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Selecting video op amps

Video amplifiers have unique and demanding specifications. Understanding them will help you select an amplifier that can do the job.

By Barry Harvey, Intersil Semiconductor -- EDN, 6/26/2008

Video op amps have improved significantly since their debut in the early 1990s. The first versions operated from ±15V supplies, featured bandwidths of 50 MHz, and delivered slew rates in the low hundreds of volts per microsecond. Today’s fastest amplifiers run on ±5V supplies with bandwidths of 1.4 GHz and slew rates of 6000V/µsec. There are hundreds of versions available, and, to add to the challenge, many applications require the lowest possible supply voltage.

To simplify the design choices, it’s important to identify major parameters of interest. Start with the kind of signal the op amp is passing, the available supply voltages, and the power dissipation that an application allows or tolerates. Important intangibles include ease of use and tolerance to board layout. This article covers the signal requirements and then reviews available amplifier topologies. Table 1 suggests amplifiers for different signals.

Video signals

The op-amp industry adopted the composite-video format in monochrome form in the early 1940s and the color standard in 1953 (Figure 1). White-level, color, and horizontal- and vertical-synchronous signals combine onto one conductor. The synchronous signals originally guided the electron beam’s horizontal line-scan in early CRTs. In today’s digital televisions they perform memory-mapped data-stream timing.

In US composite video, the synchronous pulses repeat at a 15,734-Hz rate. A flat region that represents a dark display and includes a chroma burst follows each horizontal synchronization. The burst is a number of 3.58-MHz sine waves that serves as a frequency reference for subsequent embedded color information. The composite-video receiver has its own chroma reference oscillator that resynchronizes each burst. The video-line-picture content follows the chroma burst. Figure 1 shows a sample video content in which a steady color amplitude rides on a white level that increases across the line. Pictures contain fairly unpredictable color and intensity content. The figure does not show the vertical-synchronization patterns, which are the same amplitude as the horizontal synchronization but of complex pattern and durations.

The maximum amplitudes of the synchronization feature, the chroma, and the white part of the figure are 300, 100, and 707 mV, respectively. These amplitudes make the maximum peak-to-peak standard composite-signal amplitude approximately 1.05V p-p. Not all combinations of chroma and white amplitude exist in the color space of a particular video standard. The amplifier must be biased within its supplies to be able to handle the signal.

One source of video might be a DAC output, such as a cable-tuner box. These sources generally place the bottom of the synchronized signal at ground, with video details going positive. The boxes usually make output data samples at four times the chroma frequency but still have DAC-step artifacts that require filtering before use. Active filters using op amps frequently accomplish this task. Some op amps come with the appropriate filters and buffer the DAC output when you connect them to standard 75Ω video cable. The amplifier typically drives a reverse-termination resistor in series with the cable to absorb any reflections, and this step loses one-half the output amplitude. The amplifier then has a gain of two to recover standard-output amplitude.

It also is important to consider the voltage excursions of the signal with respect to available power supplies. The synchronous amplitude is on ground at the DAC output, and an amplifier has no problem passing this amplitude with a negative-power supply. However, negative supplies are often unavailable. Some amplifiers’ inputs can linearly go to ground and have allegedly rail-to-rail outputs, but neither MOS nor bipolar rail-to-rail amplifiers are completely linear closer than about 100 mV from the supply rails. Figure 2 shows the differential gain measurement of a low-power bipolar op amp running on a single 5V power supply.

Differential gain is a measure of the deviation of ac gain over changing dc operating points. The output gain is stable only above an output dc level of 0.1V. Although the synchronizing level is not critical and may be distorted, forcing an amplifier into output overload incurs a recovery-time penalty when it has to rise back above ground. This recovery time could adversely affect synchronization. In single-supply applications, designers bias the output positive at approximately 200 mV by using offsetting circuitry.

The blue curve in the figure has a 150Ω load due to the 75Ω cable and termination in series with 75Ω back-match resistor. It exhibits large differential gain error as the output gets within 0.8V of the supply voltage. This situation occurs at a current of 28 mA, twice that of one standard load and amplitude. The proper way to bias this amplifier would be to offset the input by 100 mV. At a gain of two, this approach produces an output swing of 0.2 to 2.2V. With the positive head room of 0.8V, you establish a minimum supply voltage of 3V.

You use amplifiers to accomplish filtering, clamping, dc restoration, and buffering of the signal. Buffering provides input-termination quality and routes the signal to any manner of nonterminated loads.

Using ac coupling rather than dc restoration or clamping yields a larger peak-to-peak signal to pass. The average level of video signals varies between dark and fully white (Figure 3). The average level is the dc bias the amplifier’s input pin receives from the input coupling capacitor. The peak negative excursion occurs during a static fully white signal, and the synchronous voltage is the dc bias minus 0.86V. When a long-term, fully dark signal changes to a fully white signal, the first white level is temporarily peaking at dc bias plus 0.64V and slowly sags down to the upper waveform of Figure 4. Thus, the amplifier must support a video signal of 1.5V p-p, not 1V p-p, as in the dc-coupled case. This situation can be problematic with low supply voltage.

Generalized methods exist for offsetting or stabilizing dc levels. Circuits that perform dc restoration observe the synchronized signals and use timers to gate the burst-time interval. During this interval, a feedback loop forces the burst’s average amplitude to a reference—ground, for example—and the offset correction is in a sample-and-hold activity throughout the rest of the time. Circuits that clamp the synchronous signal’s negative-going extreme when you apply it through a capacitor also commonly establish offset.

The performance of composite-signal amplifiers has several metrics. The first is differential gain, the measure of stability of ac gain at 3.58 MHz over the video range of dc levels. The required performance is 0.05 to 1% stability, depending on quality level. The differential phase, the variation of phase lag through the amplifier at 3.58 MHz with dc variations through the video region, is similar to differential gain. An excessive deviation of phase manifests itself as color errors on the screen. The range of required performance is 0.05 to 1°. You can think of phase variation with dc level as the frequency response itself varying with output current and voltage. It is worst in low-quiescent-current amplifiers.

Another figure of merit in composite-video-reproduction quality is group delay, the change of delay of signal components at one frequency relative to another frequency within the signal spectrum. Although delay is harmless, variations of delay cause visual edges to smear as different spectral components arrive at different times. Within the moderate spectral content of 4.5 MHz, a group delay constancy of approximately 30 nsec is necessary. This delay is easy for most amplifiers that have at least 50-MHz bandwidth to achieve.

The S video standard places the luminance and synchronous parts of the composite signal onto a Y channel and the color and chroma parts onto a C channel. The C channel has no dc variation, and differential-phase performance is unnecessary. The Y channel has a slightly reduced 1V-p-p swing, and the C channel has a 286-mV-p-p swing. Dual combined DAC filters/amplifiers and DAC filters and combining amplifiers that merge the Y and C channels into a composite output are available.

You can capacitor couple the output to save power. Because no dc current goes through the capacitor, the offset current is zero, and the video content is both sourcing (drawing supply current) and sinking (drawing no supply current). This approach uses three times less supply current than dc coupling. One drawback is that the average video content causes a slow baseline wandering at the load. This wandering decalibrates the video level. To combat the problem, almost all video destinations have dc-restore circuitry that recalibrates baselines at synchronous or burst events.

The other drawback of capacitor coupling is that the capacitor must pass a lot of low-frequency content because the video picture repeats 30 times per second. With an effective 150Ω load and approximately 5-Hz low-frequency cutoffs, you need a 200-µF coupling capacitor, a large and somewhat expensive component.

Read more In-Depth Technical Features

Some video amplifiers incorporate so-called sag feedback paths that allow the use of substantially reduced coupling capacitors. They work by feeding back signal from the load side of the coupling capacitor. Feedback induces the amplifier output to rise for low frequencies. Although the coupling capacitor loses low-frequency signals, the amplifier boosts them, and the final output maintains low-frequency gain.

In many designs, you must offset the region around the chroma burst so that it is at ground, and the synchronous signal goes 300 mV below ground. This approach is practical with a negative supply and a dc-restoration or clamp circuit. Fortunately, some amplifiers come with charge-pump switching supplies that create a negative supply and dc-restore circuits that poise the burst interval at ground. Dual and quad devices are also available; they place the burst area of the Y channel of S video at ground and the C midvoltage at ground. These devices also have the appropriate DAC filters. Output-charge-pump noise of representative parts is only 0.3 IRE (Institute of Radio Engineers) p-p. An IRE unit is 1% of the peak video range, or 7 mV.

The other kind of analog-video transmission is component and has three color components. RGB (red/green/blue) is the common computer-monitor standard and offers the highest quality of component video. RGB achieves a fully white-to-fully dark transition on adjacent pixels to optimize font appearance. For a common 1280×1024-pixel display with a 60-Hz scan-refresh rate, the pixel rate is nearly 100M pixels/sec. RGB components generally do not use DAC-reconstruction filters, instead transmitting the raw DAC output or a buffered version of it. Amplifier requirements are for a –3-dB bandwidth of 300 MHz, a slew rate of 1500V/µsec, and a settling time of 7 nsec to 1%.

The typical RGB amplifier is a triple with an internally set gain of two. Back-matching resistors are external because IC processes do not give accurate resistor values. Single-supply amplifiers typically have a slew rate of only approximately 500V/µsec and barely settle within a clock time. At the highest pixel counts, the amplifiers typically run on positive and negative supplies; are current-feedback or slew-enhanced, voltage-feedback designs; and have more than enough slew rate and bandwidth. Linearity for these devices should be 1% or better, and dc offsets are not generally important because almost all monitors have a dc-restoration feature for their inputs.

The other common component video is for HDTV (high-definition television), which uses the YPrPb standard. It has an overall luminance channel, Y; Pr, which contains red content minus Y; and Pb, which contains blue minus Y. You derive green from the weighted differences of them all. In 1080i television format, the video has a spectral content of 30 MHz, which a DAC typically generates when running at 135M or 270M samples/sec. An analog filter bandlimits and buffers the output-transmission line. Amplifiers should have better than 0.5-dB flatness at 30 MHz; greater-than-200-MHz, –3-dB bandwidth; a 200V/µsec minimum slew rate; and 0.3% linearity. Complete integrated filters and amplifiers have recently become available, but many designs still use discrete amplifiers as active filters or passive LC (inductance/capacitance) filters with supporting amplifiers.

Another variety of analog video is video over twisted-pair cable. Each component of this video is differential and transmits over Category 5 cable, which normally finds use in digital-network communications. Category 5 cable is less expensive and bulky than standard RGB coaxial cables. Category 5 cable is especially useful when video is concentrated, for instance, when users must access many computers in server clusters from a central control monitor and keyboard. Category 5 cable has four twisted pairs, three of which are for video; the remaining one is for keyboard or mouse signals in the KVM (keyboard/video/mouse) function. Various twisted-pair lines can be single-ended synchronous and computer-control signals. The single-ended, bandlimited signals prevent radio emission, but the twisted-pair, self-shielded, differential signals can operate at full pixel speeds.

Single-supply, triple-Category 5-cable drivers are available that include common-mode synchronous encoding. Currently, all the differential receivers are ±5V designs, but they effectively reject common-mode interference over wide frequency ranges. Integrated receivers with equalizers can undo the high-frequency losses the cables cause. Time equalizers are also available. Category 5 cable has twisted pairs with different winding pitches, and each pair is a slightly different length. The time equalizers can delay the signals coming in from the shorter lines to catch up with the delayed signals traversing the longer lines.

Amplifier topologies

VFAs (voltage-feedback amplifiers) have noise-versus-slew-rate trade-offs. NTSC (National Television System Committee) video is forgiving of noise, having only approximately 5 MHz of signal bandwidth, and can tolerate a total noise of 50 nV/ p-p in the signal chain for one IRE. The slew-rate requirement is only 22V/µsec. Supply current need not be more than 2 mA for line drivers with filters. Thus, VFAs, including CMOS devices, are good candidates for many applications.

Component video has higher performance requirements, and you can use only the fastest VFAs in this application. These amplifiers require a bandwidth of 200 MHz or more, a slew rate of at least 200V/µsec, and noise in the chain to 20 nV/. CFAs (current-feedback amplifiers) and older slew-enhanced VFAs perform the best but need dual supplies because they require input and output head room. A new amplifier topology, a low-voltage, slew-enhanced VFA, is also now available. These devices can operate on a single supply as low as 3V, their input ranges from ground to the supply minus 1V, and they have rail-to-rail output. The output slew rate, however, is greater than 2000V/µsec, meaning that video waveforms cannot cause slew distortion in these amplifiers. Table 1 summarizes various signal tasks and recommends some part specifications. See below for additional "Amplifier topology details."


Author Information
Barry Harvey is a fellow at Intersil Semiconductor Corp, where he has worked for 22 years. He currently performs analog-circuit design. He has a master’s degree in electrical engineering from Stanford University (Palo Alto, CA). His personal interests include guitar, mandolin, Shetland sheepdogs, and running. You can reach him at bharvey@intersil.com.

Amplifier topology details

The three amplifier topologies are voltage-feedback, current feedback, and slew-enhanced voltage feedback. In the video world, voltage-feedback amplification has a couple of common forms (Figure A). The upper schematic is more wideband but has lower gain. It is composed of an input differential amplifier that has a transconductance GM. There is a gain node with an effective compensation capacitor CC, and an effective low-frequency gain-limiting impedance RN. The gain node’s signal passes through an output buffer. The gain-bandwidth product is GM/2πCC. Standard analysis tells us that the unity-gain −3dB bandwidth frequency will be just less than the gain-bandwidth product, but this is not true for wideband amplifiers. Because of the extra phase shifts within all the stages and mediocre gain margin compared with low-frequency amplifiers, wideband amplifiers exhibit a peaking or extension of gain-bandwidth product, as seen in the −3dB bandwidth. This “bandwidth expansion” is from 1.3 in very serene amplifiers to as much as 2.5 in more complex and “nervous” amplifiers. The upper diagram in Figure A has a generally lower expansion, in the range of 1.3 to 1.8. Its low-frequency gain is typically limited to the range of 500 to 2000, although its linearity can be good. 

The lower circuit in Figure A uses a second amplifier to increase low-frequency gain and can be useful to reduce distortion in the 10-MHz realm. These are not particularly important traits for video reproduction. As we will see when we look at rail-to-rail output circuits, the two-amplifier partitioning is always used there. The frequency response and phase lag of the buffer in the upper circuit are always better than the operational integrator of the output stage of the second circuit, so the upper circuit has more potential bandwidth.

The most common voltage-feedback circuit is the folded-cascode circuit in Figure B. The input pnp transistors with R form the input transconductor. Their output signal is transferred by the npn cascodes, which level-shift, or “fold” the negative-supply-biased input stage output to a gain node that swings between both supplies. One cascode output goes to the pnp current mirror, whose output rejoins the gain node. If there is not more than 300 mV across the RCAS resistors, then the input levels may linearly run up to and slightly below ground. Unless there is some level shifting and some other clever circuitry within the output buffer, the output will not traverse to the supply rails and there is no inherent single-supply or rail-to-rail output potential. Typically the output can swing within 1 to 1.4V of the supply rails. This proximity is called output headroom. The input can only swing up to within 1V of the positive supply. 

VFAs that employ folded-cascode architectures typically operate on ±5V supplies or down to a single +5V supply. There are fundamental tradeoffs between slew rate and noise, as well as between supply current and bandwidth or slew rate. Amplifiers designed to handle video have typically 10- to 15-nV/ input noise to trade off for good slew rate. That trade typically yields about equal −3dB bandwidth and slew-rate numbers, those varying with supply current. That trade also results in 5- to 10-mV input offsets and low-frequency gains ~1000. Such amplifiers have combinations of supply current/−3dB bandwidth/slew rate of 1.4 mA, 200 MHz, and 100 V/μsec; 3mA, 270 MHz, 270 V/μsec, and 6mA, 600 MHz, 700 V/μsec. The amplifiers happen to have complex gain enhancement, which allows low offsets of <1 mV, low-frequency gains of around 30,000, and accuracies in the 0.1 to 0.02%, range. But across the industry such amplifiers are generally accurate to 0.3 to 0.1%.

Many low-frequency amplifiers offer rail-to-rail input stages that support signals all the way to either supply (Figure C). This circuit resembles the folded-cascode circuit and has a pnp input pair with an npn folded-cascode. The input pnp pair is active and dominant for inputs at ground up to the vicinity of the bias voltage VSW. For inputs higher than VSW, the input pnp’s turn off and shunt the tail current through Q5, which through the current mirror Q6-Q7 biases up the alternate input npn pair Q3-Q4. They then become the input transconductors and transfer their outputs to the pnp current mirror and finally to the gain node. A number of variations of the rail-to-rail approach exist, but all have similar switching behavior.

The rail-to-rail input stage exhibits a lot of poor behavior. The offset of the npn input pair has no correlation to the offset of the pnp input pair, so as the input rises past the switching point VSW, the offset. The shift may not be monotonic. The output might locally diminish for a small increase of input voltage in the vicinity of VSW. The rail-to-rail input stage has about the same errors as the folded-cascode circuit, but non-monotonicity is all but unknown in any other input stage. The switching event also causes glitches in the output. This is often not visible in low-frequency amplifiers, where the device-level switching times are far quicker than the overall amplifier response time, but in video amplifiers the response to glitches would be highly visible. For these reasons, no video amplifiers currently have rail-to-rail inputs.

The hybrid buffer LH0002 has the oldest high-speed output stage (Figure D). This compound complementary buffer has a lot of good behaviors. It is very wideband. It can drive some reasonable amount of load capacitance. It is very symmetrical in its sourcing and sinking of load current (if the IC process has similarly good npn and pnp transistors). The output voltage is largely unshifted with respect to the ‘0002 input.

There are misbehaviors too. The output impedance varies from low values at heavy sourcing currents to higher values at zero output current to different low values at heavy sinking currents. Thus there is a crossover distortion as well as even harmonic plus-to-minus distortion. Heavy loading is reflected through an npn beta times a pnp beta to load the gain node, dropping gain at heavy loads. The output cannot approach the supply rails by more than about 1V. Finally, the output impedance includes an inductive component, also load-current-dependent, that can vary from 8 nH in high-supply-current, very wideband amplifiers, to 50 nH in low-supply-current amplifiers. This inductance will resonate with load capacitance and threaten feedback stability. Despite these drawbacks the ‘0002 output stage is the best choice for non-rail-to-rail designs.

The rail-to-rail output stage topology has come into general use (Figure E). The stage has two complete amplifiers, one at the positive supply rail and one at the negative rail. Each of the amplifiers has a differential amplifier with a current mirror to produce an output error current that is amplified by its respective output transistor Q1 or Q2. Placing the output transistors in common-emitter connection rather than the common-collector connection of the LH0002 allows the outputs to swing to within a saturation voltage of the respective output transistor. The Figure D transistors Q3 and Q4 couple and coordinate the crossover characteristics between the output transistors. MOS versions of this circuit look and operate about the same.

This circuit becomes the output stage of the lower example of Figure A. It consequently has only about 40% of the bandwidth potential of the upper circuit. Modern devices consuming 6 mA of supply current give 400 to 500-MHz −3dB bandwidths and 500V/μsec slew rates. Lower power variants scale as 2 mA, 200 MHz, 200 V/μsec, both examples having 14-nV/ input noise.

All the amplifier circuits are fine for composite and HDTV component-video signals. They are barely up to the challenge of RGB video speeds. To cope with the very high slew rates desired for RGB, engineers developed the current-feedback amplifier (Figure F). In the CFA, the negative input is really the output of an LH0002 that buffers the positive input signal. If the divided voltage of the output from RF and RG do not equal the buffered input as presented at the minus input, the feedback network will deliver an error current. This error current will split and transfer through Q3 and Q4, then be sent to the gain node by the current mirrors, and will move the gain node potential until the output, divided by the feedback RF and RG, comes to equilibrium. The bandwidth is primarily set by RF and CC.

Unlike the VFA, whose slewing current is the constant current into the input stage, the CFA has no theoretical slew limit. The feedback network provides the slewing current, and slewing is only limited by feedback impedance and CC. There is no inherent slew limit in the CFA, just linear frequency-response time limitations. Though none of the CFAs are as fast as their linear limits, many approach this perfection.

With a CFA the frequency response is set by CC (internal) and RF (external). The user can tune bandwidth with RF. While the topology still exhibits bandwidth expansion, as in the VFA, the −3dB bandwidth does not drop nearly as fast with increasing gain. The noise performance is somewhat worse than the VFA at unity gain, but input-referred noise is very low for gains greater than 4. CFA settling time can be very fast because there is no slew time delay, just linear settling and ringing die-down.

A CFA drawback is that the input and output require about 1.3V of supply headroom. The frequency responses are very sensitive to parasitic capacitance at the negative input terminal. Furthermore, the input offset is very sensitive to the positive input level, giving very poor common-mode and supply rejection and poor thermal settling responses. A CFA minus input has a very large noise and bias current that does not match those of the positive input. The CFA is only accurate to 1%, but this is fine for RGB video signals.

The dynamic performance of the CFA is stellar. Available parts yield supply current, −3dB bandwidth, and slew rate values of 1.5 mA, 500 MHz, and 4000 V/μsec; 3.5 mA, 600 MHz, and 4700 V/μsec; and 8.5 mA, 1400 MHz, and 6000 V/μsec. Remember that these amplifiers need scrupulous circuit-board layouts and attention to load and feedback component values.

As a compromise between the huge slew potential of the CFA and the better accuracy and ease-of-use of the VFA, vendors have developed the slew-enhanced topology (Figure G). This topology uses the CFA input stage but includes an input buffer and an internal GM resistor R. The slew currents into CC are not limited by a current source, but lost is the relative stability of −3dB bandwidth with gain. We are left with a VFA that has no slew limitations beyond linear time response. The accuracy of this topology is 0.3 to 0.1%. With 12-nV/ input noise, we have supply current, −3dB bandwidth, and slew rate values from current designs of 2.5 mA, 200 MHz, and 2200 V/μsec; 5.2 mA, 400 MHz, and 3500 V/μsec; and 9.5 mA, 700 MHz, and 7000 V/μsec.

One new IC now becoming available is a combination of a slew-enhanced input that can go to ground and a rail-to-rail output that can work down to 3.0V single supplies. It yields 6.5 mA, 400 MHz, and 2400 V/μsec. This is probably the ideal video cable driver for RGB.

Engineers can accomplish differential-to-single-ended signal conversion for twisted-pair signal reception in a number of ways. The crudest is to use an op-amp with four resistors. The CMRR (common-mode-rejection ratio), the most important trait of the amplifier, is limited by the matching accuracy of the four resistors. This leaves us with only 34 dB worst-case common-mode rejection using 1% accurate resistors. Even worse, mismatches in circuit-board parasitic capacitance will worsen CMRR over frequency. Amplifiers with integrated and trimmed resistors exist, but CMRR is still mediocre and there are large dc currents involved with offsetting the output level. Alternatively, there exists an electronic method of handling differential inputs (Figure H). In this scheme the input is applied to a GM stage. It is summed with currents from the feedback GM. The amplifier will strive to make the output, applied through a feedback network, equal but the negative of the input GM unbalance. Whereas feedback action always moves a normal op-amp input stage back to balance, in this differential input stage the feedback unbalances the feedback GM to exactly null the input signal’s unbalancing of the input GM. In this way nonlinearities of the GMs cancel and there is no coupling between input signals and output levels, save for the intentional transfer of differential- to single-ended signals. Input CMRR is routinely 100 dB in this approach.

In order to provide differential outputs from single-ended inputs you can add a common-mode amplifier circuit (Figure I). Again, you could use four resistors and two op amps or four resistors and one truly differential amplifier, but all of the above complaints remain. Because the input CMRR is so good, a single-ended signal can be converted to differential by the input and feedback GMs while keeping all signal paths differential. Currently the output stages of this type of driver is of the LH0002 type, and require a minimum of a single 5V supply to operate. Many are also designed for ±5V supplies.



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