CHARACTERISTICS
A
Specified operating range: D and DGS packages
–40 to +85
Thermal resistance, θJA
Junction-toambient
D
SO-8
100
°C/W
typ
C
DGS
MSOP-10
135
°C/W
typ
C
4
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Copyright © 2007, Texas Instruments Incorporated
Product Folder Link(s): OPA2890
OPA2890
www.ti.com
SBOS364A – DECEMBER 2007 – REVISED DECEMBER 2007
ELECTRICAL CHARACTERISTICS: VS = +5V
At RF = 0Ω, G = +1V/V, and RL = 100Ω, unless otherwise noted.
OPA2890ID, IDGS
TYP
MIN/MAX OVER TEMPERATURE
+25°C (2)
0°C to
+70°C (3)
–40°C to
+85°C (3)
90
55
45
40
G = +10V/V, VO = 100mVPP
12
8
6.8
G > +20V/V
120
85
70
G = +2V/V, VO = 100mVPP
15
PARAMETER
CONDITIONS
+25°C
G = +1V/V, VO = 100mVPP, RF = 0Ω
210
G = +2V/V, VO = 100mVPP
MIN/
MAX
TEST
LEVEL (1)
MHz
typ
C
MHz
min
B
6.3
MHz
min
B
68
MHz
min
B
MHz
typ
C
UNITS
AC PERFORMANCE
Small-signal bandwidth
Gain bandwidth product
Bandwidth for 0.1dB flatness
Peaking at a gain of +1V/V
Large-signal bandwidth
Slew rate
VO < 100mVPP
0.2
dB
typ
C
G = +2V/V, VO = 2VPP
100
MHz
typ
C
G = +2V/V, VO = 2V step
350
V/µs
min
B
0.2V step
3.8
ns
typ
C
G = +1V/V, VO = 2V step
18
ns
typ
C
12
ns
typ
C
Rise-and-fall time
Settling time to 0.02%
Settling time to 0.1%
Harmonic distortion
250
200
175
G = +2V/V, f = 1MHz, VO = 2VPP
2nd harmonic
RL = 200Ω
80
71
68
67
dBc
max
B
RL ≥ 500Ω
87
75
71
70
dBc
max
B
RL = 200Ω
83
79
77
76
dBc
max
B
RL ≥ 500Ω
86
83
81
80
dBc
max
B
Input voltage noise
f > 100kHz
8.1
9.1
10.1
11.1
nV/√Hz
max
B
Input current noise
f > 100kHz
1.1
1.4
1.7
2.0
pA/√Hz
max
B
Differential gain
G = +2V/V, VO = 1.4VPP, RL = 150Ω
0.06
%
typ
C
Differential phase
G = +2V/V, VO = 1.4VPP, RL = 150Ω
0.04
°
typ
C
f = 5MHz, Input-referred
-68
dB
typ
C
VO = VS/2, RL = 100Ω
60
55
54
52
dB
min
A
VCM = VS/2
±2
±5
±6.6
±7.1
mV
max
A
±35
±35
µV/°C
max
B
±1.9
±2.1
µA
max
A
±5
±6
nA/°C
max
B
±500
±550
nA
max
A
±2.5
±2.5
nA/°C
max
B
3rd harmonic
Channel-to-channel crosstalk
DC PERFORMANCE (4)
Open-loop voltage gain (AOL)
Input offset voltage
Average offset voltage drift
VCM = VS/2
Input bias current
VCM = VS/2
Average input bias current drift
±0.1
±1.7
VCM = VS/2
Input offset current
VCM = VS/2
Average input offset current drift
±70
±400
VCM = VS/2
INPUT
Most positive input voltage (5)
+4
+3.8
+3.75
+3.7
V
min
A
Least positive input voltage (5)
+1
+1.2
+1.2
+1.3
V
max
A
VCM = VS/2, Input-referred
65
59
56
55
dB
min
A
Differential
VCM = VS/2
190 || 0.6
kΩ || pF
typ
C
Common-mode
VCM = VS/2
3.2 || 0.9
MΩ || pF
typ
C
Common-mode rejection ratio (CMRR)
Input impedance
OUTPUT
Most positive output voltage
No load
+4.1
+3.9
+3.85
+3.8
V
min
A
RL = 100Ω
+3.9
+3.75
+3.7
+3.65
V
min
A
No load
+0.9
+1.1
+1.15
+1.2
V
max
A
RL = 100Ω
+1.1
+1.35
+1.4
+1.45
V
max
A
VO = VS/2
±35
±30
±28
±25
mA
min
A
Output shorted to ground
±65
mA
typ
C
G = +2V/V, f = 100kHz
0.04
Ω
typ
C
Least positive output voltage
Output current: sourcing, sinking
Short-circuit output current
Closed-loop 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 +2°C at high temperature limit for over
temperature specifications.
Current is considered positive out-of-node. VCM is the input common-mode voltage.
Tested < 3dB below minimum specified CMRR at ±CMIR limits
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Product Folder Link(s): OPA2890
5
OPA2890
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SBOS364A – DECEMBER 2007 – REVISED DECEMBER 2007
ELECTRICAL CHARACTERISTICS: VS = +5V (continued)
At RF = 0Ω, G = +1V/V, and RL = 100Ω, unless otherwise noted.
OPA2890ID, IDGS
TYP
PARAMETER
CONDITIONS
DISABLE (MSOP-10 ONLY)
MIN/MAX OVER TEMPERATURE
+25°C
+25°C (2)
0°C to
+70°C (3)
–40°C to
+85°C (3)
UNITS
MIN/
MAX
TEST
LEVEL (1)
35
90
100
130
µA
max
A
ns
typ
C
Disable low
Power-down supply current (+VS)
VDIS = 0V, Both channels
Disable time
VOUT = 1VDC
Enable time
VOUT = 1VDC
ns
typ
C
Off isolation
G = +2V/V, f = 5MHz
dB
typ
C
pF
typ
C
Output capacitance in disable
Enable voltage
3.0
3.2
3.4
3.8
V
min
A
Disable voltage
1.4
1.1
1.0
0.8
V
max
A
15
30
35
40
µA
max
A
Control pin input bias current (VDIS)
VDIS = 0V, Each channel
POWER SUPPLY
Specified operating voltage
+5
V
typ
C
Minimum operating voltage
+3
V
typ
C
Maximum operating voltage
+12
+12
+12
V
max
A
A
Maximum quiescent current
VS = +5V, Both channels
2.1
2.35
2.4
2.45
mA
max
Minimum quiescent current
VS = +5V, Both channels
2.1
1.85
1.8
1.75
mA
min
A
+VS = 4.5V to 5.5V
65
dB
typ
C
–40 to +85
°C
typ
C
Power-supply rejection ratio
(+PSRR)
THERMAL CHARACTERISTICS
Specified operating range: D and DGS packages
Thermal resistance, θJA
Junction-to-ambient
D
SO-8
100
°C/W
typ
C
DGS
MSOP-10
135
°C/W
typ
C
6
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OPA2890
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SBOS364A – DECEMBER 2007 – REVISED DECEMBER 2007
TYPICAL CHARACTERISTICS: VS = ±5V
At TA = +25°C, G = +2V/V, RF = 750Ω, and RL = 200Ω, unless otherwise noted. See Figure 49.
SMALL-SIGNAL FREQUENCY RESPONSE
LARGE-SIGNAL FREQUENCY RESPONSE
9
3
G = +1V/V
R F = 0W
2VPP
6
-3
3
G = +10V/V
Gain (dB)
Normalized Gain (dB)
0
-6
-9
0
7VPP
-3
G = +5V/V
-12
G = +2V/V
-15
-6
VO = 0.5VPP
RL = 200W
G = +2V/V
-9
-18
1
10
100
1
600
10
Figure 1.
SMALL-SIGNAL PULSE RESPONSE
LARGE-SIGNAL PULSE RESPONSE
4
VO = 500mVPP
G = +2V/V
VO = 5VPP
G = +2V/V
3
Output Voltage (1V/div)
Output Voltage (100mV/div)
400
Figure 2.
400
200
100
0
-100
-200
2
1
0
-1
-2
-3
-300
-4
-400
Time (10ns/div)
Time (10ns/div)
Figure 3.
Figure 4.
VIDEO DIFFERENTIAL GAIN/DIFFERENTIAL PHASE
0.20
-dP
0.18
CHANNEL-TO-CHANNEL CROSSTALK
0.40
-40
0.36
-45
Input-Referred
0.32
0.28
0.12
0.24
0.10
0.20
+dG
0.08
0.16
+dP
0.06
0.12
Differential Phase (°)
-dG
0.14
-50
Crosstalk (dB)
0.16
Differential Gain (%)
100
Frequency (MHz)
Frequency (MHz)
300
1VPP
4VPP
-55
-60
-65
-70
0.04
0.08
0.02
0.04
-75
0
-80
0
1
2
3
4
1
Video Loads
10
100
Frequency (MHz)
Figure 5.
Figure 6.
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OPA2890
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SBOS364A – DECEMBER 2007 – REVISED DECEMBER 2007
TYPICAL CHARACTERISTICS: VS = ±5V (continued)
At TA = +25°C, G = +2V/V, RF = 750Ω, and RL = 200Ω, unless otherwise noted. See Figure 49.
HARMONIC DISTORTION vs LOAD RESISTANCE
1MHz HARMONIC DISTORTION vs SUPPLY VOLTAGE
-75
VO = 2VPP
f = 1MHz
G = +2V/V
-75
Harmonic Distortion (dBc)
Harmonic Distortion (dBc)
-70
2nd Harmonic
-80
-85
3rd Harmonic
-90
VO = 2VPP
RL = 200W
G = +2V/V
-80
2nd Harmonic
-85
3rd Harmonic
-90
-95
-95
100
1k
2.5
4.5
Figure 8.
5.0
5.5
6.0
HARMONIC DISTORTION vs OUTPUT VOLTAGE
-75
-60
Harmonic Distortion (dBc)
VO = 2VPP
RL = 200W
G = +2V/V
-70
-80
2nd Harmonic
-90
3rd Harmonic
-100
RL = 200W
f = 1MHz
G = +2V/V
-80
2nd Harmonic
-85
-90
3rd Harmonic
-95
-110
0.1
1
0.1
10
1
10
Output Voltage Swing (VPP)
Frequency (MHz)
Figure 9.
Figure 10.
HARMONIC DISTORTION vs NONINVERTING GAIN
HARMONIC DISTORTION vs INVERTING GAIN
-70
-65
VO = 2VPP
RL = 200W
f = 1MHz
-75
2nd Harmonic
Harmonic Distortion (dBc)
Harmonic Distortion (dBc)
4.0
Figure 7.
HARMONIC DISTORTION vs FREQUENCY
-80
3rd Harmonic
-85
-90
-95
-70
VO = 2VPP
RL = 200W
f = 1MHz
2nd Harmonic
-75
-80
3rd Harmonic
-85
-90
1
8
3.5
Supply Voltage (±VS)
-50
Harmonic Distortion (dBc)
3.0
Resistance (W)
10
20
-1
-10
Gain (V/V)
Gain (V/V)
Figure 11.
Figure 12.
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SBOS364A – DECEMBER 2007 – REVISED DECEMBER 2007
TYPICAL CHARACTERISTICS: VS = ±5V (continued)
At TA = +25°C, G = +2V/V, RF = 750Ω, and RL = 200Ω, unless otherwise noted. See Figure 49.
LOW-FREQUENCY INVERTING HARMONIC DISTORTION
TWO-TONE, 3RD-ORDER INTERMODULATION SPURIOUS
-90
-30
VO = 2VPP
RL = 500W
G = -1V/V
10MHz
-50
Spurious Point (+dBc)
Harmonic Distortion (dBc)
-95
Load power at matched 50W load.
-40
-100
-105
2nd Harmonic
-60
5MHz
-70
-80
-90
1MHz
-110
-100
3rd Harmonic
-110
-115
1k
10k
100k
1M
-8
-6
-4
Frequency (Hz)
-2
0
2
4
6
8
Single-Tone Load Power (dBm)
Figure 13.
Figure 14.
RECOMMENDED RS vs CAPACITIVE LOAD
FREQUENCY RESPONSE vs CAPACITIVE LOAD
9
100
Gain to Capacitive Load (dB)
RS (W)
G = +2V/V
10
6
CL = 10pF
3
CL = 22pF
CL = 47pF
0
CL = 100pF
-3
VIN
1/2
OPA2890
RS
VOUT
CL
1kW
(1)
750W
-6
750W
NOTE: (1) 1kW is optional.
-9
1
1
10
100
0
1000
20
40
60
80
100 120 140 160 180 200
Frequency (MHz)
Capacitive Load (pF)
Figure 15.
Figure 16.
COMMON-MODE REJECTION RATIO AND POWER-SUPPLY
REJECTION RATIO vs FREQUENCY
INPUT VOLTAGE AND CURRENT NOISE
80
100
-PSRR
CMRR
Voltage Noise (nV/ÖHz)
Current Noise (pA/ÖHz)
CMRR and PSRR (dB)
70
60
+PSRR
50
40
30
20
Voltage Noise (8nV/ÖHz)
10
Current Noise (1pA/ÖHz)
1
10
0
0.1
1k
10k
100k
1M
10M
100M
1
Frequency (Hz)
10
100
1k
10k
100k
1M
Frequency (Hz)
Figure 17.
Figure 18.
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TYPICAL CHARACTERISTICS: VS = ±5V (continued)
At TA = +25°C, G = +2V/V, RF = 750Ω, and RL = 200Ω, unless otherwise noted. See Figure 49.
SUPPLY AND OUTPUT CURRENT vs TEMPERATURE
TYPICAL DC DRIFT OVER TEMPERATURE
150
2.36
Sinking Output Current
2.32
2.28
Sourcing Output Current
42.5
2.24
42.0
2.20
Quiescent Supply Current
41.5
2.16
41.0
2.12
40.5
2.08
40.0
-20
0
20
40
60
80
100
100
0
50
0
-0.4
-50
-0.6
-100
-0.8
-150
-1.0
Input Offset Voltage (VOS)
-1.2
-40
120
-20
0
20
Figure 19.
80
100
120
NONINVERTING OVERDRIVE RECOVERY
0
-2
3
2
1
0
8
4
6
3
4
2
Output Voltage
Left Scale
2
1
0
0
Input Voltage
Right Scale
-2
-1
-4
-2
-6
-3
-8
-1
-4
Time (5ns/div)
Time (10ns/div)
Figure 21.
Figure 22.
CLOSED-LOOP OUTPUT IMPEDANCE vs FREQUENCY
OPEN-LOOP GAIN AND PHASE
100
80
374W
ZO
750W
0.1
0.01
0.001
160
Open-Loop Gain
60
140
50
120
40
100
Open-Loop Phase
30
80
20
60
10
40
0
20
0
-10
1k
10k
100k
1M
10M
100M
Open-Loop Phase (°)
750W
1
180
70
1/2
OPA2890
Open-Loop Gain (dB)
10
Input Voltage (1V/div)
2
VDIS (2V/div)
4
Output Voltage (2V/div)
6
Output Voltage (2V/div)
60
Figure 20.
LARGE-SIGNAL DISABLE/ENABLE RESPONSE
Output Impedance (W)
40
Ambient Temperature (°C)
Ambient Temperature (°C)
100
1k
Frequency (Hz)
10k
100k
1M
10M
100M
1G
Frequency (Hz)
Figure 23.
10
-0.2
Input Bias Current (IB)
-200
2.04
-40
0.2
Input Offset Current (IOS)
Input Offset Voltage (mV)
43.0
Supply Current (mA)
Output Current (mA)
43.5
Input Bias and Offset Current (mA)
44.0
Figure 24.
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SBOS364A – DECEMBER 2007 – REVISED DECEMBER 2007
TYPICAL CHARACTERISTICS: VS = ±5V (continued)
At TA = +25°C, G = +2V/V, RF = 750Ω, and RL = 200Ω, unless otherwise noted. See Figure 49.
DISABLE FEEDTHROUGH
-70
VDIS = 0
Disable Feedthrough (dB)
-75
-80
-85
-90
-95
-100
-105
-110
-115
-120
1
10
100
Frequency (MHz)
Figure 25.
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TYPICAL CHARACTERISTICS: VS = ±5V, Differential
At TA = +25°C, Differential Gain = +2V/V, and RL = 400Ω, unless otherwise noted. See Figure 52.
DIFFERENTIAL SMALL-SIGNAL FREQUENCY RESPONSE
DIFFERENTIAL LARGE-SIGNAL FREQUENCY RESPONSE
3
9
GD = 1V/V
6
VO = 5VPP
GD = 2V/V
-3
3
Gain (dB)
Normalized Gain (dB)
0
-6
-9
GD = 10V/V
-12
-15
-18
1M
VO = 8VPP
-3
VO = 14VPP
-6
GD = 5V/V
RF = 750W
RL = 400W
0
-9
RL = 400W
GD = 2V/V
-12
10M
100M
400M
1
Figure 26.
Figure 27.
DIFFERENTIAL DISTORTION vs LOAD RESISTANCE
200
DIFFERENTIAL DISTORTION vs FREQUENCY
-30
2nd Harmonic
-70
-75
-80
3rd Harmonic
VO = 4VPP
f = 1MHz
GD = 2V/V
-85
VO = 4VPP
RL = 400W
GD = 2V/V
-40
Harmonic Distortion (dBc)
-65
-90
-50
-60
2nd Harmonic
-70
-80
3rd Harmonic
-90
-100
100
1k
1
10
Resistance (W)
20
Frequency (MHz)
Figure 28.
Figure 29.
DIFFERENTIAL DISTORTION vs OUTPUT VOLTAGE
DIFFERENTIAL DISTORTION vs FREQUENCY
-65
-90
2nd Harmonic
-70
Harmonic Distortion (dBc)
Harmonic Distortion (dBc)
100
Frequency (MHz)
-60
Harmonic Distortion (dBc)
10
Frequency (Hz)
RL = 400W
f = 1MHz
GD = 2V/V
-75
-80
-85
-100
RL_DIFF = 1kW
GD = -1V/V
VO = 4VPP
3rd Harmonic
-110
-120
-130
2nd Harmonic
-140
3rd Harmonic
-150
-90
1
12
10
1k
10k
100k
Output Voltage (VPP)
Frequency (Hz)
Figure 30.
Figure 31.
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SBOS364A – DECEMBER 2007 – REVISED DECEMBER 2007
TYPICAL CHARACTERISTICS: VS = +5V
At TA = +25°C, G = +2V/V, RF = 750Ω, and RL = 200Ω, unless otherwise noted. See Figure 49.
NONINVERTING
SMALL-SIGNAL FREQUENCY RESPONSE
NONINVERTING
LARGE-SIGNAL FREQUENCY RESPONSE
3
9
G = +1V/V
R F = 0W
RL = 200W
G = +2V/V
6
1VPP
-3
3
Gain (dB)
Normalized Gain (dB)
0
-6
G = +10V/V
-9
2VPP
0
-3
-12
G = +5V/V
-6
-15
3VPP
G = +2V/V
VO = 500mVPP
-18
-9
1
10
100
500
1
10
Frequency (MHz)
Figure 32.
SMALL-SIGNAL PULSE RESPONSE
LARGE-SIGNAL PULSE RESPONSE
4.1
VO = 0.5VPP
G = +2V/V
VO = 2VPP
G = +2V/V
3.7
Output Voltage (400mV/div)
2.8
Output Voltage (100mV/div)
300
Figure 33.
2.9
2.7
2.6
2.5
2.4
2.3
2.2
3.3
2.9
2.5
2.1
1.7
1.3
2.1
0.9
Time (10ns/div)
Time (10ns/div)
Figure 34.
Figure 35.
RECOMMENDED RS vs CAPACITIVE LOAD
FREQUENCY RESPONSE vs CAPACITIVE LOAD
9
Gain to Capacitive Load (dB)
100
RS (W)
100
Frequency (MHz)
10
CL = 10pF
6
3
CL = 22pF
CL = 100pF
0
-3
CL = 47pF
-6
VIN
1/2
OPA2890
-9
RS
VOUT
CL
1kW
(1)
750W
-12
750W
NOTE: (1) 1kW is optional.
-15
1
1
10
100
1000
0
20
40
60
80
100 120 140 160 180 200
Capacitive Load (pF)
Frequency (MHz)
Figure 36.
Figure 37.
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SBOS364A – DECEMBER 2007 – REVISED DECEMBER 2007
TYPICAL CHARACTERISTICS: VS = +5V (continued)
At TA = +25°C, G = +2V/V, RF = 750Ω, and RL = 200Ω, unless otherwise noted. See Figure 49.
HARMONIC DISTORTION vs LOAD RESISTANCE
5.5
4.0
4.5
3.5
3.5
3.0
Output Voltage
Left Scale
2.5
2.5
Input Voltage
Right Scale
1.5
2.0
0.5
1.5
-0.5
1.0
-70
Harmonic Distortion (dBc)
4.5
Input Voltage (1V/div)
Output Voltage (1V/div)
NONINVERTING OVERDRIVE RECOVERY
6.5
0.5
-1.5
VO = 2VPP
f = 1MHz
G = +2V/V
-75
2nd Harmonic
-80
-85
3rd Harmonic
-90
-95
100
Time (10ns/div)
1k
Resistance (W)
Figure 38.
Figure 39.
HARMONIC DISTORTION vs FREQUENCY
HARMONIC DISTORTION vs OUTPUT VOLTAGE
-75
-60
VO = 2VPP
RL = 200W to VS/2
G = +2V/V
Harmonic Distortion (dBc)
Harmonic Distortion (dBc)
-50
-70
-80
2nd Harmonic
-90
RL = 200W to VS/2
f = 1MHz
G = +2V/V
-80
2nd Harmonic
-85
3rd Harmonic
3rd Harmonic
-100
-90
0.1
1
0.1
10
1
10
Output Voltage Swing (VPP)
Frequency (MHz)
Figure 40.
Figure 41.
TWO-TONE, 3RD-ORDER INTERMODULATION SPURIOUS
-30
Load Power at Matched 50W Load
-40
Intercept Point (dBc)
10MHz
-50
-60
5MHz
-70
-80
1MHz
-90
-100
-8
-7
-6
-5
-4
-3
-2
-1
0
1
2
Single-Tone Load Power (dB)
Figure 42.
14
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SBOS364A – DECEMBER 2007 – REVISED DECEMBER 2007
TYPICAL CHARACTERISTICS: VS = +5V, Differential
At TA = +25°C, Differential Gain = +2V/V, and RL = 400Ω, unless otherwise noted. See Figure 58.
DIFFERENTIAL SMALL-SIGNAL FREQUENCY RESPONSE
DIFFERENTIAL LARGE-SIGNAL FREQUENCY RESPONSE
3
9
GD = 1V/V, RF = 0W
VO = 4VPP
6
GD = 2V/V
-3
3
Gain (dB)
Normalized Gain (dB)
0
-6
-9
GD = 10V/V
-12
-15
-18
1
-3
GD = 5V/V
RF = 750W
RL = 400W
VO = 1VPP
0
RF = 750W
RL = 400W
GD = +2V/V
-6
-9
10
100
300
1
100
Frequency (MHz)
Figure 43.
Figure 44.
DIFFERENTIAL DISTORTION vs LOAD RESISTANCE
200
DIFFERENTIAL DISTORTION vs FREQUENCY
-60
-30
2nd Harmonic
VO = 4VPP
RL = 400W
GD = 2V/V
-40
-65
-70
VO = 4VPP
f = 1MHz
GD = 2V/V
-75
3rd Harmonic
-80
Harmonic Distortion (dBc)
Harmonic Distortion (dBc)
10
Frequency (MHz)
-50
-60
2nd Harmonic
-70
3rd Harmonic
-80
-90
-100
-85
100
1k
0.1
1
Resistance (W)
Figure 45.
20
Figure 46.
DIFFERENTIAL DISTORTION vs OUTPUT VOLTAGE
DIFFERENTIAL DISTORTION vs FREQUENCY
-60
-80
RL = 400W
f = 1MHz
GD = 2V/V
2nd Harmonic
Harmonic Distortion (dBc)
Harmonic Distortion (dBc)
10
Frequency (MHz)
-70
-80
3rd Harmonic
RL_DIFF = 1kW
GD = 1V/V
VO = 4VPP
-85
3rd Harmonic
-90
-100
-110
2nd Harmonic
-120
Shift Phase 180° of Input Signal
-130
-90
0.1
1
10
1
10
100
Output Voltage (VPP)
Frequency (Hz)
Figure 47.
Figure 48.
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APPLICATIONS INFORMATION
WIDEBAND VOLTAGE-FEEDBACK
OPERATION
+5V
+VS
0.1mF
The OPA2890 provides an exceptional combination
of high output power capability in a dual, wideband,
unity-gain stable, voltage-feedback op amp using a
new high slew rate input stage. Typical differential
input stages used for voltage-feedback op amps are
designed to steer a fixed-bias current to the
compensation capacitor, setting a limit to the
achievable slew rate. The OPA2890 uses a new input
stage that places the transconductance element
between two input buffers, using the output currents
as the forward signal. As the error voltage increases
across the two inputs, an increasing current is
delivered to the compensation capacitor. This
configuration provides high slew rate (400V/µs) while
consuming
relatively
low
quiescent
current
(1.12mA/ch). This exceptional full-power performance
comes at the price of a slightly higher input noise
voltage than alternative architectures; however, the
8nV/√Hz input voltage noise for the OPA2890 is
exceptionally low for this type of input stage.
Figure 49 shows the DC-coupled, gain of +2V/V, dual
power-supply circuit configuration used as the basis
of the ±5V Electrical Characteristics and Typical
Characteristics. This illustration is for one channel;
the other channel is connected similarly. For test
purposes, the input impedance is set to 50Ω with a
resistor to ground and the output impedance is set to
200Ω. Voltage swings reported in the Electrical
Characteristics are taken directly at the input and
output pins, while output powers (dBm) are at the
matched 50Ω load. For the circuit of Figure 49, the
total effective load is 200Ω || 1.5kΩ. The disable
control line (MSOP-10 package only) is typically left
open for normal amplifier operation. Two optional
components are included in Figure 49. First, an
additional resistor (350Ω) is included in series with
the noninverting input. Combined with the 25Ω dc
source resistance looking back towards the signal
generator, this resistor gives an input bias current
cancelling resistance that matches the 750Ω source
resistance seen at the inverting input (see the DC
Accuracy and Offset Control section). In addition to
the usual power-supply decoupling capacitors to
ground, a 0.1µF capacitor is also included between
the two power-supply pins. In practical printed circuit
board (PCB) layouts, this optional capacitor typically
improves the 2nd-harmonic distortion performance by
3dB to 6dB.
16
50W Source
VI
6.8mF
+
350W
DIS
VD
50W
VO
1/2
OPA2890
0.1mF
100W
100W Load
RF
750W
RG
750W
+
6.8mF
0.1mF
-VS
-5V
Figure 49. DC-Coupled, G = +2V/V, Bipolar
Supply, Specification and Test Circuit
Figure 50 illustrates the ac-coupled, gain of +2V/V,
single-supply circuit configuration used as the basis
of the +5V Electrical Characteristics and Typical
Characteristics. Though not a rail-to-rail design, the
OPA2890 requires minimal input and output voltage
headroom compared to other very wideband
voltage-feedback op amps. It delivers a 3VPP output
swing on a single +5V supply with greater than
80MHz bandwidth. The key requirement of
broadband single-supply operation is to maintain
input and output signal swings within the usable
voltage ranges at both the input and the output. The
circuit of Figure 50 establishes an input midpoint bias
using a simple resistive divider from the +5V supply
(two 698Ω resistors). Separate bias networks would
be required at each input. The input signal is then
ac-coupled into the midpoint voltage bias. The input
voltage can swing to within 1.5V of either supply pin,
giving a 2VPP input signal range centered between
the supply pins. The input impedance matching
resistor (59Ω) used for testing is adjusted to give a
50Ω input load when the parallel combination of the
biasing divider network is included.
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+5V
+VS
+5V
GD =
0.1mF
+
1/2
OPA2830
6.8mF
698W
0.1mF
50W
698W
59W
RG
RF
RG
RF
DIS
VD
VI
RF
RG
1/2
OPA2890
VIN
VO
200W
RL
VOUT
VS/2
RF
750W
1/2
OPA2830
RG
750W
-5V
0.1mF
Figure 51. Differential Inverting Specification and
Test Circuit
Figure 50. DC-Coupled, G = +2V/V, Single-Supply,
Specification and Test Circuit
+5V
GD = 1 +
2RF
RG
1/2
OPA2830
Again, an additional resistor (50Ω in this case) is
included directly in series with the noninverting input.
This minimum recommended value provides part of
the dc source resistance matching for the
noninverting input bias current. It is also used to form
a simple parasitic pole to roll off the frequency
response at very high frequencies ( > 500MHz) using
the input parasitic capacitance. The gain resistor (RG)
is AC-coupled, giving the circuit a dc gain of +1V/V,
which puts the input dc bias voltage (2.5V) on the
output as well. The output voltage can swing to within
1V of either supply pin while delivering greater than
40mA output current.
RF
VIN
RG
RL
RF
1/2
OPA2830
-5V
Figure 52. Differential Noninverting Specification
and Test Circuit
DIFFERENTIAL OPERATION
Figure 51 shows the inverting differential
configuration used as the basis for the ±5V and +5V
Typical Characteristics. This circuit offers a
combination of excellent distortion with low quiescent
current for frequencies below 100kHz.
The other possibility is to use the OPA2890 in a
differential configuration as shown in Figure 52. This
figure illustrates the differential noninverting
configuration that has the advantage of showing a
high input impedance to any prior stage.
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HIGH-PERFORMANCE DAC
TRANSIMPEDANCE AMPLIFIER
WIDEBAND VIDEO MULTIPLEXING
One common application for video speed amplifiers
that include a disable pin is to wire multiple amplifier
outputs together, then select one of several possible
video inputs to source onto a single line. This simple
wired-OR video multiplexer can be easily
implemented using the OP2890IDGS (MSOP-10
package only), as shown in Figure 54.
High-frequency DDS digital-to-analog converters
(DACs) require a low distortion output amplifier to
retain SFDR performance into real-world loads.
Figure 53 shows a single-ended output drive
implementation. The diagram shows the signal output
current(s) connected into the virtual ground summing
junction(s) of the OPA2890, which is set up as a
transimpedance stage or I-V converter. If the DAC
requires that its outputs terminate to a compliance
voltage other than ground for operation, the
appropriate voltage level may be applied to the
noninverting input of the OPA2890. The dc gain for
this circuit is equal to RF. At high frequencies, the
DAC output capacitance (CD in Figure 53) produces a
zero in the noise gain for the OPA2890 that may
cause peaking in the closed-loop frequency
response. CF is added across RF to compensate for
this noise gain peaking. To achieve a flat
transimpedance frequency response, the pole in each
feedback network should be set to:
1
GBP
=
2pRFCF
4pRFCD
(1)
50W
1/2
OPA2890
High-Speed
DAC
VO = IO RF
RF1
CF1
IO
CD1
RF2
CF2
-IO
CD2
1/2
OPA2890
which gives a cutoff frequency f–3dB of approximately:
GBP
f-3dB =
2pRFCD
50W
-VO = -IO RF
GBP ® Gain Bandwidth
Product (Hz) for the OPA2890
Figure 53. DAC Transimpedance Amplifier
+5V
2kW
VDIS
+5V
305W
DISA
Video 1
1/2
OPA2890
75W
634W
750W
-5V
75W Cable
634W
750W
Video 2
RG-59
75W Load
+5V
305W
82.5W
82.5W
1/2
OPA2890
DISB
75W
2kW
-5V
Figure 54. 2-Channel Video Multiplexer (MSOP-10 package only)
18
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Typically, channel switching is performed either on
sync or retrace time in the video signal. The two
inputs are approximately equal at this point. The
make-before-break disable characteristic of the
OPA2890 ensures that there is always one amplifier
controlling the line when using a wired-OR circuit
such as that shown in Figure 54. Because both inputs
may be on for a short period during the transition
between channels, the outputs are combined through
the output impedance matching resistors (82.5Ω in
this case). When one channel is disabled, its
feedback network forms part of the output impedance
and slightly attenuates the signal in getting out onto
the cable. The gain and output matching resistor are
slightly increased to get a signal gain of +1V/V at the
matched load and provide a 75Ω output impedance
to the cable. The video multiplexer connection (see
Figure 54) also ensures that the maximum differential
voltage across the inputs of the unselected channel
does not exceed the rated ±1.2V maximum for
standard video signal levels.
See the Disable Operation section for the turn-on and
turn-off switching glitches using a 0V input for a
single channel is typically less than ±50mV. Where
two outputs are switched (see Figure 54), the output
line is always under the control of one amplifier or the
other as a result of the make-before-break disable
timing. In this case, the switching glitches for two 0V
inputs drops to less than 20mV.
HIGH-SPEED DELAY CIRCUIT
The OPA2890 makes an ideal amplifier for a variety
of active filter designs. Figure 55 illustrates a circuit
that uses the two amplifiers within the dual OPA2890
to design a two-stage analog delay circuit. For
simplicity, the circuit uses a dual-supply (±5V)
operation, but it can also be modified to operate on a
signal supply. The input to the first filter stage is
driven by the OPA890 as a gain of +2V/V to isolate
the signal input from the filter network.
Each of the two filter stages is a 1st-order filter with a
voltage gain of +1V/V. The delay time through one
filter is given by Equation 2.
tGR0 = 2RC
(2)
For a more accurate analysis of the circuit, consider
the group delay for the amplifiers. For example, in the
case of the OPA2890, the group delay in the
bandwidth from 1MHz to 100MHz is approximately
1.0ns. To account for this delay, modify the transfer
function, which now comes out to be:
tGR = 2 (2RC + TD)
(3)
with TD = (1/360) × (dφ/df) = delay of the op amp
itself. The values of resistors RF and RG should be
equal and low to avoid parasitic effects. If the all-pass
filter is designed for very low delay times, include
parasitic board capacitances to calculate the correct
delay time. Simulating this application using the
PSpice model of the OPA2890 allows this design to
be tuned to the desired performance.
C
VIN
OPA890
1/2
OPA2890
C
1/2
OPA2890
R
750W
750W
VOUT
R
RG
402W
RF
402W
RG
402W
RF
402W
Figure 55. Two-Stage, All-Pass Network
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DIFFERENTIAL RECEIVER/DRIVER
A very versatile application for a dual operational
amplifier is the differential amplifier configuration
shown in Figure 56. With both amplifiers of the
OPA2890 connected for noninverting operation, the
circuit provides a high input impedance, while the
gain can easily be set by just one resistor, RG. When
operated in low gains, the output swing may be
limited as a result of the common-mode input swing
limits of the amplifier itself. An interesting modification
of this circuit is to place a capacitor in series with RG.
Now the dc gain for each side is reduced to +1V/V;
the ac gain follows the standard transfer function of G
= 1 + 2RF/RG. This configuration might be
advantageous for applications processing only a
frequency band that excludes dc or very low
frequencies. An input dc voltage resulting from input
bias currents is not amplified by the ac gain and can
be kept low. This circuit can be used as a differential
line receiver, driver, or as an interface to a differential
input ADC.
50W
VI
1/2
OPA2890
SINGLE-SUPPLY MFB DIFFERENTIAL
ACTIVE FILTER: 2MHz BUTTERWORTH
CONFIGURATION
The active filter circuit illustrated in Figure 58 can be
easily implemented using the OPA2890. In this
configuration, each amplifier of the OPA2890
operates as an integrator. For this reason, this type of
application is also called an infinite gain filter
implementation. A Butterworth filter can be
implemented using the following component ratios:
1
fO =
2´p´R´C
R1 = R2 = 0.65 ´ R
R3 = 0.375 ´ R
C1 = C
C2 = 2 ´ C
The frequency response for a 2MHz Butterworth filter
is shown in Figure 57. One advantage for using this
type of filter is the independent setting of ωo and Q. Q
can be easily adjusted by changing the R3A, B
resistors without affecting ωo.
RO
3
RF
750W
VDIFF = 1 +
RF
750W
RG
50W
1/2
OPA2890
2RF
RG
VI - (-VI)
Gain (dB)
0
-3
-6
RO
-9
-VI
-12
Figure 56. High-Speed Differential Receiver
10k
100k
1M
10M
Frequency (Hz)
Figure 57. Multiple Feedback Filter Frequency
Response
20
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+12V
6kW
50W
VCM
1/2
OPA2890
1000pF
6kW
C1A
128.7pF
R3A
232W
R1A
402W
R2A
402W
C2
257.4pF
VIN
R1B
402W
R2B
402W
R3B
232W
50W
VOUT
C1B
128.7pF
1/2
OPA2890
VCM
Figure 58. Single-Supply, MFB Active Filter, 2MHz LP Butterworth
DESIGN-IN TOOLS
MACROMODELS
DEMONSTRATION FIXTURES
Two printed circuit boards (PCBs) are available to
assist in the initial evaluation of circuit performance
using the OPA2890 in its two package options. Both
of these are offered free of charge as unpopulated
PCBs, delivered with a user’s guide. The summary
information for these fixtures is shown in Table 1.
Table 1. Demonstration Fixtures by Package
PRODUCT
PACKAGE
ORDERING NUMBER
LITERATURE
NUMBER
OPA2890ID
SO-8
DEM-OPA-SO-2A
SBOU003
OPA2890IDG
S
MSOP-10
DEM-OPA-MSOP-2B
SBOU040
Computer simulation of circuit performance using
SPICE is often useful when analyzing the
performance of analog circuits and systems. This
principle is particularly true for video and RF amplifier
circuits where parasitic capacitance and inductance
can have a major effect on circuit performance. A
SPICE model for the OPA2890 (use two OPA890
SPICE models) is available through the Texas
Instruments web page (www.ti.com). This model does
a good job of predicting small-signal ac and transient
performance under a wide variety of operating
conditions. It does not do as well in predicting the
harmonic distortion or dG/dP characteristics. This
model does not attempt to distinguish between the
package types in small-signal ac performance.
The demonstration fixtures can be requested at the
Texas Instruments web site (www.ti.com) through the
OPA2890 product folder.
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OPERATING RECOMMENDATIONS
OPTIMIZING RESISTOR VALUES
Because the OPA2890 is a unity-gain stable,
voltage-feedback op amp, a wide range of resistor
values may be used for the feedback and gain setting
resistors. The primary limits on these values are set
by dynamic range (noise and distortion) and parasitic
capacitance considerations. For a noninverting
unity-gain follower application, the feedback
connection should be made with a 25Ω resistor, not a
direct short. This feedback resistor isolates the
inverting input capacitance from the output pin and
improve the frequency response flatness. Usually, the
feedback resistor value should be between 200Ω and
1.5kΩ. Below 200Ω, the feedback network presents
additional output loading that can degrade the
harmonic distortion performance of the OPA2890.
Above 1.5kΩ, the typical parasitic capacitance
(approximately 0.2pF) across the feedback resistor
can cause unintentional band-limiting in the amplifier
response.
A good rule of thumb is to target the parallel
combination of RF and RG (see Figure 49) to be less
than approximately 400Ω. The combined impedance
RF || RG interacts with the inverting input capacitance,
placing an additional pole in the feedback network
and thus, a zero in the forward response. Assuming a
2pF total parasitic on the inverting node, holding RF ||
RG < 400Ω keeps this pole above 160MHz. By itself,
this constraint implies that the feedback resistor RF
can increase to several kΩ at high gains. This
increase in resistor size is acceptable as long as the
pole formed by RF and any parasitic capacitance
appearing in parallel is kept out of the frequency
range of interest.
BANDWIDTH vs GAIN: NONINVERTING
OPERATION
Voltage-feedback op amps exhibit decreasing
closed-loop bandwidth as the signal gain increases.
In theory, this relationship is described by the Gain
Bandwidth Product (GBP) shown in the Electrical
Characteristics. Ideally, dividing GBP by the
noninverting signal gain (also called the Noise Gain,
or NG) predicts the closed-loop bandwidth. In
practice, this principle only holds true when the phase
margin approaches 90°, as it does in high gain
configurations. At low gains (increased feedback
factors), most amplifiers exhibit a more complex
response with lower phase margin. The OPA2890 is
compensated to give a slightly peaked response in a
noninverting gain of 2V/V (see Figure 49). This
compensation results in a typical gain of +2V/V
bandwidth of 100MHz, far exceeding that predicted
by dividing the 60MHz GBP by 2. Increasing the gain
causes the phase margin to approach 90° and the
22
bandwidth to more closely approach the predicted
value of (GBP/NG). At a gain of +10V/V, the 12MHz
bandwidth shown in the Electrical Characteristics
agrees with that predicted using the simple formula
and the typical GBP of 120MHz.
The frequency response in a gain of +2V/V may be
modified to achieve exceptional flatness simply by
increasing the noise gain to 2.5V/V. One way to
modify the response without affecting the +2V/V
signal gain, is to add an 1.5kΩ resistor across the two
inputs, as illustrated in the circuit of Figure 49. A
similar technique may be used to reduce peaking in
unity-gain (voltage follower) applications. For
example, by using a 750Ω feedback resistor along
with a 750Ω resistor across the two op amp inputs,
the voltage follower response is similar to the gain of
+2V/V response of Figure 50. Reducing the value of
the resistor across the op amp inputs further limits the
frequency response due to increased noise gain.
The OPA2890 exhibits minimal bandwidth reduction
going to single-supply (+5V) operation as compared
with ±5V. This feature arises because the internal
bias control circuitry retains nearly constant quiescent
current as the total supply voltage between the
supply pins changes.
INVERTING AMPLIFIER OPERATION
The OPA2890 is a general-purpose, wideband,
voltage-feedback op amp; therefore, all of the familiar
op amp application circuits are available to the
designer. Inverting operation is one of the more
common
requirements
and
offers
several
performance benefits. See Figure 59 for a typical
inverting configuration where the I/O impedances and
signal gain from Figure 49 are retained in an inverting
circuit configuration.
In the inverting configuration, three key design
considerations must be noted. The first is that the
gain resistor (RG) becomes part of the signal channel
input impedance. If input impedance matching is
desired (which is beneficial whenever the signal is
coupled through a cable, twisted-pair, long PCB
trace, or other transmission line conductor), RG may
be set equal to the required termination value and RF
adjusted to give the desired gain. This consideration
is the simplest approach and results in optimum
bandwidth and noise performance. However, at low
inverting gains, the resultant feedback resistor value
can present a significant load to the amplifier output.
For an inverting gain of –2V/V, setting RG to 50Ω for
input matching eliminates the need for RM but
requires a 100Ω feedback resistor. This consideration
has the interesting advantage that the noise gain
becomes equal to 2V/V for a 50Ω source
impedance—the same as the noninverting circuits
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discussed in the previous section. The amplifier
output, however, now sees the 100Ω feedback
resistor in parallel with the external load. In general,
the feedback resistor should be limited to the 200Ω to
1.5kΩ range. In this case, it is preferable to increase
both the RF and RG values (see Figure 56), and then
achieve the input matching impedance with a third
resistor (RM) to ground. The total input impedance
becomes the parallel combination of RG and RM.
+5V
+
0.1mF
6.8mF
0.1mF
RB
261W
50W
Source
VO
1/2
OPA2890
RO
50W
50W Load
RG
375W
VO
= -2V/V
VI
RF
750W
VI
RM
57.6W
0.1mF
+
6.8mF
-5V
Figure 59. Gain of –2V/V Example Circuit
The second major consideration, touched on in the
previous paragraph, is that the signal source
impedance becomes part of the noise gain equation
and influences the bandwidth. For the example in
Figure 59, the RM value combined in parallel with the
external 50Ω source impedance yields an effective
driving impedance of 50Ω || 57.6Ω = 26.7Ω. This
impedance is added in series with RG for calculating
the noise gain (NG). The resultant NG is 2.86V/V for
Figure 59, as opposed to only 2V/V if RM could be
eliminated as discussed above. Therefore, the
bandwidth is slightly lower for the gain of –2V/V
circuit of Figure 59 than for the gain of +2V/V circuit
of Figure 49.
The third important consideration in inverting amplifier
design is setting the bias current cancellation resistor
on the noninverting input (RB). If this resistor is set
equal to the total dc resistance looking out of the
inverting node, the output dc error (as a result of the
input bias currents) is reduced to [(Input Offset
Current) × RF]. If the 50Ω source impedance is
DC-coupled in Figure 57, the total resistance to
ground on the inverting input is 402Ω.
Combining this resistance in parallel with the
feedback resistor gives the RB = 261Ω used in this
example. To reduce the additional high-frequency
noise introduced by this resistor, it is sometimes
bypassed with a capacitor. As long as RB < 350Ω, the
capacitor is not required because the total noise
contribution of all other terms is less than that of the
op amp input noise voltage. As a minimum, the
OPA2890 requires an RB value of 50Ω to damp out
parasitic-induced peaking—a direct short to ground
on the noninverting input runs the risk of a very
high-frequency instability in the input stage.
DRIVING CAPACITIVE LOADS
One of the most demanding and yet very common
load conditions for an op amp is capacitive loading.
Often, the capacitive load is the input of an
ADC—including additional external capacitance that
may be recommended to improve ADC linearity. A
high-speed, high open-loop gain amplifier such as the
OPA2890 can be very susceptible to decreased
stability and closed-loop response peaking when a
capacitive load is placed directly on the output pin.
When the open-loop output resistance of the amplifier
is considered, this capacitive load introduces an
additional pole in the signal path that can decrease
the phase margin. Several external solutions to this
problem have been suggested. When the primary
considerations are frequency response flatness,
pulse response fidelity, and/or distortion, the simplest
and most effective solution is to isolate the capacitive
load from the feedback loop by inserting a
series-isolation resistor between the amplifier output
and the capacitive load. This solution does not
eliminate the pole from the loop response, but rather
shifts it and adds a zero at a higher frequency. The
additional zero acts to cancel the phase lag from the
capacitive load pole, thus increasing the phase
margin and improving stability.
The Typical Characteristics show the recommended
RS versus capacitive load (see Figure 15 and
Figure 36) and the resulting frequency response at
the load. Parasitic capacitive loads greater than 2pF
can begin to degrade the performance of the
OPA2890. Long PCB traces, unmatched cables, and
connections to multiple devices can easily exceed
this value. Always consider this effect carefully, and
add the recommended series resistor as close as
possible to the OPA2890 output pin (see the Board
Layout Guidelines section).
DISTORTION PERFORMANCE
The OPA2890 provides good distortion performance
into a 100Ω load on ±5V supplies. Relative to
alternative solutions, it provides exceptional
performance into lighter loads and/or operating on a
single +5V supply. Generally, until the fundamental
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signal reaches very high frequency or power levels,
the 2nd harmonic dominates the distortion with a
negligible 3rd harmonic component. Focusing then on
the 2nd harmonic, increasing the load impedance
improves distortion directly. Remember that the total
load includes the feedback network; in the
noninverting configuration (see Figure 49), this value
is the sum of RF + RG, while in the inverting
configuration it is only RF. Also, providing an
additional supply-decoupling capacitor (0.1µF)
between the supply pins (for bipolar operation)
improves the 2nd-order distortion slightly (3dB to
6dB).
Operating
differentially
also
lowers
2nd-harmonic distortion terms (see the plot on the
front page).
In most op amps, increasing the output voltage swing
increases harmonic distortion directly. The output
stage used in the OPA2890 holds the difference
between fundamental power and the 2nd- and
3rd-harmonic powers relatively constant with
increasing output power until very large output swings
are required ( > 4VPP). This also shows up in the
two-tone, 3rd-order intermodulation spurious (IM3)
response curves. The 3rd-order spurious levels are
extremely low at low output power levels. The output
stage continues to hold them low even as the
fundamental power reaches very high levels. As the
Typical
Characteristics
show,
the
spurious
intermodulation powers do not increase as predicted
by a traditional intercept model. As the fundamental
power level increases, the dynamic range does not
decrease significantly. For two tones centered at
10MHz, with 4dBm/tone into a matched 50Ω load
(that is, 1VPP for each tone at the load, which requires
4VPP for the overall two-tone envelope at the output
pin), the Typical Characteristics show a 38dBc
difference between the test tone powers and the
3rd-order intermodulation spurious powers. This
exceptional performance for all 22.5mW internal
power dissipation parts improves further when
operating at lower frequencies or powers.
NOISE PERFORMANCE
High slew rate, unity-gain stable, voltage-feedback op
amps usually achieve the slew rate at the expense of
a higher input noise voltage. However, the 8nV/√Hz
input voltage noise for the OPA2890 is much lower
than that of comparable amplifiers. The input-referred
voltage noise, and the two input-referred current
noise terms, combine to give low output noise under
a wide variety of operating conditions. Figure 60
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.
24
ENI
1/2
OPA2890
RS
EO
IBN
ERS
RF
Ö4kTRS
Ö4kTRF
4kT
RG
RG
IBI
4kT = 1.6E - 20J
at 290°K
Figure 60. Op Amp Noise Analysis Model
The total output spot noise voltage can be computed
as the square root of the sum of all squared output
noise voltage contributors. Equation 4 shows the
general form for the output noise voltage using the
terms shown in Figure 60.
EO =
2
2
2
2
[ENI
+ (IBNRS) + 4kTRS]NG + (IBIRF) + 4kTRFNG
(4)
Dividing this expression by the noise gain (NG = (1 +
RF/RG)) gives the equivalent input-referred spot noise
voltage at the noninverting input, as shown in
Equation 5.
EN =
2
2
( ) + 4kTR
NG
2
ENI
+ (IBNRS) + 4kTRS +
IBIRF
NG
F
(5)
Evaluating these two equations for the OPA2890
circuit and component values (see Figure 49) gives a
total output spot noise voltage of 17.5nV/√Hz and a
total equivalent input spot noise voltage of 8.7nV/√Hz.
This result includes the noise added by the bias
current cancellation resistor (350Ω) on the
noninverting input. This total input-referred spot noise
voltage is only slightly higher than the 8nV/√Hz
specification for the op amp voltage noise alone. This
result is the case as long as the impedances
appearing at each op amp input are limited to the
previously recommend maximum value of 400Ω.
Keeping both (RF || RG) and the noninverting input
source impedance less than 400Ω satisfies both
noise
and
frequency
response
flatness
considerations. Because the resistor-induced noise is
relatively negligible, additional capacitive decoupling
across the bias current cancellation resistor (RB) for
the inverting op amp configuration of Figure 59 is not
required.
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DC ACCURACY AND OFFSET CONTROL
The balanced input stage of a wideband
voltage-feedback op amp allows good output dc
accuracy in a wide variety of applications. The
power-supply current trim for the OPA2890 gives
even tighter control than comparable amplifiers.
Although the high-speed input stage does require
relatively high input bias current (typically 5µA out of
each input terminal), the close matching between
them may be used to reduce the output dc error
caused by this current. The total output offset voltage
may be considerably reduced by matching the dc
source resistances appearing at the two inputs. This
matching reduces the output dc error resulting from
the input bias currents to the offset current times the
feedback resistor. Evaluating the configuration of
Figure 49, and using worst-case +25°C input offset
voltage and current specifications, gives a worst-case
output offset voltage equal to:
±(NG ´ VOS(MAX)) ± (RF ´ IOS(MAX))
= ±(2 ´ 5mV) ± (750W ´ 1.6mA)
= ±11.2mV with -(NG = noninverting signal gain)
A fine-scale output offset null, or dc operating point
adjustment, is often required. Numerous techniques
are available for introducing dc offset control into an
op amp circuit. Most of these techniques eventually
reduce to adding a dc current through the feedback
resistor. In selecting an offset trim method, one key
consideration is the impact on the desired signal path
frequency response. If the signal path is intended to
be noninverting, the offset control is best applied as
an inverting summing signal to avoid interaction with
the signal source. If the signal path is intended to be
inverting, applying the offset control to the
noninverting input may be considered. However, the
dc offset voltage on the summing junction sets up a
dc current back into the source that must be
considered. Applying an offset adjustment to the
inverting op amp input can change the noise gain and
frequency response flatness. For a DC-coupled
inverting amplifier, Figure 61 shows one example of
an offset adjustment technique that has minimal
impact on the signal frequency response. In this
case, the dc offsetting current is brought into the
inverting input node through resistor values that are
much larger than the signal path resistors. This
configuration ensures that the adjustment circuit has
minimal effect on the loop gain and thus, the
frequency response.
+5V
Power-supply
decoupling not shown.
261W
0.1mF
1/2
OPA2890
VO
-5V
RG
375W
+5V
5kW
RF
750W
VI
20kW
±200mV Output Adjustment
10kW
0.1mF
VO
5kW
VI
=-
RF
RG
= -2
-5V
Figure 61. DC-Coupled, Inverting Gain of –2, with
Offset Adjustment
DISABLE OPERATION (MSOP-10 Package
Only)
The OPA2890IDGS provides an optional disable
feature that can be used either to reduce system
power or to implement a simple channel multiplexing
operation. If the DIS control pin is left unconnected,
the OPA2890IDGS operates normally. To disable, the
control pin must be asserted LOW. Figure 62 shows
a simplified internal circuit for the disable control
feature.
+VS
50kW
Q1
200kW
VDIS
2MW
IS
Control
-VS
Figure 62. Simplified Disable Control Circuit
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In normal operation, base current to Q1 is provided
through the 2MΩ resistor, while the emitter current
through the 50kΩ resistor sets up a voltage drop that
is inadequate to turn on the two diodes in the Q1
emitter. As VDIS is pulled LOW, additional current is
pulled through the 50kΩ resistor, eventually turning
on those two diodes (≈30µA). At this point, any
further current pulled out of VDIS goes through those
diodes holding the emitter-base voltage of Q1 at
approximately 0V. This current shuts off the collector
current out of Q1, turning the amplifier off. The supply
currents in the disable mode are only those required
to operate the circuit of Figure 62. Additional circuitry
ensures that turn-on time occurs faster than turn-off
time (make-before-break).
When disabled, the output and input nodes go to a
high-impedance state. If the OPA2890 is operating at
a gain of +1V/V, the device shows a very high
impedance at the output and exceptional signal
isolation. If operating at a gain greater than +1V/V,
the total feedback network resistance (RF + RG)
appears as the impedance looking back into the
output, but the circuit still shows very high forward
and reverse isolation. If configured as an inverting
amplifier, the input and output are connected through
the feedback network resistance (RF + RG) and the
isolation is very poor as a result.
THERMAL ANALYSIS
Operating junction temperature (TJ) is given by TA +
PD × θJA. 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, PDL is
at a maximum when the output is fixed at a voltage
equal to 1/2 of either supply voltage (for equal bipolar
supplies). Under this condition, PDL = VS2/(4 × RL),
where RL includes feedback network loading.
Note that it is the power in the output stage and not
into the load that determines internal power
dissipation.
As a worst-case example, compute the maximum TJ
using an OPA2890ID (SO-8 package) in the circuit of
Figure 49 operating at the maximum specified
ambient temperature of +85°C and with both outputs
driving a grounded 20Ω load to +2.5V.
2
PD = 10V ´ 2.5mA + 2[5 /(4 ´ (75W || 1.5kW))] = 200mW
Maximum TJ = +85°C + (0.2W ´ 125°C/W) = 110°C
This absolute worst-case condition does not exceed
the specified maximum junction temperature. Actual
PDL is normally less than that considered here.
Carefully consider maximum TJ in your application.
Maximum desired junction temperature sets the
maximum allowed internal power dissipation as
described below. In no case should the maximum
junction temperature be allowed to exceed +150°C.
26
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Product Folder Link(s): OPA2890
OPA2890
www.ti.com
SBOS364A – DECEMBER 2007 – REVISED DECEMBER 2007
BOARD LAYOUT GUIDELINES
Achieving
optimum
performance
with
a
high-frequency amplifier such as the OPA2890
requires careful attention to board layout parasitics
and external component types. Recommendations
that optimize performance include:
a) Minimize parasitic capacitance to any ac ground
for all of the signal I/O pins. Parasitic capacitance on
the output and inverting input pins can cause
instability: on the noninverting input, it can react with
the source impedance to cause unintentional
bandlimiting. To 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.
b) Minimize the distance (< 0.25in, or 6.35mm) from
the power-supply pins to high-frequency 0.1µF
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. An optional supply
decoupling capacitor (0.1µF) across the two power
supplies
(for
bipolar
operation)
improves
2nd-harmonic distortion performance. Larger (2.2µF
to 6.8µF) 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 printed circuit
board (PCB).
c) Careful selection and placement of external
components
preserves
the
high-frequency
performance of the OPA2890. Resistors should be
a very low reactance type. Surface-mount resistors
work best and allow a tighter overall layout. Metal film
or carbon composition axially-leaded resistors can
also provide good high-frequency performance.
Again, keep the leads and PCB traces as short as
possible. Never use wirewound type resistors in a
high-frequency application. Because the output pin
and inverting input pin are the most sensitive to
parasitic capacitance, always position the feedback
and series output resistor, if any, as close as possible
to the output pin. Other network components, such as
noninverting input termination resistors, should also
be placed close to the package. Even with a low
parasitic capacitance shunting the external resistors,
excessively high resistor values can create significant
time constants that can degrade performance. Good
axial metal film or surface-mount resistors have
approximately 0.2pF in shunt with the resistor. For
resistor values > 1.5kΩ, this parasitic capacitance
can add a pole and/or zero below 500MHz that can
effect circuit operation. Keep resistor values as low
as
possible
consistent
with
load
driving
considerations. The 750Ω feedback used in the
Electrical Characteristics is a good starting point for
design. Note that a 0Ω feedback resistor is suggested
for the unity-gain follower application.
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. Estimate the
total capacitive load and set RS from the plots of
Figure 15 and Figure 36. Low parasitic capacitive
loads (< 3pF) may not need an RS because the
OPA2890 is nominally compensated to operate with a
2pF parasitic load. Higher parasitic capacitive loads
without an RS are allowed as the signal gain
increases (increasing the unloaded phase margin;
see Figure 61). If a long trace is required, and the
6dB signal loss intrinsic to a doubly-terminated
transmission line is acceptable, implement a matched
impedance transmission line using microstrip or
stripline techniques (consult an ECL design handbook
for microstrip and stripline layout techniques). A 50Ω
environment is normally not necessary on board, and
in fact, a higher impedance environment improves
distortion as shown in the distortion versus load plots.
With a characteristic board trace impedance defined
(based on board material and trace dimensions), a
matching series resistor into the trace from the output
of the OPA2890 is used as well as a terminating
shunt resistor at the input of the destination device.
Remember also that the terminating impedance is the
parallel combination of the shunt resistor and the
input impedance of the destination device; this total
effective impedance should be set to match the trace
impedance.
e) Socketing a high-speed part such as the
OPA2890 is not recommended. The additional lead
length and pin-to-pin capacitance introduced by the
socket can create an extremely troublesome parasitic
network that can make it almost impossible to
achieve a smooth, stable frequency response. Best
results are obtained by soldering the OPA2890 onto
the board.
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Product Folder Link(s): OPA2890
27
OPA2890
www.ti.com
SBOS364A – DECEMBER 2007 – REVISED DECEMBER 2007
INPUT AND ESD PROTECTION
+VCC
The OPA2890 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
device pins are protected with internal ESD protection
diodes to the power supplies, as shown in Figure 63.
These diodes provide moderate protection to input
overdrive voltages above the supplies as well. The
protection diodes can typically support 30mA
continuous current. Where higher currents are
possible (for example, in systems with ±15V supply
parts driving into the OPA2890), current-limiting
series resistors should be added into the two inputs.
Keep these resistor values as low as possible since
high values degrade both noise performance and
frequency response.
28
External
Pin
Internal
Circuitry
-VCC
Figure 63. Internal ESD Protection
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Product Folder Link(s): OPA2890
OPA2890
www.ti.com
SBOS364A – DECEMBER 2007 – REVISED DECEMBER 2007
Revision History
NOTE: Page numbers for previous revisions may differ from page numbers in the current version.
Changes from Original (December, 2007) to Revision A ............................................................................................... Page
•
Corrected CMRR characteristic values.................................................................................................................................. 3
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Product Folder Link(s): OPA2890
29
PACKAGE OPTION ADDENDUM
www.ti.com
17-Dec-2007
PACKAGING INFORMATION
Orderable Device
Status (1)
Package
Type
Package
Drawing
Pins Package Eco Plan (2)
Qty
OPA2890ID
ACTIVE
SOIC
D
8
OPA2890IDGSR
ACTIVE
MSOP
DGS
OPA2890IDGST
ACTIVE
MSOP
OPA2890IDR
ACTIVE
SOIC
75
Lead/Ball Finish
MSL Peak Temp (3)
Green (RoHS &
no Sb/Br)
CU NIPDAU
Level-2-260C-1 YEAR
10
2500 Green (RoHS &
no Sb/Br)
CU NIPDAU
Level-2-260C-1 YEAR
DGS
10
250
Green (RoHS &
no Sb/Br)
CU NIPDAU
Level-2-260C-1 YEAR
D
8
2500 Green (RoHS &
no Sb/Br)
CU NIPDAU
Level-2-260C-1 YEAR
(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.
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 1
PACKAGE MATERIALS INFORMATION
www.ti.com
13-Dec-2007
TAPE AND REEL BOX INFORMATION
Device
Package Pins
Site
Reel
Diameter
(mm)
Reel
Width
(mm)
A0 (mm)
B0 (mm)
K0 (mm)
P1
(mm)
W
Pin1
(mm) Quadrant
OPA2890IDGST
DGS
10
SITE 41
180
12
5.3
3.4
1.4
8
12
Q1
OPA2890IDR
D
8
SITE 41
330
12
6.4
5.2
2.1
8
12
Q1
Pack Materials-Page 1
PACKAGE MATERIALS INFORMATION
www.ti.com
13-Dec-2007
Device
Package
Pins
Site
Length (mm)
Width (mm)
Height (mm)
OPA2890IDGST
DGS
10
SITE 41
184.0
184.0
50.0
OPA2890IDR
D
8
SITE 41
346.0
346.0
29.0
Pack Materials-Page 2
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