IC op-amps are dead. And we killed them. Op-amps are a key component for processing and amplifying audio signals. They can be found in virtually all audio gear in the form of tiny integrated circuits (IC's) like the one laying on its back in the picture. They also come with all of the pitfalls and shortcomings that IC op-amps have, like limited power dissipation and crummy compensation capacitors. Discrete op amps do not have these limitations and are a vastly superior op-amp for amplifying audio signals than their IC counterparts are. They can run much higher power, have a much deeper class A bias, and deliver a much more realistic and detailed sound. Discrete op-amps also permit the use of high-quality compensation capacitors and allow for two-pole compensation schemes which are impossible to implement in IC designs. All of this translates into a more detailed and engaging listening experience with better imaging and soundstaging than IC op-amps can deliver. In short, discrete designs are the best op-amp for audio.
Taking your gear to the next level.
Discrete op-amp installation in most gear is simple, requires no soldering, and is plug and play. Simply remove the IC op-amps from their sockets, install the discrete in their place, and then prepare yourself for audio bliss. The explainer video above illustrates the process and explains why discrete op-amps are the best op-amp for amplifying audio signals. And of course, we are here to answer all of your questions and walk you through the process together if you like. Contact us today, and we will gladly assist you. Just know that when you submit a contact form to Sparkos Labs, you will get a response from Sparko himself.
SS3602 Dual Discrete Op Amp
SS3601 Single Discrete Op Amp
Discrete op-amp nitty-gritty.
The SS3601 / SS3602 discrete op-amps will outperform virtually all audio grade monolithic IC op-amps in open-loop gain, noise performance, output current, and magnitude of class A bias current. Even the coveted OPA627 monolithic op amp, with a price tag of over 25 dollars, has 30dB less gain and around twice the noise of these discrete op-amps. The table below details the superior performance of the Sparkos Labs discrete op-amps to an array of audio grade monolithic IC op-amps.
Overview: All of Sparkos Labs discrete op-amps are based on Lin 3 Stage topology consisting of an input stage differential pair, a gain (VAS) stage, and an output stage all biased in class A mode with two pole compensation. All active devices are Bipolar Junction Transistors (BJTs) for the greatest linearity and agility that any silicon device has to offer. The devices are fully protected from over current conditions by active current limit circuitry in the output and gain stages, as well as being protected from large differential input voltages by back to back high-speed Schottky diodes across the inputs.
Input Stage: The input stage of these devices are comprised of a dual matched pair of NPN BJTs. This means that the device’s inputs will pull a small input bias current (specified as Ib) that will flow into the device. The common-mode input voltage range of the input stage can be as high as a few volts below the supply rails, however the best performance is obtained by minimizing this to a few volts above and below ground in a split supply application. The input offset voltage is factory trimmed and typically turns out to be better than 250uV @ ±12Vcc. The input stage is protected in the event that the inputs are driven apart, which usually happens during output clipping or rapid slewing. A cascode Wilson current mirror is utilized as the active load for the input differential pair for precise current matching between the input pair transistors.
Gain (VAS) Stage: The gain stage of the device is a cascode loaded Darlington for the highest linearity and open-loop gain possible. The cascode biasing voltage is derived from precision shunt references, which have a much lower dynamic impedance and lower noise than the low voltage zener diodes which are commonly used to derive this bias voltage. The gain stage is current limited by diode clamping action as opposed to a feedback action, which results in greater stability during clip.
Output Stage: The output stage is a push-pull emitter follower biased in class A mode with 8mA of standing current. Due to push-pull action, the output stage can source or sink 16mA of current and still remain in class A mode. The output stage will automatically revert to class AB mode in the event that more output current is demanded by the load, however, the best THD performance will be obtained by ensuring that the output stage stays in class A mode. Active current limiting is employed in the output stage to protect it from an overcurrent condition. The output transistors are high gain (β) individual devices in a SOT23 package manufactured by Diodes, Inc. who have developed a special manufacturing and encapsulation process that allows their devices to dissipate two to three times the power of a typical SOT23 packaged device. Utilizing these output devices allows Sparkos Labs discrete op-amps to have a high class A bias current and the ability to source or sink far more output current than comparable monolithic op-amps in a DIP8 package.
|Two pole compensation, despite its superiority to single pole schemes, is not often used in monolithic op amps due to the difficulty in fabricating the 2 capacitors at minimum that are required to implement it. Capacitors inside of monolithics consume a large amount of the die area and are therefore kept to a minimum in both capacitor value and quantity. The amount of capacitance required for at least one of the two capacitors in a 2 pole scheme tends be impossibly large for monolithic designs anyway, even if the die area were available for two capacitors. Beings how the Sparkos Labs discrete op amps employ 3 capacitors for compensation, they are impossible to fabricate as a monolithic, and are only possible as a discrete op amp. Such are the reasons that discrete op amps are the best op amp for amplifying audio signals.|
Monolithic op-amps mostly employ single-pole compensation schemes. They pay for this with a reduction in open-loop gain at audio frequencies, as well as a reduction in maximum open-loop gain that they can have in the first place. Since compensation schemes burn off gain by nature, and since a single-pole scheme burns it off at half of the rate of a two-pole scheme, there is a limitation that exists in how much gain they can start out within the first place to ensure they can burn it all off by the time the phase lag has shifted 180˚.
The monolithic op-amps that DO have a high open-loop gain always wind up having an excessively high bandwidth in the 50MHz region or so, which tends to make for a finicky device prone to instability and oscillation. Such high bandwidth devices also suffer from more susceptibility to ill effects from layout parasitics, capacitive loading, resistive feedback networks, and usually require a more stringent power supply bypassing capacitor arrangement comprised of a tantalum and a small value ceramic. Such limitations give most monolithic op-amps, even the good ones, little chance of working as drop-in replacements.
- Full Data Sheet Available
- 140 dB Open Loop Gain
- 415nV RMS (2.9nV√HZ) Noise to 20KHZ
- +/- 18 Vcc Max
- 15mA Class A Output Current
- 65mA Max Output Current
- 14mA Supply Current
- < 300µV Typical Offset
- Best Op Amp For Amplifying Audio Signals
- Available In Single Or Dual
- DIP8 Compatible Package
- Circular Machined Gold Plated Pins
- Smallest Discrete Op-Amp On The Market
- 100% Class A Biasing
- Two Pole Compensation
- NPO Capacitors
- 1% Metal Film Resistors
- Sound Cards
- Gain Stages
- Mic Amplifiers
- RIAA Amplifiers
- Crossovers / Filters
- Line Drivers
- Line Receivers
- Any Op-Amp In The Audio Path