How preamp and power tubes interact with wattage and speaker ratings to yield the glorious tones of yesterday and today.
Famous tube amps from companies like Fender, Marshall, Vox, and others have come to define the sound of virtually all electric-guitar music. To varying degrees, we know that these amps sound different from each other—and we might even know some basic specs, like what kind of tubes different models use, and maybe some details about stock speakers. But it can be hard to understand some of the finer reasons why these amps sound different from each other.
Once we plug in our guitars, all sorts of electrical processes happen as our signal makes its way from the input jack on through the unique set of electrical components that give each amp its signature sound and on through to the speaker. What goes on inside of our amp once we've plugged in our guitar? And what makes one amp louder than the next?
Although there's much, much more to cool amp tones than could possibly be discussed in an introductory piece like this, there are a lot of basics in common between the various brands and types of circuits, particularly with regard to how tubes (preamp and power), watt ratings, and speakers work. Because of this, we can learn a lot from a more specific example. To that end, let me tell you a little story about one of my favorite amps.
Dan Formosa found his 1960 Vox AC15's international voltage selector was incorrectly rated, and avoided overloading the amp's original tubes after doing an extensive online search and calculations.
I recently had a revelation about a beautiful, fawn-Tolex-covered, circa 1960 Vox AC15 that I bought from a dealer in the U.K. (full disclosure: many years ago) and finally got around to restoring. That meant replacing the electrolytic capacitors before daring to turn it on, since they have a life span. The AC15's international voltage selector on the far right of the control panel has settings for 115, 160, 205, 225 and 245 volts. I expected my U.S. wall voltage to be a few volts higher than its nominal 120, but still within reason for powering the amp at the 115 setting. However, the readings I got when checking the internal voltages were sky high. Its original Mullard EL84 power tubes were being overloaded at almost 17 watts, while 12 watts is the designated maximum and 14 watts would be pushing my luck. A few Variac voltage experiments over the next few days, along with some obsessively created Excel calculations and charts, verified that a wall voltage of 105 would be more appropriate. A week of deep Google searches and an eventual exclamation of "Thank you online discussion boards!" uncovered the problem. While there were no markings on my AC15's power transformer, chassis photos of two exact same amps and transformers showed the power transformer input terminals labeled as 105, 145 (not connected, like on mine), 160, 205 and 245. Despite the control panel's graphics, the amp never had a 115 volt option. That setting connects to the power transformer's 105 volt terminal. Furthermore, the 225 and 245 selections were both connected to the 245 terminal. Apparently when Vox printed that panel in 1960, they were just kidding.
My near-miss chance of seeing the power tubes glow like it's Christmas led me to think about the journey electrons take through an amp, combining forces emanating from your wall and your guitar to power the speaker. And what it means to overload a tube, as I came close to doing. Did you ever wonder why a single EL84 tube is rated at 12 watts, but powers a 5 watt amp? Or why two EL84s power a 15 watt amp? And why, when adding two more to the set, four will produce 30 watts? Let's explore watts and electrons, and investigate how exactly they travel in your amp, from power tube to speaker.
Identifying the limit of a tube or a speaker in watts means defining the maximum amount of energy per second it can safely handle.
Power In Vs. Power Out
When discussing power and watts, keep in mind that your tube amp isn't primarily functioning as a guitar amplifier. It's more of a space heater that produces sound. Here's a question that Steven Fryette, of Fryette Amplification and Sound City Amps, is frequently asked: "How is this a 30-watt amp when it says 100 watts on the back?" The short answer: An amplifier is filled with components that consume power that never gets to the speaker. Power transformers get warm, the pilot light and heating filaments within the tubes suck up a lot of juice—the preamp tubes and power tubes are approximately only 50 percent efficient— and there's heat being produced by the output transformer. Power-wise, the speaker operates mostly as a heat sink. A tube amp is therefore far less efficient than you might guess. More than 99 percent of the incoming power ends up as heat. Less than 1 percent exits as sound. To help understand how all that power turns into hardly any sound, we'll discuss EL84 tubes—although any power tube could serve as an example, since all are guided by the same physics.
At the center of the tube, preamp tubes included, is a cathode, a small tube that emits a cloud of electrons when heated. The plate—that's the gray or silver metal wall that you see when looking through the tube's glass—contains a high-voltage, electron-attracting DC charge. The signal from your pickups is sent to the preamp tube's grid, and eventually to the power tube's grid. The grid is a wrap of wires within the tube surrounding the cathode. The grid regulates the flow of electrons traveling from the cloud to the plate. In a class A or class AB amplifier (more on that to come), the grid allows electrons to flow even when at rest, or "idle," meaning electrons are on the move even with no guitar signal on the grid. Start to play and an increase and decrease of electron flow perfectly mirrors the guitar's signal. Electron flow is also known as current.
An RCA 6BQ5, aka EL84, tube consumes 12 watts, but like all power tubes it produces about half of that in power. The EL84 is a staple in the world of power tubes, typically associated with Vox and Marshall amps.
So, what's a watt? A watt is a rate of power—one joule per second, with a joule being a unit of energy—and can be calculated by multiplying volts times amps. Therefore, a watt is a measure of energy per second. Identifying the limit of a tube or a speaker in watts means defining the maximum amount of energy per second it can safely handle. Given the calculation for wattage (volts x amps = watts), you can see that increasing voltage, amps, or both will increase wattage.
Defining that power relationship one step further, what's an amp? It's short for "ampere" (not, in this case, "amplifier"). An amp holds the "per second" dimension of time seen in watts. In a classic plumbing analogy, volts are equivalent to water pressure, while amps measure the flow rate of that water. Too much of either will electrically flood your tube or speaker.
Water flow and pressure may not be a great analogy, because what really results when a tube or speaker becomes overloaded with watts is too much heat. But to complete the water analogy, resistance (or the related term "impedance" … we'll get to that, too) is like reducing the diameter of the water pipe. It's therefore fair to think of a tube as an electron pump, continually circulating electrons.
The Secret Life of Watts and Tubes
Electrons bombarding the plate too quickly will cause it to glow red and radically shorten the life of your tubes.
Receiving the up-and-down voltage waves of a guitar signal, the grid controls the flow of electrons, holding some back or unleashing them in accordance with whether you're delicately picking or bashing. The high level of positive, electron-attracting DC voltage on the screen grid and plate elements determines the amount of electrons pulled from the cathode. (Essentially determining how loud your amp gets.) Tubes, however, have limits, both on the rate at which the cathode can produce electrons and on the rate at which the plate will accept them.
Try to attract more electrons than the cathode can emit and you'll reach saturation. Flood the plate with too many electrons and you'll exceed its maximum dissipation level, overheating the tube. Set the grid's bias voltage too negative and you'll reach cutoff, a point where the negative swing of the guitar signal's sine wave will suddenly prevent any further electron flow from the cathode.
Picture your guitar's signal as a simple sine wave—a pure A440, for instance. Turning the volume up high can produce too much voltage swing on the tube's grid, and then on the plate, to be handled cleanly. The result you hear will be the sound of a sine wave being abruptly flattened at the high and low points of the wave. You may be perfectly happy with that level of distortion. But what if we overload a tube in a less friendly manner?
Amplifier circuits are designed to use tubes in different ways. The circuits we are primarily concerned with in tube amplifiers are class A and class AB. However understanding classes A and B helps to explain class AB, a hybrid of the two. So….
How Class A Circuits Catch a Wave
In a class A amp circuit, the power tube constantly carries the entire signal. So, a tube operating in a class A design is always conducting at maximum dissipation—full on—whether you're playing guitar or not.
Amplifiers with one power tube—single-ended amplifiers—operate in class A. That one power tube carries the entire 360-degree span of the sine wave, measured along a horizontal axis in degrees. The bias is set so that the amp idles along the vertical (Y-axis) center of the sine wave, evenly positioned between the peaks and valleys. That means the tube is always conducting at maximum dissipation—that it's always on full whether you're playing or not. When playing, the guitar signal creates peaks and valleys in the sine wave. Many, actually. The peak of the sine wave increases current flow; the valley of the wave reduces it.
This flow diagram shows how an EL84's power comes from electrons flowing from ground, through the tube, through the output transformer, and back to ground. It's a cycle.
An EL84 power tube can produce approximately 5 watts in a single-ended amp. Therefore, you would think two EL84 tubes would produce 10 watts. And that's true: Power tubes can be configured in parallel to double the output power. Consider, for instance a Gibson GA-9 amp, which puts two 6V6 tubes in parallel. It's done, but not often. Why? Because a class AB configuration can produce more than double the power output from two power tubes. But before we get to that….
Make Some Noise, Class B
In a class B amp, each tube carries exactly half of the signal. Because the transfer of the signal from one tube to the other is never perfect, it creates crossover distortion.
In a class B amp, two power tubes share the sine wave. One conducts the first 180 degrees of the wave, and the other conducts the second. It's a push-pull arrangement. Unlike in a class A amp, each tube is at work only half the time. This allows each tube to be pushed further, into higher amplification, during the time it's conducting. To take advantage of that rest time, voltages at the plates can be higher, as can the signals going into the power tubes' grids. If a single EL84 tube can deliver 5 watts in class A, it can deliver twice that in class B during its half of the sine wave. Two tubes, therefore, will deliver four times the power, in theory. In practice, it may be less. Another advantage of a class B circuit is that at idle, neither tube is conducting, so it's a very efficient configuration for power consumption and for tube life.
All of that would be great for a guitar amplifier if the transition from one tube to the other occurred instantaneously. It doesn't. As the sine wave moves from positive to negative and back to positive, there's a delay—a misalignment in the transition between the tubes. The delay creates crossover distortion. Steven Fryette's description: "Crossover distortion can create a fizzy sound in the amplifier, [because] one tube is turned off before the other is fully turned on." And that, in a nutshell, is why class B isn't a common option for guitar amps. Enter class AB.
Class AB—Double the Fun
A class AB circuit solves the crossover distortion problem by having two (or four) tubes overlap responsibilities. Each tube, or each pair of tubes, carries more than half of the 360-degree signal of the sine wave.
In a class AB circuit, two power tubes share the responsibility of conducting the sine wave, similar to class B, but with some overlap. The tubes are set up so that one starts conducting before the other finishes, so each tube conducts for more than 180 degrees of the sine wave. This eliminates issues with the transition from one tube to the other. While not as powerful or efficient as a class B circuit, it's close—and the reason two EL84 tubes can deliver 15 watts in class AB amplifiers.
But if one EL84 delivers 5 watts and two can boost that to 15 watts, why do four only deliver 30 watts? Because in an AB amplifier with four power tubes, the tubes work together in two pairs, with each set delivering exactly twice the power of one tube. In a Vox AC30, for example, each pair of parallel EL84s creates 10 watts. It then puts the pairs in class AB configuration, doubling the output of a two-power-tube-amplifier, like the Vox AC15, from 15 to 30 watts. The diagram here explains that in greater detail.
In a class AB circuit, each power tube get a chance to rest half the time an amp is operating. Because of that, power tubes can be pushed harder when they are conducting.
The Output Transformer Takes Sides
The output transformer converts high voltage and low current on the primary side—which is to say, the tube side—of the circuit to enough low voltage and high current on the secondary—or speaker—side to drive a speaker. An output transformer's primary side is rated in ohms, but ohms in impedance, not resistance. The difference is that impedance takes into account that an AC signal is involved, since resistance will vary significantly depending on the frequency. (Frequency is the number of oscillations per second in the AC signal.) The impedance determines the rate of flow of electrons, with higher impedance being more restrictive.
The Alliance: Speakers and Transformers
It's important to match a speaker's impedance rating with the output transformer, because, interestingly (and maybe somewhat surprising), the impedance on the primary side of the output transformer will change based on the impedance of the speaker you connect on the secondary side. If you connect a speaker rated at half the impedance—for example, put a 4-ohm speaker in place of an 8-ohm speaker—the impedance seen by the tubes will be cut in half. Twice the current will flow on both the tube side and the primary side. The 4-ohm speaker will be louder but can lead to trouble. Your power tubes or output transformer can overheat. It's not risky, however, to put a 16-ohm speaker in place of an 8-ohm speaker, although it won't sound as loud. In discussing this with John Paice at speaker manufacturer Celestion in Ipswich England, he had some simple advice: "Don't do it." Best practice is to match the speaker with the output transformer.
Doubling the wattage of a 15-watt amplifier will increase perceived loudness by 23 percent, not double it. And so, a 5-watt amp would sound 71 percent as loud as a 15-watt amp.
In terms of guitar amplification, we measure—and hear—power and loudness along a logarithmic curve. Doubling the wattage going into a speaker results in a 3 dB increase. At 3 dB more, we're not doubling loudness. It's approximately a 23 percent increase in volume. You can therefore expect a 30-watt amplifier to sound 23 percent louder than a 15 watt amplifier. And a 5-watt amplifier will be 71 percent as loud as a 15-watter.
If mixing speakers in a multi-speaker cabinet, be conscious of each speaker's impedance rating (they should match) and also of each speaker's sensitivity rating, found on its spec sheet. (Sensitivity is usually determined with a microphone connected to a sound level meter placed one meter in front of the speaker. The result is expressed in dB.) Advice from Celestion's Paice: "If mixing speakers, try to keep their sensitivity rating within 3 dB of each other, because any more than that will become noticeable. The more sensitive speaker will dominate the blend."
What’s with Speaker Wattage
A large speaker magnet does double-duty. It will hold the voice coil more firmly, producing more bass. It also acts as a larger heat sink. A Celestion G12M rated at 25 watts incorporates a 35-ounce magnet. A G12H at 30 watts incorporates a 50-ounce magnet. "A bigger lump of metal is better at dissipating heat, so you can put more power into it," explains Paice. In addition to heat, too much power into a speaker can potentially result in too much cone movement, damaging the cone and its surround, and possibly resulting in failure. Nonetheless, a 50- or 100-watt Marshall amp pushing a set of four Celestion 25-watt speakers is a classic sound, employed by Hendrix, Clapton, Page, Slash, and many other guitar heroes. Running multiple speakers in a cab reduces the punishment any single speaker must take. And, of course, using a high-power-rated speaker with a low-power amp can also net good sonic results. "Some people think that you have to put as much power into a speaker as it will take," says Paice, "but you can get lots of breakup with a high-power speaker using just a lunchbox-size amp."
Bactrian Amps, Anyone?
You may be thinking, okay, if doubling watts into a speaker doesn't double the loudness, I'll just use two amplifiers. No, no, no—the same principles apply. Since we hear logarithmically, two 15-watt amplifiers will give you the same output as a single 30-watt amplifier. It's an increase, but not double.
I like going back to the classic 1959 publication on sound and amplification, Basic Audio, Vol 1. by Norman H. Crowhurst. He shows an illustration of two crying babies in a twin stroller, comparing their loudness with one crying baby in a stroller. Two babies are louder, but not twice as loud. So while that physics phenomenon may not work to your advantage as a guitar player, think of how grateful you would be if you were the parent of twins.
Peeling the Onion
Let's take a deeper look inside tubes, output transformers, and speakers.
This diagram shows the ve components within an EL84 tube. Note the minute distance between the grid and cathode. That's the open range for negative-charged electrons.
Under the Glass
Ever wonder what's behind the glass of your amp's tubes? Well, there's a lot going on in your average pentode or triode—electrons charging around, hitting walls, held at bay. Let's examine an EL84, which is a pentode, as is an EL34 and many other power tubes. That means five elements are at work within the tube (not counting the filament, the heating element tucked inside the cathode). Schematic diagrams like the one below portray tubes as if the cathode is on one side of the glass and electrons flow in a straight line through the tube, with all elements evenly spaced.
In reality, the cathode sits vertically in the center of the tube, and its electrons flow outward. When the cathode is heated, a "space charge" of electrons—a cloud of negative-charged particles—form around it like swarming microscopic bees. Because opposites attract, they are instantly drawn to the high positive-DC voltage of the plate. But the grid stops them. The grid is a wrap of thin wires encircling the cathode that carry your guitar's signal. The grid's at-rest charge appears negative to the cathode, slowing the electron flow. There are two ways for the grid to assume that negative appearance, depending on an amplifier's design: Either the grid is connected to a small negative charge or the cathode has a small positive charge. Electrons don't care which method is used. Just ask 'em.
The cathode, grid, and plate are elements common to triodes (three-element preamp tubes, like a 12AX7) and pentodes. The two additional elements inside the pentode are the screen grid and the suppressor grid. Like the guitar-signal grid, they are wraps of thin wire with mostly open areas that allow flying electrons to reach the plate without being blocked. And like the plate, the screen grid carries a high electron-attracting DC voltage, but its voltage, unlike the plate, is consistent, whereas plate voltage will vary with the signal.
The suppressor grid, the outermost wrap of wire closest to the plate, is connected to the cathode and its job is to repel electrons, which hit the plate and bounce off. The suppressor grid sends them back to the plate to avoid power loss. Beam tetrode tubes like the 6V6, which have four elements, incorporate metal plates that serve a function similar to a pentode's suppressor grid, working to keep the electrons in place.
This illustration shows the three grids plus the cathode and plate in a typical pentode tube.
Are Your Tubes Biased?
Sure, you've heard the term bias, but what is it and what does it do for your amplifier? Bias refers to the amount of negative charge the cathode detects on the grid, and it is set to keep the electron flow in check at a happy, medium level. Too negative and not enough electrons will flow when you're playing, so your amp won't produce enough volume and will sound anemic. Too positive you'll be bombarding the plate with too many electrons and overheating it, producing a warm red glow that you don't ever want to see in a tube. At that point, its lifespan could be measured in minutes.
The wattage a tube's plate receives can be determined by multiplying the rate at which electrons flow from the cathode to the plate times the voltage at the plate. The former is measured in amps, and in a cathode-biased amplifier can be calculated by knowing the value of the resistor connected between the cathode and ground, and the voltage drop across the resistor (the "drop" is the voltage measured between one end of the resistor and the other). An EL84 is designed to receive up to 12 watts maximum, and this or just below becomes the target when adjusting the tube's bias. So there you go.
The Many Tasks of Output Transformers
In the main story, we talked about how the output transformer wrangles voltage and works to impede and control the flow of electrons toward the speaker. That's not all it does, but in the process of doing that, it also blocks high voltage DC from streaming through the circuit, which is why you won't get electrocuted touching your speaker connections.
On the primary, or tube, side, the output transformer's impedance rating should more or less match the required impedance for the power tube or tubes being used. That impedance is measured in ohms, on the order of 4,500 ohms for a single EL84 tube, and 8,000 for two in class AB. An output transformer designed for an impedance lower than what the tubes want will lead to too much current flow, overloading the transformer, the tubes, or both. And soon they're kaput.
High voltage on the power tubes' plates also comes from the output transformer, via the rectifier tube or circuit. And that DC voltage is regulated by a large filter capacitor to help smooth out any ripples in voltage.
Yes, Speakers Are Sensitive
There's a rating for how reactive a speaker is to a signal that's typically called sensitivity. Awwww…. A speaker's sensitivity is measured by sending a 1-watt, 1-kHz signal into the speaker and measuring the loudness at 1 meter away.
If 1 watt sounds low, remember that power efficiency of a speaker is also surprisingly low. Most of the power going into a speaker is dissipated as heat. According to Celestion's John Paige, 97 percent of input power becomes heat, and only 2 to 3 percent converts to sound. Years ago, regulations required that speaker voice coils include a fire retardant, because occasionally they'd ignite onstage.
Since speaker sensitivity varies, an easy way to increase or decrease the loudness of an amplifier is to simply change speakers. But here's a quick lesson in sound physics. We measure loudness in decibels, or dB, a unit of sound pressure level, or SPL. Similar to the way we rate the magnitude of earthquakes, decibels are based on a logarithmic scale. So, check out this chart. It illustrates the perceived loudness you might expect for speakers of varying decibels.
And remember, our ears work in a surprising way. To perceive sound as being twice as loud requires an increase of 10 times the sound pressure, or 10 dB. Therefore 70 dB will sound twice as loud as 60 dB, and 80 dB will sound four times as loud as 60 dB. For reference, casual conversation is around 60 dB and 120 dB is jackhammer painful.
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For these new recreations, Fender focuses on the little things that make original golden-era Fenders objects of obsession.
If there’s one thing players love more than new guitars, it’s old guitars—the unique feel, the design idiosyncrasies, the quirks in finish that all came from the pre-CNC era of instrument manufacturing. These characteristics become the stuff of legend, passed on through the years via rumors and anecdotes in shops, forums, and community networks.
It’s a little difficult to separate fact from fiction given these guitars aren’t easy to get your hands on. Fender Telecasters manufactured in the 1950s and 1960s sell for upwards of $20,000. But old is about to become new again. Fender’s American Vintage II series features 12 year-specific electric guitar and bass models from over two decades, spanning 1951 to 1977, that replicate most specs on their original counterparts, but are produced with modern technologies that ensure uniform build and feel.
Chronologically, the series begins and ends, fittingly, with the Telecaster—starting with the butterscotch blonde, blackguard 1951 Telecaster (built with an ash body, one-piece U-shaped maple neck, and 7.25" radius fretboard) and ending with the 1977 Telecaster Custom, which features a C-shaped neck, a CuNiFe magnet-based Wide Range humbucker in the neck position, and a single-coil at the bridge. The rest of the series spans the highlights of Fender’s repertoire: the 1954 Precision Bass, 1957 Stratocaster in ash or alder, 1960 Precision Bass, 1961 Stratocaster, 1963 Telecaster, 1966 Jazz Bass, 1966 Jazzmaster, 1972 Tele Thinline, 1973 Strat, and 1975 Telecaster Deluxe. The 1951 Telecaster, 1957 Strat, 1961 Strat, and 1966 Jazz Bass will also be offered as left-handed models. Street prices run from $2,099 to $2,399.
Fender '72 American Vintage II Telecaster Thinline Demo | First Look
Spec’d To Please
Every guitar in the series sports the era’s 7.25" radius fretboard, a mostly abandoned spec found on Custom Shop instruments—Mexico-made Vintera models, and Fender’s Artist Series guitars like the Jimmy Page, Jason Isbell, and Albert Hammond Jr. models. Most modern Fenders feature a 9.5" radius, while radii on Gibsons reach upwards of 12". Videos experimenting with the 7.25" radius’ playability pull in tens of thousands of viewers, suggesting both a modern fascination with and a lack of exposure to the radius among some younger and less experienced players.
T.J. Osborne of the Brothers Osborne picks an American Vintage II 1966 Jazzmaster in Dakota red.
Bringing back the polarizing 7.25" radius across the entire series is a gamble, and it’s been nearly five years since Fender released year-specific models. But Fender executive vice president Justin Norvell says that two years ago when the Fender brain trust was conceptualizing the American Vintage II line, they decided the time was right to “go back to the well.”
“We’ve been doing the same [models], the same years, over and over again for 30 years,” says Norvell. “We really wanted to change the line and expand it into some new things that we hadn’t done before and pick some different years that we thought were cool.”
“It takes a lot of doing to go back in time and sort of uncover the secret-sauce recipes.”—Steve Thomas, Fender
To decide on which years to produce, Fender drew from what Norvell calls a “huge cauldron of information” from Custom Shop master builders to collectors with vintage models to former employees from the 1950s and 1960s. The hands-on manufacturing of Fender’s golden years meant guitars produced within the same year would have marked differences in design and finish. So, the team had to procure multiple versions of the same year’s guitar to decide which models to replicate. Norvell says some purists would advocate for the “cleanest, most down-the-middle kind of variant,” while others would push for more esoteric and rare versions. Norvell says that ultimately, the team picked the models that they felt best represented “the throughline of history on our platforms.”
Simple and agile, the Fender Precision Bass—here in its new American Vintage II ’54 incarnation—earned its reputation in the hands of Bill Black, James Jamerson, Donald “Duck” Dunn, and other foundational players.
Norvell says the American Vintage II series was developed, in part, in response to calls to reproduce vintage guitars. Just like with classic cars, he says, people are passionate about year-specific guitars. Plus, American Vintage II fits perfectly with the pandemic-stoked yearning for bygone times. “For some people, these specific years are representative of experiences they had when they were first playing guitar, or a favorite artist that played guitars from these eras,” says Norvell. “These are touchstones for those stories, and that makes them very desirable.”
Fender’s electric guitar research and design team, led by director Steve Thomas, dug through the company’s archive of original drawings and designs—dating all the way back to Leo Fender’s original shop in Fullerton, California. They found detailed notes, including some documenting body woods that changed mid-year on certain models. Halfway through 1956, for example, Stratocaster bodies switched from ash to alder. That meant the American Vintage II 1957 Stratocaster needed to be alder, too. That, in turn, meant ensuring enough alder was on hand to fulfill production needs.
Among the series’ Stratocaster recreations is this 1973-style instrument, with an ash body, maple C-profile neck, rosewood fretboard, and the company’s Pure Vintage single-coils.
Thomas and his team discovered another piece of the production puzzle when researching how pickups for that same 1957 Strat were made. “We realized that if we incorporated a little bit more pinch control on the winders, we could more effectively mimic the way pickups would have been hand-wound in the ’50s,” says Thomas. “It takes a lot of doing to go back in time and sort of uncover the secret-sauce recipes.”
Thomas proudly calls the guitars “some of the best instruments we’ve ever made here in the Fender plant,” pointing to the level of detail put into design features, including more delicate lacquer finishes which take longer to cure and dry, and vintage-correct tweed cases for some guitars. New pickups were incorporated in the series, like a reworking of Seth Lover’s famed CuNiFe Wide Range humbuckers, which were discontinued around 1981. Even more minute details, like the width of 12th fret dots and the material used for them, were labored over. Three different models in the line feature clay dot inlays at unique, year-specific spacings.
Ironically, modern CNC manufacturing now makes these design quirks consistent features in mass-produced instruments. While the hand-crafted guitars from the ’50s and ’60s varied a lot from instrument to instrument. “Everything needs to be located perfectly, and it wasn’t necessarily back in the day,” says Norvell. “Now, it can be.”
Don’t Look Back
With this new series so firmly planted in the rose-tinted past, Fender does run the risk of netting only vintage-obsessed players. But Norvell says the team, despite being sticklers for period-correct detail, sought to strike a balance between vintage specs, practicality, and playability. The 1957 Stratocaster, for example, has a 5-way switch rather than the original’s 3-way switch. Norvell also asserts that the “ergonomic” old-school radius feels great when chording. “It might not be [right for] a shred machine, but it feels great and effortless.”
The 1966 Jazz Bass is also represented, shown here in a left-handed version.
Norvell also pushes back on the notion that Fender is playing it safe by indulging nostalgia and leaning on their past successes. He says that while the vintage models are some of the most desirable on the market, the team “purposely did not stick to the safe bets,” citing unusual year models like the 1954 P Bass and the 1973 Stratocaster.There’s a good reason why anything that hails back to “the good ol’ days” hits home with every generation. We’re constantly plagued by a belief that what came before is better than what we’ve got now. But with the American Vintage II series, Fender makes the case that guitars from the ’50s, ’60s, and ’70s can very easily be a relevant part of the 2020s.
Module 4 was designed to be a highly versatile take on a classic vintage compressor - Dan Armstrong's Orange Squeezer from the ‘70s.
The Module 4 can be transformed to a standard 'Full Frequency' range compressor by pushing the Orange button. Basically, the user gets two compression flavors and they are easily distinguishable. Orange brings a warm, vintage sound and feel while 'Full Frequency range' brings a more modern, brighter, clearer tone. The pedal is equipped with several colorful, and practical options, all packed into the new DryBell enclosure line.
- Output - Controls the output volume (make-up gain) of the compressor. It also acts as a high headroom and distortion-free clean Boost, thanks to the high internal power supply voltage
- Tone - Controls the overall high-frequency spectrum of the unit Blend - Sets the mix of dry and compressed signals
- Attack - Controls the reaction time of the compressor
- Release - Controls the time before the unit releases or stops compression
- Preamp - Controls the input gain of (any) instrument
- ORANGE pushbutton - Enables/disables the ORANGE mode. When the ORANGE mode is off, Module 4 becomes a 'Full Frequency range' compressor
- Expander - Automatically attenuates incoming background noise
- 3-color compression level meter - A visual representation of gain reduction and input signal level
- LOW END cut – Option to keep or remove certain low-end frequencies
- True bypass or buffered bypass options
- Orange button also works in buffered bypass when the pedal is turned off. In that case, the buffered bypass reacts like the Orange Squeezer’s Front-end, keeping the bypass EQ very similar to the EQ when the pedal is active
- Power on settings save option
- Dot marks around knobs - Represent the settings of the original OrangeSqueezer
- Standard power supply 9-18V DC, 100mA minimum
DryBell Module 4 is available for $315.00. The first batch of Module 4s is available exclusively from the DryBell webshop.
For more information, please visit drybell.com.
DryBell Module 4 demo (official)
The Flat Earth has minimal knob count and feed-forward compression circuitry.
The Mayfly Flat Earth uses Feed-Forward circuitry which determines the amount of compression by analyzing the signal before it’s compressed. Old school compressors (you know: the Red one, the Orange one, the Grey one)use Feed-Back circuitry which looks at the signal after it’s already compressed. This results in noise, pumping, and tone-loss.
Boutique pedals based on older designs try to get around these problems by adding more knobs: blend knobs, tone knobs, etc. According to Mayfly Audio, "The Flat Earth has minimal knob count to allow guitarists to get to ‘wow’ quicker."
- Feed-forward compression circuitry: great compression that’s easy to setup
- No pumping or other compression artifacts
- Very low noise floor, very low distortion
- Level, sustain, and attack controls. That’s all you need
- Full bypass using relays with Fail Safe (automatically switches to bypass if the pedal loses power)
- Cast aluminum enclosure with stunning artwork
- MSRP $149 USD ($199 CAD) direct online
Introducing the MayFly Flat Earth Compressor
For more information, please visit mayflyaudio.com.
This pedal combines boutique high gain & Swedish chainsaw mayhem in collaboration with award-winning metal engineer Glenn Fricker.
The Canadian metal masters are on a mission with award-winning engineer Glenn Fricker to inject some mayhem back into your metal. One half of the Northern Mauler is an unforgettable sonic assault inspired by the iconic HM-2 sound of Swedish Death Metal & American Hardcore. The other is the punchy high gain Revv is known for;custom-tuned to Glenn’s specs. Blend freely between the 2 circuits to find your own unique, memorable sound into a wide variety of setups.
"I've been wanting to mix the Swedish Chainsaw into modern metal tones for quite a while now. So I reached out to the guys at Revv, & after many months & many revisions, we've come up withThe Northern Mauler. This combines the best of Revv's wonderful super-tight metal tones with the out-of-control nastiness of the Chainsaw... & the results are better than I could have hoped for! We even kept the labeling simple so even the bass players could use it!” -Glenn Fricker
The Revv Glenn Fricker Northern Mauler features:
- Seamlessly combine Revv’s boutique high gain & Swedish chainsaw mayhem in collaboration with award-winning metal engineer Glenn Fricker.
- Embrace the chaos by blending in a grimy, out-of-control sound that gives your tone character & makes it memorable.
- A punchy new voice of Revv high gain amp tone & Revv’s homage to the legendary HM-2 in one pedal.
- Optimized for use with clean amps, high gain amps, power amps, &direct to interface with impulse responses.
- True bypass, top jacks, & 9v (20mA) center negative external power supply operation.
- Gloss white finish w/ custom bear graphic & Glenn Fricker signature.
- Manufactured in Canada to rugged quality standards w/ 2-year registered limited warranty.
Revv Glenn Fricker Northern Mauler | Performance Demo & Specs
The Revv Glenn Fricker Northern Mauler has a street price of $249. For more information, please visit revvamplification.com.