Datasheet OPA658N-250, OPA658P, OPA658NB-3K, OPA658U-2K5, OPA658UB-2K5 Datasheet (Burr Brown)

...
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®
OPA658
FEATURES
UNITY GAIN STABLE BANDWIDTH:
900MHz
LOW POWER: 50mW
LOW DIFFERENTIAL GAIN/PHASE ERRORS:
°
HIGH SLEW RATE: 1700V/µs
GAIN FLATNESS: 0.1dB to 135MHz
HIGH OUTPUT CURRENT (80mA)
Wideband, Low Power Current Feedback
OPERATIONAL AMPLIFIER
APPLICATIONS
MEDICAL IMAGING
HIGH-RESOLUTION VIDEO
HIGH-SPEED SIGNAL PROCESSING
COMMUNICATIONS
PULSE AMPLIFIERS
ADC/DAC GAIN AMPLIFIER
MONITOR PREAMPLIFIER
CCD IMAGING AMPLIFIER
OPA658
DESCRIPTION
The OPA658 is an ultra-wideband, low power current feedback video operational amplifier featuring high slew rate and low differential gain/phase error. The current feedback design allows for superior large sig­nal bandwidth, even at high gains. The low differential gain/phase errors, wide bandwidth and low quiescent
current make the OPA658 a perfect choice for numer­ous video, imaging and communications applications.
The OPA658 is optimized for low gain operation and is also available in dual (OPA2658) and quad (OPA4658) configurations.
®
C
COMP
Current Mirror
In
In
+
V
OUT
I
BIAS
I
BIAS
+V
S
–V
S
Current Mirror
Buffer
OPA658
OPA658
International Airport Industrial Park • Mailing Address: PO Box 11400, Tucson, AZ 85734 • Street Address: 6730 S. Tucson Blvd., Tucson, AZ 85706 • Tel: (520) 746-1111 • Twx: 910-952-1111
Internet: http://www.burr-brown.com/ • FAXLine: (800) 548-6133 (US/Canada Only) • Cable: BBRCORP • Telex: 066-6491 • FAX: (520) 889-1510 • Immediate Product Info: (800) 548-6132
© 1994 Burr-Brown Corporation PDS-1268F Printed in U.S.A. March, 1998
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OPA658
FREQUENCY RESPONSE
Closed-Loop Bandwidth
(2)
G = +1
(4)
900
(1)
MHz G = +2 680 400 MHz G = +5 370 MHz
G = +10 200 MHz
Slew Rate
(3)
G = +2, 2V Step 1700 1000 V/µs
At Minimum Specified Temperature 1500 900 V/µs
Settling Time: 0.01% G = +2, 2V Step 15 ns
0.1% G = +2, 2V Step 11.5 ns 1% G = +2, 2V Step 6 ns
Spurious Free Dynamic Range f = 5MHz, G = +2, V
O
= 2Vp-p 68 dBc
f = 20MHz, G= +2, V
O
= 2Vp-p 56 dBc Third Order Intercept Point f = 10MHz, 4dBm Each Tone 40 dBm Differential Gain G = +2, NTSC, V
O
= 1.4Vp-p, RL = 150 0.025 %
Differential Phase G = +2, NTSC, V
O
= 1.4Vp-p, RL = 150 0.02 degrees
Bandwidth for 0.1dB Flatness G = +2 135
(5)
MHz
OFFSET VOLTAGE
Input Offset Voltage V
CM
= 0V ±3 ±5.5 ±2 ±4.5 mV
Over Temperature Range ±5 ±8 ±4 ±7mV
Power Supply Rejection Ratio V
S
= ±4.7 to ±5.5V 55 64 58 67 dB
INPUT BIAS CURRENT
Non-Inverting V
CM
= 0V ±5.7 ±30 ±18 µA
Over Temperature Range ±10 ±80 ±35 µA
Inverting V
CM
= 0V ±1.1 ±35 ✻✻ µA
Over Temperature Range ±30 ±75 ✻✻ µA
NOISE
Input Voltage Noise Density
f = 100Hz 16 nV/Hz f = 2kHz 4.9 nV/Hz f = 10kHz 3.2 nV/Hz f = 1MHz 3.2 nV/Hz f
B
= 100Hz to 200MHz 45.3 µVrms
Input Bias Current Noise Density
Inverting: f = 1MHz 32 pA/Hz Non-Inverting: f = 1MHz 11.9 pA/Hz
INPUT VOLTAGE RANGE
Common-Mode Input Range
Over Temperature Range ±2.5 ±2.9 ✻✻ V
Common-Mode Rejection V
CM
= ±1V 45 50 ✻✻ dB
INPUT IMPEDANCE
Non-Inverting 500 || 1 k || pF Inverting 50
OPEN-LOOP TRANSRESISTANCE
Open-Loop Transresistance V
O
= ±2V, RL = 100 150 190 200 250 k
Over Temperature Range V
O
= ±2V, RL = 100 100 150 k
OUTPUT
Voltage Output No Load ±2.7 ±2.9 ✻✻ V
Over Temperature Range ±2.5 ±2.75 ✻✻ V
Voltage Output R
L
= 250Ω±2.7 ±2.9 ✻✻ V
Over Temperature Range ±2.5 ±2.7 ✻✻ V
Voltage Output R
L
= 100Ω±2.2 ±2.8 ✻✻ V
Over Temperature Range ±2.0 ±2.5 ✻✻ V
Output Current, Sourcing 80 120 ✻✻ mA
Over Temperature 70 mA
Output Current, Sinking 60 80 ✻✻ mA
Over Temperature 35 mA Short Circuit Current 150 mA Output Resistance 0.1MHz, G = +2 0.02
POWER SUPPLY
Specified Operating Voltage ±5 V Operating Voltage Range ±4.5 ±5.5 ✻✻V Quiescent Current V
S
= ±5V ±5 ±7.75 ±4.5 ±5.75 mA
Over Temperature Range ±5.5 ±8.5 ±4.7 ±6.5 mA
TEMPERATURE RANGE
Specification: P, U, N, UB, NB –40 +85 ✻✻°C Thermal Resistance,
θ
JA
P 8-Pin DIP 100 °C/W
U SO-8 125 °C/W
N SOT23-5 150 °C/W
NOTES: (1) An asterisk () specifies the same value as the grade to the left. (2) Frequency response can be strongly influenced by PC board parasitics. The demonstration boards show low parasitic layouts for this part. Refer to the demonstration board layout for details. (3) Slew rate is rate of change from 10% to 90% of output voltage step. (4) At G = +1, R
FB
= 560 for PDIP and 402 for SO-8. (5) This specification is PC board layout dependent.
SPECIFICATIONS
At TA = +25°C, VS = ±5V, RL = 100, and RFB = 402Ω, unless otherwise noted.
OPA658P, U, N OPA658UB, NB
PARAMETER CONDITION MIN TYP MAX MIN TYP MAX UNITS
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OPA658
1
2 3 4
8
7 6 5
NC
+V
S
Output NC
NC
–Input +Input
–V
S
1
2
3
54+V
S
–Input
Output
–V
S
+Input
Top View DIP/SO-8
The information provided herein is believed to be reliable; however, BURR-BROWN assumes no responsibility for inaccuracies or omissions. BURR-BROWN assumes no responsibility for the use of this information, and all use of such information shall be entirely at the user’s own risk. Prices and specifications are subject to change without notice. No patent rights or licenses to any of the circuits described herein are implied or granted to any third party. BURR-BROWN does not authorize or warrant any BURR-BROWN product for use in life support devices and/or systems.
PIN CONFIGURATION
Supply ............................................................................................... ±5.5V
Internal Power Dissipation .......................... See Thermal Considerations
Differential Input Voltage .................................................................. ±1.2V
Input Voltage Range ............................................................................ ± V
S
Storage Temperature Range: P, U, UB, N, NB ............ –40°C to +125°C
Lead Temperature (soldering, 10s).............................................. +300°C
(soldering, SOIC 3s) ...................................................................... +260°C
Junction Temperature (T
J
) ............................................................ +175°C
ABSOLUTE MAXIMUM RATINGS
ELECTROSTATIC DISCHARGE SENSITIVITY
Electrostatic discharge can cause damage ranging from per­formance degradation to complete device failure. Burr-Brown Corporation recommends that all integrated circuits be handled and stored using appropriate ESD protection methods.
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 published speci­fications.
SOT23-5
PACKAGE DRAWING TEMPERATURE PACKAGE ORDERING
PRODUCT PACKAGE NUMBER
(1)
RANGE MARKING
(2)
NUMBER
(3)
OPA658U SO-8 Surface Mount 182 –40°C to +85°C OPA658U OPA658U OPA658UB SO-8 Surface Mount 182 –40°C to +85°C OPA658UB OPA658UB OPA658N 5-pin SOT23-5 331 –40°C to +85°C A58 OPA658N-250
OPA658N-3k
OPA658NB 5-pin SOT23-5 331 –40°C to +85°C A58B OPA658NB-250
OPA658NB-3k
OPA658P 8-Pin Plastic DIP 006 –40°C to +85°C OPA658P OPA658P
NOTE: (1) For detailed drawing and dimension table, please see end of data sheet, or Appendix C of Burr-Brown IC Data Book. (2) The “B” grade of the SO-8 will be marked with a “B” by pin 8. The “B” grade of the SOT23-5 will be marked with a “B” near pins 3 and 4. (3) The SOT23-5 is only available on a 7" tape and reel (e.g. ordering 250 pieces of “OPA658N-250” will get a single 250 piece tape and reel. Ordering 3000 pieces of “OPA658N-3k” will get a single 3000 piece tape and reel). Please refer to Appendix B of Burr-Brown IC Data Book for detailed Tape and Reel Mechanical information.
PACKAGE/ORDERING INFORMATION
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OPA658
TYPICAL PERFORMANCE CURVES
At TA = +25°C, VS = ±5V, RL = 100, and RFB = 402Ω, unless otherwise noted.
55
50
45
40
35
30
25
–4 –3 –2 –1 0 1 2 3 4
COMMON-MODE REJECTION
vs INPUT COMMON-MODE VOLTAGE
Common-Mode Rejection (dB)
Common-Mode Voltage (V)
SUPPLY CURRENT vs TEMPERATURE
5
4
–75 –50 –25 0 25 50 75 100 125
Ambient Temperature (°C)
Supply Current (±mA)
NON-INVERTING INPUT BIAS CURRENT
vs TEMPERATURE
–75 –50 –25 0 25 50 75 100 125
Ambient Temperature (°C)
Non-Inverting Input Bias Current I
B
+ (µA)
10
8
6
4
2
3.20
3.10
3.0
2.90
2.80
2.70
2.60
2.50
2.40
2.30
OUTPUT SWING vs TEMPERATURE
Temperature (°C)
–60 –40 –20 0 20 40 60 80 100
Output Swing (V)
+V
O
–V
O
RL = 250
RL = 100
–V
O
+V
O
PSRR AND CMR vs TEMPERATURE
75
70
65
60
55
50
45
–75 –50 –25 0 25 50 75 100 125
PSRR , CMR (dB)
CMR
PSR–
Temperature (°C)
PSR+
PSRR
120
110
100
90
80
70
–75 –50 –25 0 25 50 75 100 125
OUTPUT CURRENT vs TEMPERATURE
Ambient Temperature (°C)
Output Current (±mA)
IO–
I
O
+
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OPA658
At TA = +25°C, VS = ±5V, RL = 100, and RFB = 402Ω, unless otherwise noted.
TYPICAL PERFORMANCE CURVES (CONT)
10
6
10
5
10
4
10
3
10
2
10
1
1
0
–45
–90
–135
–180
–225
1k 10k 100k 1M 10M 100M 1G
OPEN-LOOP TRANSIMPEDANCE AND PHASE
vs FREQUENCY
Frequency (Hz)
Transimpedance ()
Open-Loop Phase (°)
Phase
Transimpedance
INVERTING INPUT BIAS CURRENT
vs TEMPERATURE
–75 –50 –25 0 25 50 75 100 125
Temperature (°C)
Inverting Input Bias Current I
B
– (µA)
2.0
1.8
1.6
1.4
1.2
1.0
0.8
0.6
0.4
OPEN-LOOP GAIN AND PHASE vs FREQUENCY
Frequency (Hz)
60
40
20
0
–20
–40
–60
0
–45
–90
–135
–180
–225
1k 10k 100k 1M 10M 100M 1G
Open-Loop Gain (dB)
Open-Loop Phase (°)
Gain
Phase
6
3
0
–3
–6
–9
1M 10M 100M 1G
CLOSED-LOOP BANDWIDTH
Frequency (Hz)
Gain (dB)
SO-8 Bandwidth = 881MHz, RFB = 402
G = +1
DIP Bandwidth = 949MHz, RFB = 560
9
6
3
0
–3
–6
1M 10M 100M 1G
CLOSED-LOOP BANDWIDTH
Frequency (Hz)
Gain (dB)
DIP Bandwidth = 682MHz
SO-8 Bandwidth = 680MHz
G = +2
20
17
14
11
8
5
2
1M 10M 100M 1G
CLOSED-LOOP BANDWIDTH
Frequency (Hz)
Gain (dB)
SO-8/DIP Bandwidth= 372MHz
G = +5
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OPA658
TYPICAL PERFORMANCE CURVES (CONT)
At TA = +25°C, VS = ±5V, RL = 100, and RFB = 402Ω, unless otherwise noted.
160 120
80 40
0 –40 –80
–120 –160
Time (5ns/div)
SMALL SIGNAL TRANSIENT RESPONSE
Output Voltage (mV)
G = +2
1.6
1.2
0.8
0.4 0
–0.4 –0.8 –1.2 –1.6
LARGE SIGNAL TRANSIENT RESPONSE
Time (5ns/div)
Output Voltage (V)
G = +2
–50
–60
–70
–80
–90
–100
100k 1M 10M 100M
HARMONIC DISTORTION vs FREQUENCY
Frequency (Hz)
Harmonic Distortion (dBc)
2f
O
3f
O
5MHz HARMONIC DISTORTION vs OUTPUT SWING
Output Swing (Vp-p)
–60 –65 –70 –75 –80 –85 –90 –95
–100
01234
Harmonic Distortion (dBc)
2f
O
3f
O
G = +2
26
23
20
17
14
11
8
1M 10M 100M 1G
CLOSED-LOOP BANDWIDTH
Frequency (Hz)
Gain (dB)
SO-8/DIP Bandwidth = 200MHz
G = +10
40
35
30
25
20
15
10
10
1009080706050403020
RECOMMENDED ISOLATION RESISTANCE
vs CAPACITIVE LOAD
Capacitive Load (pf)
Isolation Resistance
G = +2
OPA658
C
L
1k
R
ISO
402
402
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OPA658
At TA = +25°C, VS = ±5V, RL = 100, and RFB = 402Ω, unless otherwise noted.
TYPICAL PERFORMANCE CURVES (CONT)
–60
–65
–70
–75
–80
–85
–75 –50 –25 0 25 50 75 100 125
Temperature (°C)
HARMONIC DISTORTION vs TEMPERATURE
(V
O
= 2Vp-p, G = +2)
Harmonic Distortion (dBc)
3f
O
2f
O
HARMONIC DISTORTION vs GAIN
(f
O
= 5MHz, VO = 2Vp-p)
Non-Inverting Gain (V/V)
–50
–55
–60
–65
–70
–75
Harmonic Distortion (dBc)
012345678910
3f
O
2f
O
10MHz HARMONIC DISTORTION vs OUTPUT SWING
Output Swing (Vp-p)
–60
–70
–80
–90
–100
0.01 0.1
2f
O
14V10
Harmonic Distortion (dBc)
3f
O
INPUT VOLTAGE AND CURRENT NOISE
vs FREQUENCY
Frequency (Hz)
100
10
1
Voltage Noise (nV/Hz)
Current Noise (pA/Hz)
10
2
10
3
10
4
10
5
10
6
10
7
Non-Inverting Noise
Inverting Current Noise
Voltage Noise
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OPA658
For non-inverting operation, the input signal is applied to the non-inverting (high impedance buffer) input. The output (buffer) error current (IE) is generated at the low impedance inverting input. The signal generated at the output is fed back to the inverting input such that the overall gain is (1 + RFB/RFF). Where a voltage-feedback amplifier has two symmetrical high impedance inputs, a current feedback amplifier has a low inverting (buffer output) impedance and a high non-inverting (buffer input) impedance.
The closed-loop gain for the OPA658 can be calculated using the following equations:
(1)
(2)
At higher gains the small value inverting input impedance causes an apparent loss in bandwidth. This can be seen from the equation:
(3)
This loss in bandwidth at high gains can be corrected without affecting stability by lowering the value of the feedback resistor from the specified value of 402Ω.
OFFSET VOLTAGE AND NOISE
The output offset is the algebraic sum of the input offset voltage and bias current errors. The output offset for non­inverting operation is calculated by the following equation:
(4)
If all terms are divided by the gain (1 + R
FB/RFF
) it can be observed that input referred offsets improve as gain increases. The effective noise at the output can be determined by taking
APPLICATIONS INFORMATION
THEORY OF OPERATION
Conventional op amps depend on feedback to drive their inputs to the same potential, however the current feedback op amp’s inverting and non-inverting inputs are connected by a unity gain buffer, thus enabling the inverting input to automatically assume the same potential as the non-invert­ing input. This results in very low impedance at the inverting input to sense the feedback as an error current signal.
DISCUSSION OF PERFORMANCE
The OPA658 is a low-power, unity gain stable, current feedback operational amplifier which operates on ±5V power supply. The current feedback architecture offers the follow­ing important advantages over voltage feedback architec­tures: (1) the high slew rate allows the large signal perfor­mance to approach the small signal performance, and (2) there is very little bandwidth degradation at higher gain settings.
The current feedback architecture of the OPA658 provides the traditional strength of excellent large signal response plus wide bandwidth, making it a good choice for use in high resolution video, medical imaging and DAC I/V Conver­sion. The low power requirements make it an excellent choice for numerous portable applications.
DC GAIN TRANSFER CHARACTERISTICS
The circuit in Figure 1 shows the equivalent circuit for calculating the DC gain. When operating the device in the inverting mode, the input signal error current (I
E
) is ampli-
fied by the open loop transimpedance gain (T
O
). The output
signal generated is equal to T
O
x IE. Negative feedback is
applied through R
FB
such that the device operates at a gain
equal to –R
FB/RFF
.
FIGURE 1. Equivalent Circuit.
FIGURE 2. Output Offset Voltage Equivalent Circuit.
V
O
T
O
C
C
L
SRS
(50)
C
1
V
I
V
N
R
FF
R
FB
I
E
+
Inverting Gain =
R
FB
R
FF
 
 
1 +
1
Loop Gain
NonInverting Gain =
1 +
R
FB
R
FF
 
 
1 +
1
Loop Gain
whereLoop Gain =
T
O
RFB+ RS1 +
R
FB
R
FF
 
 
    
    
ƒ
ACTUAL
BW
ƒ
AV=+2
()
BW
[]
x1.25
()
1+
R
S
R
FB
 
 
× 1 +
R
FB
R
FF
 
 
 
 
 
 
VIO1 +
R
FB
R
FF
 
 
± Ib
I
× R
FB
OutputOffsetVoltage =±IbN× RN1 +
R
F
B
R
FF
 
 
±
R
FB
R
FF
Ib
I
R
N
Ib
N
V
IO
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OPA658
The 402 used in setting the specification achieves a nomi­nal maximally flat butterworth response while assuming a 2pF output pin parasitic. Increasing the feedback resistor will over compensate the amplifier, rolling off the frequency response, while decreasing it will decrease phase margin, peaking up the frequency response. Note that a non-invert­ing, unity gain buffer application still requires a feedback resistor for stability (560 for SO-8, 402 for PDIP, and 324 for SOT23).
d) Connections to other wideband devices on the board may be made with short direct traces or through on-board transmission lines. For short connections, consider the trace and the input to the next device as a lumped capacitive load. Relatively wide traces (50 to 100 mils) should be used, preferably with ground and power planes opened up around them. Estimate the total capacitive load and set R
ISO
from
the plot of recommended R
ISO
vs capacitive load. Low
parasitic loads may not need an R
ISO
since the OPA658 is
nominally compensated to operate with a 2pF parasitic load. If a long trace is required and the 6dB signal loss intrinsic to
doubly terminated transmission lines 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 50 environ­ment is not necessary on board, and in fact a higher imped­ance environment will improve distortion as shown in the distortion vs load plot. With a characteristic impedance defined based on board material and desired trace dimen­sions, a matching series resistor into the trace from the output of the amplifier is used as well as a terminating shunt resistor at the input of the destination device. Remember also that the terminating impedance will be the parallel combination of the shunt resistor and the input impedance of the destination device; the total effective impedance should match the trace impedance. Multiple destination devices are best handled as separate transmission lines, each with their own series and shunt terminations.
If the 6dB attenuation loss of a doubly terminated line is unacceptable, a long trace can be series-terminated at the source end only. This will help isolate the line capacitance from the op amp output, but will not preserve signal integrity as well as a doubly terminated line. If the shunt impedance at the destination end is finite, there will be some signal attenuation due to the voltage divider formed by the series and shunt impedances.
e) Socketing a high speed part like the OPA658 is not recommended. The additional lead length and pin-to-pin
capacitance introduced by the socket creates an extremely troublesome parasitic network which can make it almost impossible to achieve a smooth, stable response. Best results are obtained by soldering the part onto the board. If socket­ing for the DIP package is desired, high frequency flush mount pins (e.g., McKenzie Technology #710C) can give good results.
The OPA658 is nominally specified for operation using ±5V power supplies. A 10% tolerance on the supplies, or an ECL –5.2V for the negative supply, is within the maximum
the root sum of the squares of equation (4) and applying the spectral noise values found in the Typical Performance Curve graph section. This applies to noise from the op amp only. Note that both the noise figure (NF) and the equivalent input offset voltages improve as the closed loop gain increases (by keeping R
FB
fixed and reducing RFF with RN = 0).
INCREASING BANDWIDTH AT HIGH GAINS
The closed-loop bandwidth can be extended at high gains by reducing the value of the feedback resistor R
FB
. This band­width reduction is caused by the feedback current being split between RS and R
FF
(refer to Figure 1). As the gain increases
(for a fixed R
FB
), more feedback current is shunted through
R
FF
, which reduces closed-loop bandwidth.
CIRCUIT LAYOUT AND BASIC OPERATION
Achieving optimum performance with a high frequency am­plifier like the OPA658 requires careful attention to layout parasitics and selection of external components. Recommen­dations for PC board layout and component selection 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. Otherwise, ground and power planes should be unbroken elsewhere on the board.
b) Minimize the distance (< 0.25") from the two power pins to high frequency 0.1µF decoupling capacitors. At the 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. Larger (2.2µF to 6.8µF) decoupling capacitors, effective at lower frequencies, should also be used. These may be placed somewhat farther from the device and may be shared among several devices in the same area of the PC board.
c) Careful selection and placement of external compo­nents will preserve the high frequency performance of the OPA658. 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 their leads as short as possible. Never use wirewound type resistors in a high frequency application.
Since the output pin and the inverting input pin are most sensitive to parasitic capacitance, always position the feed­back and series output resistor, if any, as close as possible to the package pins. Other network components, such as non­inverting input termination resistors, should also be placed close to the package.
The feedback resistor value acts as the frequency response compensation element for a current feedback type amplifier.
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OPA658
402
OPA658
V
AC
402
R
L
+V
S
+V
S
V
S
2
R
OUT
V
S
2
V
OUT
= + AV V
AC
AV = +2
specified total supply voltage of 11V. Higher supply voltages can break down internal junctions possibly leading to cata­strophic failure. Single supply operation is possible as long as common mode voltage constraints are observed. The com­mon mode input and output voltage specifications can be interpreted as a required headroom to the supply voltage. Observing this input and output headroom requirement will allow non-standard or single supply operation. Figure 3 shows one approach to single-supply operation.
THERMAL CONSIDERATIONS
The OPA658 will not require heatsinking under most oper­ating conditions. Maximum desired junction temperature will set a maximum allowed internal power dissipation as described below. In no case should the maximum junction temperature be allowed to exceed 175°C.
Operating junction temperature (T
J
) is given by
T
A
+ PD •
θ
JA
. The total internal power dissipation (PD) is
the sum of quiescent power (P
DQ
) and additional power
dissipated in the output stage (P
DL
) to deliver load power. Quiescent power is simply the specified no-load supply current times the total supply voltage across the part. P
DL
will depend on the required output signal and load but would, for a grounded resistive load, be at a maximum when the output is fixed at a voltage equal to 1/2 either supply voltage (for equal bipolar supplies). Under this condition PDL = V
S
2
/(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 an example, compute the maximum T
J
for an OPA658N
at A
V
= +2, RL = 100, RFB = 402, ±VS = ±5V, and the
specified maximum T
A
= +85°C. PD = 10V • 8.5mA + 52/
[4 • (100 || 804)] = 155mW. Maximum T
J
= 85°C +
0.155W • 150°C/W = 108°C.
DRIVING CAPACITIVE LOADS
The OPA658’s output stage has been optimized to drive low resistive loads. Capacitive loads, however, will decrease the amplifier’s phase margin which may cause high frequency peaking or oscillations. Capacitive loads greater than 5pF should be buffered by connecting a small resistance, usually 10 to 35, in series with the output as shown in Figure 5. This is particularly important when driving high capacitance loads such as flash A/D converters.
In general, capacitive loads should be minimized for opti­mum high frequency performance. Coax lines can be driven if the cable is properly terminated. The capacitance of coax cable (29pF/foot for RG-58) will not load the amplifier when the coaxial cable or transmission line is terminated with its characteristic impedance.
FIGURE 4. Closed-Loop Output Impedance vs Frequency.
100
10
1
0.1
0.01
0.001 10k 100k 1M 10M 100M
Output Impedance ()
Frequency (Hz)
G = +2
ESD PROTECTION
ESD static damage has been well recognized for MOSFET devices, but any semiconductor device deserves protection from this potentially damaging source. This is particularly true for very high speed, fine geometry processes.
ESD static damage can cause subtle changes in amplifier input characteristics without necessarily destroying the de­vice. In precision operational amplifiers, this may cause a noticeable degradation of offset voltage and drift. Therefore, static protection is strongly recommended when handling the OPA658.
OUTPUT DRIVE CAPABILITY
The OPA658 has been optimized to drive 75 and 100 resistive loads. The device can drive 2Vp-p into a 75 load. This high-output drive capability makes the OPA658 an ideal choice for a wide range of RF, IF, and video applica­tions. In many cases, additional buffer amplifiers are un­needed.
Many demanding high-speed applications such as ADC/DAC buffers require op amps with low wideband output impedance. For example, low output impedance is essential when driving the signal-dependent capacitances at the inputs of flash A/D converters. As shown in Figure 4, the OPA658 maintains very low closed-loop output imped­ance over frequency. Closed-loop output impedance in­creases with frequency since loop gain is decreasing with frequency.
FIGURE 3. Single Supply Operation.
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OPA658
close-in spurious tones will appear at fO ±3 • f. The two tone, third-order spurious plot shown in Figure 7 indicates how far below these two equal power, closely spaced, tones the intermodulation spurious will be. The single tone power is at a matched 50 load. The unique design of the OPA658 provides much greater spurious free range than what a two­tone third-order intermodulation intercept specification would predict. This can be seen in Figure 7 as the spurious free range actually increases at the higher output power levels.
COMPENSATION
The OPA658 is internally compensated and is stable in unity gain with a phase margin of approximately 62°, and approxi­mately 64° in a gain of +2V/V when used with the recom­mended feedback resistor value. Frequency response for other gains are shown in the Typical Performance Curves.
The high-frequency response of the OPA658 in a good layout is very flat with frequency.
DISTORTION
The OPA658’s Harmonic Distortion characteristics into a 100 load are shown versus frequency and power output in the Typical Performance Curves. Distortion can be further improved by increasing the load resistance as illustrated in Figure 6. Remember to include the contribution of the feedback resistance when calculating the effective load re­sistance seen by the amplifier.
Narrowband communication channel requirements will ben­efit from the OPA658’s wide bandwidth and low intermodulation distortion on low quiescent power. If output signal power at two closely spaced frequencies is required, third-order nonlinearities in any amplifier will cause spuri­ous power at frequencies very near the two funda­mental frequencies. If the two test frequencies, f
1
and f2, are specified in terms of average and delta frequency, fO = (f1 + f2)/2 and f = f2 – f1, the two, third-order,
DIFFERENTIAL GAIN AND PHASE
Differential Gain (dG) and Differential Phase (dP) are among the more important specifications for video applications. dG is defined as the percent change in closed-loop gain over a specified change in output voltage level. dP is defined as the change in degrees of the closed-loop phase over the same output voltage change. Both dG and dP are specified at the NTSC sub-carrier frequency of 3.58MHz and the PAL sub­carrier of 4.43MHz. All NTSC measurements were per­formed using a Tektronix model VM700A Video Measure­ment Set.
dG/dP of the OPA658 were measured with the amplifier in a gain of +2V/V with 75 input impedance and the output back-terminated in 75. The input signal selected from the generator was a 0V to 1.4V modulated ramp with sync pulse. With these conditions the test circuit shown in Figure 8 delivered a 100IRE modulated ramp to the 75 input of the videoanalyzer. The signal averaging feature of the analyzer
FIGURE 5. Driving Capacitive Loads.
FIGURE 6. 5MHz Harmonic Distortion vs Load Resistance.
–55
–60
–65
–70
–75
–80
–85
5MHz HARMONIC DISTORTION vs
LOAD RESISTANCE (G = +2)
Load Resistance ()
Harmonic Distortion (dBc)
10 100 1k
G = +2, VO = 2Vp-p, fO = 5MHz
3f
O
2f
O
FIGURE 7. Third-Order Spurious Level vs Frequency.
–65
–70
–75
–80
–85
–90
–18 –16 –14 –12 –10 –8 –6 –4 –2 0 2 4
Third-Order Spurious Level (dBc)
TWO TONE, THIRD-ORDER SPURIOUS LEVELS
Single Tone Power (dBm)
20MHz
10MHz
5MHz
OPA658
75
75
402
402
75
75
TEK TSG 130A
TEK VM700A
FIGURE 8. Configuration for Testing Differential Gain/Phase.
OPA658
50
R
ISO
RLC
L
10 to 35
402402
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®
OPA658
was used to establish a reference against which the perfor­mance of the amplifier was measured. Signal averaging was also used to measure the dg and dp of the test signal in order to eliminate the generator’s contribution to measured ampli­fier performance. Typical performance of the OPA658 is
0.025% differential gain and 0.02° differential phase to both NTSC and PAL standards.
SPICE MODELS AND EVALUATION BOARDS
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 have a major effect on circuit performance. SPICE models are available on a disk from the Burr-Brown Appli­cations Department.
Demonstration boards are available for each OPA658 pack­age style. These boards implement a very low parasitic layout that will produce the excellent frequency and pulse responses shown in the Typical Performance Curves. For each package style, the recommended demonstration board is:
Contact your local Burr-Brown sales office or distributor to order demonstration boards.
DEM-OPA65xP 8-Pin DIP for the OPA658P DEM-OPA65xU SO-8 for the OPA658U DEM-OPA6xxN SOT23 for the OPA658N
FIGURE 9. Layout Detail For DEM-OPA65xP Demonstration Board.
R
6
R
1
OPA658
Out
J
1
1 2
GND
–5V
P2
R
7
R
5
+In
R
3
R
4
R
5
–In
J
1
J
2
2
7
4
6
3
C
2
0.1µF
C
4
2.2µF
402
C
1
2.2µF
C
3
0.1µF
1 2
GND
+5V
P1
+
+
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®
OPA658
FIGURE 10a. Evaluation Board Silkscreen (Bottom). 10b. Evaluation Board Silkscreen (Top). 10c. Evaluation Board Layout
(Solder Side). 10d. Evaluation Board Layout (Layout Side).
(C)
(D)
(A)
(B)
DEM-OPA65xP Demonstration Board Layout
TYPICAL APPLICATION
FIGURE 11. Low Distortion Video Amplifier.
OPA658
V
OUT
402402
Video
Input
75
75
75 Transmission Line
75
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