The non-electronic tech's guide to understanding the classic 5E3
tube amplifier.
By Rob Robinette
'5E3' was Fender's internal model designation for the 1957 tweed
Deluxe. The February 1957 Fender price list shows the Deluxe at
$129.50 which is equal to $1,145 in 2017 inflation adjusted dollars.
Fender 1957 Catalog
The Deluxe retailed for $129.50
There were several other models of the 'Deluxe' but the
5E3 is by far the most popular. The 5E3 amp kit phenomenon is still going strong so there's
lots of new tube amp guitarists that would like a not-too-technical explanation
of how the amp works, what each component does, and how changing those
components will affect the amp's voice.
I recommend you take a look at my How Tube Amps Work and How Vacuum Tubes Work webpages for a detailed
explanation how vacuum
tubes work in the very simple Fender 5F1 Champ guitar amp. I won't be going over
tube theory and other introductory material here so check it out if you have
trouble understanding this webpage. For information on the
evolution of the Fender Deluxe and
Deluxe Reverb circuit see this. If you like to mod your amps check out my
5E3 Modifications webpage. I also have a
page dedicated to the magical 5F6-A Bassman
amp.
The 5E3 Chassis
Controls on top, Circuit Board inside, tubes on bottom right to left: V1
Preamp, V2 Preamp & Phase Inverter, V3 and V4 Power Tubes, and V5
Rectifier Tube at far left. The Power Transformer and
Output Transformer are attached to the other side of the chassis. Photo and
chassis by Bob Arbogast.
Some of the elements that give the 5E3 Deluxe such a
unique voice are its funky interactive volume and tone controls and it's
raw, deep voice. Both volumes and the tone controls all interact to create some
unique tones. Its rawness comes from both preamp gain stages having bypassed
cathodes for maximum gain and with no negative feedback loop breakup comes on
early. This leads to little headroom, early dirt and a lazy
transition from clean to distortion.
The 5E3's very
large coupling and bypass capacitors give the amp more bass response than most
but this can lead to boominess and 'farting out'. Amplifying all those low
frequencies uses a lot of power and can overwhelm the power supply circuit which
leads to voltage sag, output volume compression and 'note bloom.' The relatively
small output transformer also contributes to output volume compression. Its
cathode biased power tubes sound rounder, tubey and warm compared to more modern
fixed bias amps. Its old school, almost no gain
cathodyne phase inverter doesn't drive the power tubes as hard as amps with a
long tail pair phase inverter. From a modern perspective the 5E3 Deluxe
has many design 'defects' but they come together to create a unique and beloved
tone that's still gaining in popularity.
We'll start the analysis of the 5E3 Deluxe with my annotated versions of the original Fender
schematic and layout diagrams for a broad overview of the amp's function then
we'll dive deeper and examine individual components and their value tweaking.
The 5E3 Deluxe Schematic with Signal Flow and Annotations
Click the image to view the full size (readable) annotated schematic.
A pdf version is
here.
The amp's signal flow in the schematic above is shown by the thick grey line
from the input jack at upper left to the speaker at upper right (to see the larger, readable version
of a diagram on this page just click on the diagram). The very low level AC signal voltage
from the guitar's coils enters the amplifier at upper left through one of the
4 Input Jacks. Typical signal level from the guitar pickup coils is about
0.1 volt AC rms but can vary greatly
due to the number of pickups, their design and of course how and what is played
on the guitar. Quiet jazz played on a guitar with a vintage single coil can
produce signals below the single digit millivolt range (0.001v).
The 5E3 has 2 channels, the Normal and Bright Channel. The Bright
Channel is brighter because of the addition of a single component, the Bright
Capacitor or Brite Cap, which allows high frequencies to bypass the Bright Volume control at
lower volume settings. The lower the volume the more highs are bypassed so the
Bright Channel is usually preferred for lower volume playing. At max
volume the Bright Cap does nothing and the Bright and Normal Channels are
identical. The
original Fender Bright Cap was 500 pF (pico Farads) but modern standard cap
values have made it convenient to use an equivalent 470pF instead. Using a larger value
Bright Cap will allow lower frequencies to pass around the Bright Volume
control. Using a smaller value Bright Cap will
raise the cutoff frequency so less mids would be affected. The Fender 5F6A
Bassman used a tiny 100pF Bright Cap so only very high freqs were passed
around the volume control. Many modern guitar
amps use a mid size 250pF Bright Cap.
The 5E3 Deluxe is famous for it's control interaction. Both volume
controls and the tone control all interact with one another even when only one
channel is in use. Changing the volume level of the unused channel will alter
the tone and breakup of the channel in use.
Both volume controls alter how the tone control functions. When the 5E3's Bright
channel volume is turned full down its bright cap is connected directly to
ground on one end and connected to the bright end of the tone pot on the other.
The bright cap then acts as a high freq tone cap that bleeds high freqs to
ground. It's not a huge effect but the brightest setting on the tone control
moves to less than max on the tone dial. This only occurs when the Normal
channel is in use, the Bright channel does not suffer from this control quirk.
It's another reason (besides the bright cap) the Bright channel is brighter than
the Normal channel.
The unused channel volume pot and 100k plate load resistor change the load on
the channel in use and therefore affect the gain. The unused channel load can
run from 100k at max volume to 1M at min volume. Turning the unused channel
volume full down offers up the most preamp gain.
To get the most
out of the 5E3 you must play around with all three controls--especially at
high volume levels. This is where much of the 5E3 Deluxe's magic resides.
Here's an informative quote on setting the controls from clintj, "So, one setting
combo that gets me a good amount of warm breakup is this: in-use volume control
on 8 or 9, unused volume set on 4, tone set to at least 9. Adjust your unused
volume down for more dirt, up for less, zero should get you in Neil Young
territory."
Each channel has two input jacks, a Hi and Lo. The Lo jacks'
inputs run through a voltage divider formed by the two 68K Grid Stopper
resistors which cuts the guitar
signal in half (-6dB). If you find that you prefer the Lo input jacks you should consider using
the Hi jacks and just turn down the volume on your guitar which gives you the
same signal level but you'll have control at the guitar. You should also try
"jumpering" the channels together. Plug a short cable into two jacks in the
normal and bright channels for a thicker tone that's paralleled through both
channel's preamps (example: guitar is plugged into Bright Hi jack then jumper
from the Bright Lo jack to the Normal Hi jack). For the graduate level explanation of how the jacks work and how jumpering the two channels together works
see this.
Jumpering Channels
Bright - Hi input used with 6" patch cable between Bright - Lo and Normal
- Hi. Photo by sookwinder.
Each channel has an Input Resistor on its Hi Input Jack. The Input
Resistors set the amp's input impedance and they act as tube V1's grid leak
resistors. For best signal voltage transfer from guitar
to amp you want a low impedance from the guitar and a high
impedance for the amp (at least 10 times more impedance for the amp is a guide
called "the rule of 10"). This intentional impedance mismatch trades guitar
pickup coil current for voltage--this is called impedance bridging. 1 megaohm is a standard
value for most all guitar amps so there's no reason to tweak its value. A higher
value would add impedance but also add noise. A lower value would decrease noise
but reduce the voltage signal from the guitar. Some high gain amps use lower
value grid leak resistors to intentionally attenuate the signal to control gain
between amplifier stages.
In the
50's and 60's carbon composition resistors were used and if you want your
amp to look 'period correct' then use them but metal film resistors are
over 10 times quieter than carbon comp so use them if you want the best quality
audio and lowest noise. Resistors generate the white noise hiss you hear when
the amp is turned up to max with no guitar plugged into the amp. The input and
grid stopper resistors
are a good place to use metal film resistors because
their hiss will be amplified by every gain stage.
Grid Stopper resistors help stabilize the amplifier by removing much of
the audio signal above human hearing. [Bonus info: The
Grid Stoppers also act as 'mixing resistors' to
prevent interaction between two simultaneous Hi and Lo inputs like two guitars or a guitar
and microphone] The Hi input uses both 68k grid stoppers in parallel so
the grid stopper resistance is actually 34k. Grid stop resistors on the first
amplifier stage do remove some high freqs from the guitar signal so some modern
amps use smaller grid stoppers and some amps do without them altogether. You can
use an alligator clip wire to jumper around the grid stopper resistors to try
the amp with lower or no grid stopper resistance but the difference is very subtle and
only affects very high frequencies but it may add some "sparkle." The
optimal location for a grid stopper resistor is on the tube grid (input) pin
itself so there's no bare wire after it to act as a radio antenna to pick up
radio frequency interference (RFI).
5E3 Layout with Signal Flow and Annotations
Click the image to view the full size (readable) annotated layout. Notice how
convoluted the signal path (thick grey lines) is compared to the schematic. A schematic shows
electrical flow while a layout diagram shows the physical location of the amp's
components.
The Input Resistors act as tube V1’s grid leak resistors.
The volume pots act as the tube V2A grid leak.
Load Resistors transform the amplification
stage from current to voltage amplification.
Coupling capacitors block the flow of high voltage DC but pass
the AC guitar signal voltage to the next amplifier stage.
Cathode Resistors set the cathode bias voltage.
Cathode Bypass Capacitors allow signal voltage to bypass the
cathode resistor to boost gain.
The Output Transformer steps down voltage but steps up current
to drive the speaker voice coil which is a simple electromagnet.
After going through the grid stopper resistors the audio signal flows down the wire to the
preamp tube's pin 2 (control grid), which is the entry to the 'A' half of the preamp tube (V1A).
It's called V1A because tubes were called 'Valves' and this is tube number
1 and we're using half of the tube, the 'A' triode. A triode has three
electrodes, a grid, cathode and plate (anode).
12AY7 is the type of tube and it's really two tubes in one
(dual triode). The grid is the 'control valve' that controls the flow of
electrons through the tube. The AC guitar audio signal charges the grid
positively and negatively as it alternates. A positive grid will allow electrons
to flow from the cathode, through the grid to the plate. A negatively charged
grid will block the flow of electrons through the tube. See How Tubes Work
for more info.
Notice that tube V1 has only one cathode resistor valued at 820 ohms. It is
shared by both triodes (both halves) of V1 so the cathode resistor is
approximately half the value of a cathode resistor used for a single triode such
as V2A's 1.5k cathode resistor. Two triode circuits sharing one cathode resistor
will pull twice the current through it so you have to cut the resistance in half
to get the same voltage drop across the resistor. The voltage drop across the
cathode resistor puts the cathode at a positive voltage compared to the control
grid (normally around +1.7 volts DC). This voltage difference is the triode's
bias. Some modern high gain amps bias their preamp triodes cooler using a 2.7k
cathode resistor or bias it hotter with an 820 ohm resistor. Both will reduce headroom and boost preamp distortion. Increasing the
cathode resistor value also reduces gain and decreasing it will boost gain.
The hottest bias for a preamp gain stage I have ever seen in a commercial amp is
an 820 ohm cathode resistor (not shared). The coldest bias I have seen is a 39k
cathode resistor in a Soldano high gain amp. The very high value cathode
resistor is designed for early clipping to intentionally generate preamp
distortion. This type of preamp stage is called a
Cold Clipper and
was first used in the Marshall 2204
amplifier.
The 5E3 uses a 12AY7 preamp tube for the first gain stage. You can substitute a
higher gain 12AX7 to boost amplification, reduce headroom and increase breakup
and distortion. The preamp tube amplifies the guitar audio signal then sends it
out pin 1 (plate) to a coupling capacitor or 'cap.' Coupling caps are
sometimes called 'blocking caps' because they block DC (direct current) voltage.
DC flows in only one direction where AC (alternating current) alternates its
direction of flow--the electrons actually change direction and move back and
forth through a circuit.
High voltage DC power used by the tube is brought in through the load resistor.
Load resistors change the amplification stage from a current amplifier to a
voltage amplifier. Many modern amps have load resistor bypass capacitors to remove
frequencies above human hearing to stabilize the amplifier and prevent
oscillation in high gain amps. You can also remove "ice pick highs" with a load
resistor bypass cap.
The wire between tube pin 1 (plate) and the load resistor carries up to 250 volts DC.
This wire carries the AC audio signal out while simultaneously bringing in the high voltage DC power the tube
needs to function. Coupling capacitors allow the AC audio signal to pass through
but block the high voltage DC and keep it from flowing into the following amp
stage.
How capacitors block DC but let AC pass: Caps are actually made with
sandwiched conductive plates but I like to visualize them
as having a stretchable rubber membrane inside that blocks the flow of
electricity. When voltage is applied to a capacitor the 'rubber
membrane' stretches and bulges as electrons try to flow through it. The higher
the voltage the more the membrane bulges. If you quickly reverse the
capacitor's voltage polarity it will go from bulging one way to bulging the
other way. This is what a small AC signal does--it stretches the 'membrane' back
and forth as the voltage alternates which allows electrons on both sides of the
capacitor to move back and forth (alternate) but a constant DC voltage that is trying to flow in one direction will be blocked by the membrane.
Capacitors are made of two conductive plates separated by an insulator or
dielectric. Common dielectrics are mica, polypropylene, ceramic, paper and even
oil.
The Fender 5E3 Deluxe uses very large value .1uF (micro Farads) coupling capacitors which allow low frequencies to
flow through the amp. These low frequencies use a lot of power and
cause the 5E3's infamous "loose low end" and can lead to severe
blocking distortion known as "farting out." Reducing
the value of the coupling caps will filter out some lows and tighten up the amp
and make the amp more humbucker pickup friendly. The overdrive tone will also
tighten up. Modern, high gain amps use extremely small coupling caps
(0.0022uF) to reduce bias drift, blocking distortion and keep
the overdrive tone tight. See my Tube
Amp Overdrive page for more info. Some people lower the value of the 5E3 coupling cap in
only one channel and leave the other channel alone so you can choose between
standard Deluxe or a tighter, more modern tone (see the
Voice a Lead Channel mod). Smaller coupling caps can
also improve the way the 5E3 works with FX pedals, especially gain boost, delay
and reverb pedals.
Another way to trim the 5E3's low end 'fat' and tighten up the amp is to reduce
tube V1's or V2A's cathode bypass capacitor. Both have a 25uF 25v
cap that is large enough to boost all guitar frequencies but many modern amps use a
bypass cap as low as .68uF (680 nano Farads) to boost only mid and high freqs. If you wanted to
alter just one of the 5E3's channels you'd have to separate the V1A and V1B cathodes
by adding another cathode resistor and bypass cap (see the
Voice a Lead Channel mod).
After the coupling cap the guitar audio signal flows to the volume and tone potentiometers (pots).
The volume pot acts as a variable voltage divider which when turned down
will attenuate the signal voltage. Volume knob left = less voltage signal and lower
volume. Volume knob right = more voltage signal and higher volume.
Changing the volume pots from 1 meg to 500k (1 million ohms to 500,000 ohms)
will send more signal to ground and attenuate the signal path.
[Bonus info: The volume pots also function as V2A's grid
stopper and grid leak resistors]
The tone pot in combination with
the tone capacitor create a variable RC (resistance capacitance) low pass
filter which removes high frequencies by shunting them to ground. Using a higher
value tone cap will lower the cutoff frequency of the tone control so it will
affect more mid frequencies. Reducing it will raise the cutoff frequency and
affect less mid freqs.
The guitar signal next flows to tube V2A's pin 7 (grid). This stage acts
as the second gain stage which boosts the guitar signal voltage. The audio signal leaves tube V2A via pin 6 (plate) and
flows to another coupling cap that blocks DC. The signal then flows to V2B,
the cathodyne phase inverter where the guitar signal is split into two
streams for the two power tubes. The signal enters at V2B's grid and flows out
its plate to a coupling cap and on to power tube V3's grid. This signal is
inverted compared to the phase inverter input. The signal also flows out V2B's
cathode to a coupling cap and on to power tube V4's grid. This signal is not
inverted so the two signals flowing to the power tubes are 180 degrees out of
phase--mirror images of one another--one is inverted and one isn't. Unlike the
5F6A Bassman's long tail pair phase inverter, the 5E3's cathodyne phase
inverter barely amplifies the guitar signal. It's differential gain factor is always slightly
lower than 2. If you upgrade the 5E3 to run big 6L6 power tubes the cathodyne
phase inverter won't be able to drive them to full distortion the way a long
tail pair phase inverter can.
After the phase inverter the guitar signal flows through another coupling cap to
block high voltage then to the power tube grid stopper resistors. Like
the preamp grid stopper resistors they help filter out noise above human hearing
to prevent oscillation but they also perform another important function, they help control blocking distortion to keep
the overdrive tone sweet even when pushed very hard. Like all grid leak
resistors you can use the
power tube grid leak resistors value to control the input signal voltage. A larger
value grid leak will cause less signal attenuation and a smaller value will
increase attenuation. Typical power tube grid leak values are 100k and 220k.
The power tubes, V3 and V4, are sometimes referred to as the
output
tubes. While the preamp tubes have three electrodes: Cathode, control grid and
plate (a tube with 3 electrodes is called a triode) the power tubes are pentodes
with five electrodes: Cathode, control grid (g1), screen grid (g2), suppressor
grid or beam forming plates (g3) and plate. The screen grid is held at a constant, high positive
voltage to help pull free electrons from the cathode, through the control grid
to the plate. The suppressor grid helps prevent electrons from bouncing off the
plate. It is tied directly to the cathode.
Although the 5E3 doesn't have them, screen grid resistors
are used in most amps to prevent tube damage from excessive screen grid current.
These resistors are usually between 470 to 1500 ohms and rated for 3 or 5 watts
of heat dissipation. The 6V6GT is a beam pentode and therefore flows little
screen current so the 5E3 can get away with running without screen grid
resistors. But if you want to run non-beam, true pentodes like the EL34 then you
should install 1k 5 watt screen resistors. Screen grid resistors will also
increase the screen voltage drop when screen current flows which will increase
the amount of power tube distortion caused by screen voltage drop. Adding a 470
ohm 3 watt resistor to the 5E3 can add sweet sounding power tube distortion so
it is a modification to consider.
The power tubes are the final stage of amplification. Where the
preamp tubes are voltage amplifiers, V3 and V4 are power amplifiers (power = voltage x current) and
their output is expressed as watts. The guitar signal enters at pin 5 (control grid) and leaves via pin 3 (plate)
and flows through the output
transformer (OT).
The output transformer's primary and secondary windings are really just two wire coils
wrapped around an iron core. The
input, or primary coil winding uses electric current flowing through the coil to
generate a magnetic field or flux. This magnetic field fluctuates with the AC
signal voltage. The magnetic flux flows around the transformer iron core to the secondary coil
which generates a voltage in the secondary coil winding. You can alter the
voltage and current from primary to secondary by changing the ratio of coil
wraps from primary coil to secondary.
Transformers
Current flowing into the primary winding induces magnetic flux flow around the transformer core which in turn induces an
electric current in the secondary winding. Put fewer wire wraps on the secondary
(output) winding and its voltage will decrease (step down) but its current will
increase. Most guitar amp transformers are of the 'shell' type (bottom of diagram) and made with laminated iron magnetic cores.
Example: The primary winding has 200 wraps of wire in its coil
and the secondary has 100 wraps. If a 10 volt 1 amp alternating current is applied to
the primary winding the secondary will generate 1/2 of the voltage but twice the
current so 5 volts and 2 amps would be put out by the secondary winding. This is
what an amplifier's output transformer does, it steps down the signal's voltage but steps
up the current because the speaker's voice coil needs current to move the
speaker cone.
At high volume the 5E3's output transformer reaches saturation
which tends to compress the signal. Once saturated an output transformer can't
flow any more flux or get any louder so loud notes are capped but softer notes are still amplified so
there's less volume difference between loud and soft guitar notes. Upgrading the
5E3 to a larger, higher watt rated output transformer will boost maximum volume
and reduce compression (the output will be more dynamic, accurate and solid
state sounding)--but some of the Deluxe's magic lies in its high
volume compression.
The output transformer's primary takes in a high voltage, low
current signal (high impedance) and puts out a low voltage, high current signal
(low impedance). Typically about 320 volts of swing from the power tube plates
flow into the output transformer primary and about 12 volts AC flows out the
secondary through the
blue wire to the speaker jack and on to the speaker.
The speaker jack has a built in switch that grounds the output transformer's
secondary when no speaker is plugged in. It does this because if you power up
the amp with no speaker connected the output transformer will generate very high
voltage in the secondary winding and fry itself if it sees an open circuit. The
ground switch on the jack gives the transformer secondary a closed, short
circuit which it can handle much better than an open circuit. Always have a
speaker connected to a tube amp when you power it up. The aux jack is
tied directly to the main speaker jack's tip and ground. Because of the main
jack's ground switch you must have a speaker plugged into the main jack for
the aux jack to function. You should use an 8 ohm aux speaker along with the
cab speaker which will give the amp a 4 ohm load which Fender considers safe for
the amp. A 4 ohm aux speaker will give the amp a too low load which will reduce
output and stress the power tubes.
From the speaker jack the signal moves on to the speaker. The
alternating current audio signal flows
through the speaker's voice coil which generates a magnetic field. The
voice coil is simply a single wire wrapped into a coil as shown below. The
magnetic field created by the voice coil is either attracted to or repelled by the speaker's magnet. Positive
voltage in the voice coil generates a repulsive magnetic force and the speaker coil and cone moves outward away
from the speaker magnet. Negative voltage generates an attractive magnetic force and pulls the speaker
cone
inward. The speaker cone alternates between moving outward and inward as
the guitar signal voltage alternates between positive and negative.
Speaker Voice Coil is an Electromagnet
Electric current flowing through the speaker's voice coil
generates a magnetic field. When the audio signal electric current reverses the magnetic
field also reverses causing attraction and repulsion to the speaker magnet.
This
in and out movement of the voice coil and speaker cone creates air
pressure waves that our ears perceive as sound--the sweet sound of electric
guitar. For every movement of a guitar string the amplifier generates a
corresponding movement of the speaker cone. When the speaker cone moves
outward a positive air pressure wave is created and when the cone moves inward a
negative (low pressure) wave trough is generated. These air pressure waves move
our ear drums in and out. The ear drum movement is translated into neuron
activity which is sent to the brain where pleasure is created, thus electric
guitar + amp = pleasure.
Speaker
The 'voice coil' is an electromagnet that interacts with
the speaker magnet. The 'spider' supports
the voice coil but allows it to move in and out freely.
So the main purpose of the 5E3 guitar amplifier is to take the tiny
electrical signal generated by the guitar's pickup and make it strong enough to
push and pull a speaker cone. The guitar amp is also used to shape the tone
and control distortion giving us the clean, mellow sound of jazz guitar
or the animal growl of hard rock. Distortion is an important part of guitar
amplifier design and this is the primary difference between guitar and audio
amplifiers. Audio amps are usually designed for absolute minimum distortion.
See
Tube Guitar Amplifier Overdrive for specific information on how
overdrive distortion is created.
5E3 V2A Load Line Chart
The 5E3's V2A is a very generic gain stage with a nice
center bias for maximum headroom and symmetric clipping. Note the color coded legend at upper right.
Load line in red, cathode load line
in magenta, AC load line in yellow and operating point
(bias point) in green. For information on how these lines were charted
see How to
Draw Load Lines.
Power Supply
Now that we've covered the signal flow I'll go back and cover
the other amplifier components that I didn't mention. Wall plug power of 120 volts AC (or
100, 220 or 240 volts AC in
other countries) runs through the fuse and on to the power switch.
The fuse is a 2 amp slow blow fuse. Slow blow means it
won't blow instantaneously when the turn-on power surge runs through it.
Sustained current greater than 2 amps is required to blow the fuse.
120 AC volts RMS (DC equivalent average) wall power equals 339.4 volts peak-to-peak.
After the amp's fuse and On/Off switch the 120v AC runs to the power
transformer (PT), through its primary winding, then back to the wall plug
via the white neutral wire*. The power transformer has three secondary windings.
The first winding steps the 120v AC up to 650 volts AC. Two other small
secondary windings step the 120v AC down to 6.3 volts AC and 5 volts AC (notice
all voltages output by transformers are always AC). The 6.3 volts is used to
power the pilot light and heat the preamp and power tubes' heater filaments
which heat the tubes' cathodes. The 5 volts is used to
heat the rectifier tube's cathode.
*Bonus Info: When I first
learned that the power transformer primary coil was made up of one long wire
that directly connects the 120v hot wire to the neutral (ground) wire I wondered
why it didn't short out. The reason is the primary and secondary coils are
coupled together by the transformer's iron core. Alternating current in the
primary coil creates a magnetic field or flux that is captured by the core. That
flux flowing around the core creates an AC voltage in the secondary coil. The
load (impedance) placed on the secondary winding by the amplifier is transferred
through the core to the primary coil. That impedance keeps the primary coil from
"shorting out."
The 650 volts AC power from the
power transformer is fed directly into V5, the 5Y3 rectifier
tube. V5 is a full wave dual plate rectifier tube that converts
alternating current (AC) into direct current (DC), which the amplifier's
electronics actually need to function. The power transformer and rectifier tube
have internal resistance that cause voltage sag when higher current is
demanded. Installing a higher rated power transformer can reduce voltage sag and
"stiffen" the amp's tone, make it sound "punchier" and help
tighten the bottom end.
370 volts of DC flows out of the rectifier tube's pin 8 (cathode) and is referred to
as B+ or B+1 voltage (from old Battery Positive designation). You can
raise the DC voltages in the amp by swapping out the 5Y3 rectifier tube for a
higher output tube but be careful because your 6V6 power tubes can be damaged by
too high a plate voltage. Higher amp voltage tends to increase output power,
tighten up the tone and make it "punchier."
The B+1 DC voltage flows to the output transformer's primary winding and
to the circuit
board's three large filter/reservoir capacitors and two voltage dropping
resistors. These
resistors and capacitors form RC (resistance capacitance) low pass filters that take the lumpy, pulsing DC output of the rectifier tube and smooth it
out--the smoother the better. Any waves or ripples left over in the DC power
would be added to our audio signal and heard as 120Hz hum in the preamp and power
tubes. The filter caps also act as a power reservoir so the larger the value of
the capacitors the "stiffer" the amp sounds because the amp can react to power
demands with less voltage sag. Low frequencies demand more power so larger
capacitors can really help the low end and prevent "farting out."
Notice the resistors between the filter caps. These are
voltage dropping or step down resistors that reduce the 370 volts DC B+1
down to 295 volts DC B+2 then to 250 volts DC B+3. The B+1 voltage from the rectifier is tapped off
to feed directly to the output transformer's primary center tap which feeds the power
tubes' plates. The 295 volts DC B+2 is connected to the power tubes' pins 4--the screen grids. The 250
volts DC B+3 is used to power the preamp and phase inverter tubes but it's stepped down even more by their load
resistors. The filter capacitors and voltage dropping resistors also decouple
the three B+ power nodes to prevent interaction, feedback and oscillations
between the preamp and power tube. You can raise or lower the B+2 and B+3 voltages by adjusting the
value of the voltage dropping resistors.
B+ current is
supplied by the power transformer's high voltage secondary. Preamp tube current
is so low it isn't necessary to actually calculate the value so we can simply
estimate it at 3ma per triode (2 triodes per preamp tube).
Power Tube B+ Current Calculations:
Transformer voltage: 355-0-355
volts AC RMS. The 0 means the transformer has a grounded 0 volt center tap and
the transformer puts out +355v on one wire while simultaneously putting out
-355v on the other for a 710v AC RMS voltage wire-to-wire.
Max_Plate_Dissipation
in watts from tube data
sheets:
KT88/6550: 42,
KT66: 25,
EL34/6CA7: 25,
6V6: 12,
EL84/6BQ5: 12,
6L6GC: 30,
6L6WGB/5881: 23,
6L6/G/GA/GB/WGA/5932: 19,
Preamp tubes using both triodes as power tubes: 12AX7: 2, 12AT7: 5, 12AU7: 5.5,
12BH7A: 7
Rectifier_Efficiency: Solid state full
wave diode: 1.37,
GZ34: 1.36,
EZ81: 1.30,
5U4B: 1.28,
5Y3: 1.25
Unloaded_B+ voltage = Transformer AC * Rectifier_Efficiency
= 355V * 1.25 = 443.8V. This would be the B+ voltage with no preamp or power
tubes installed.
B+_Voltage_Drop under load
is estimated at 16% = 443.8 * .16 = 71V
How far the B+ drops is dependant upon the
output transformer's current rating. A transformer
operating near its max current rating can't refill the filter (reservoir)
capacitors as quickly as a larger, higher rated transformer so the voltage will
drop more.
So a 5E3 power transformer must supply at least 2
amps of 5V rectifier heater current, 1.5 amps of 6.3V current for the tube
heaters and 90.8 milliamps (0.0932 amps) of B+ current. It uses 10 watts of 5V,
9.5 watts of 6.3V and 34 watts of B+ for a total of 53.6 watts, less than a 60
watt light bulb.
This is my take on the best possible layout for a
standard 5E3 chassis. This is a basic 5E3 circuit, there are no
modifications that will affect the tone. I have deleted the totally unnecessary Standby Switch and
Death Cap.
Shielded cable is used to connect the grid stoppers directly
(across the chassis) to V1. The cable shield is grounded to an input jack ground
tab. The V1 end of the cable is not grounded to prevent a ground loop. A nice,
clean option is to use shielded microphone cable which has four conductors and
run both input wires through one microphone cable. Shielded cable isn't a
necessity in the 5E3 but if you use standard wire I recommend you run it along
the chassis floor and below the circuit board to allow the chassis act as a
noise shield.
Separate eyelets are provided for the preamp tube cathode
resistors and bypass caps. The B+3 filter cap is moved to supply V1 directly.
The V2A coupling cap is reoriented to reduce cable runs. Wire routing is optimized for
shorter runs, 90 degree wire crossings and maximum separation between grid and
plate wires.
The choice of resistor is up to you but I recommend 1 watt metal
film everywhere except where noted on the layout. Metal film resistors generate
1/10th the resistor hiss compared to carbon composition resistors but I did
follow R.G. Keen's suggestion to use 1 or .5 watt carbon
comp resistors on just the phase inverter load and tail resistors for a
little carbon mojo. A 10 watt 250 ohm cement resistor is used for the power tube
cathode. The plate load resistors are bumped up to 2 watts and the voltage dropping resistors are
upgraded to 3 and 5 watts for component longevity.
I employed a unified ground bus that is only grounded at the
Normal Low input jack. The power transformer high voltage center tap is
connected directly to the B+1 filter capacitor negative terminal to minimize hum.
The typical split-bus ground sends all the preamp return current through the chassis.
This ground scheme doesn't flow any current through the chassis which any
electrical engineer will tell you is a good thing.
The 6.3v center tap is connected to the tube side of the power
tube cathode resistor to elevate the reference voltage to reduce hum. If you want to
use an artificial 6.3v center tap then I recommend putting the 100 ohm resistors
on the V3 power tube socket like
this.
I also shortened up the component span to keep from stretching
the small component leads so much.
I added optional power tube screen resistors to the circuit
board. They are shown
"ghosted" on the circuit board between the power tube cathode resistor and the
B+2 filter cap. I add them to all my 5E3 builds because they help protect the
tubes during heavy overdrive and they sweeten the power tube distortion. If you do want to use them then do not use the red wire that
runs from the B+2 cap to the power tube pins 4, use the wires from the top of
the screen resistors to pins 4 instead.
The worthless standby switch has been removed which allowed
some simplification and optimization of this point-to-point layout. I used a
simple three-point grounding scheme with the first two filter caps' ground
isolated. The "Cap Ground" and "Power Amp Ground" tag strips are grounded to the
chassis. The preamp ground at lower right is grounded through the black wire
connected to the Normal Hi input jack at upper right--the tag strip's center
ground terminal is not used.
The VHT Standard 12 is a 5E3 Deluxe with a 12AX7 in V1, added V1B Bright
Channel local negative feedback (Local NFB center left), 470 ohm power tube
screen resistors and headphone jack (upper right).
2.7M Local Negative Feedback (LNFB at center right), 470
ohm 2 watt screen resistors on the power tube sockets and added headphone jack
circuit (center low). Green wires are ground connections.
The addition of the V1B local negative feedback circuit will
slightly reduce Bright Channel gain and distortion and help tame the extra gain
from the 12AX7 in V1 (5E3 uses a 12AY7 in V1). Adding 470 ohm power tube screen resistors
would sweeten power tube distortion and help protect the tube from screen
failure during heavy overdrive. The amp uses a star grounding scheme with
isolated Cliff input jacks connected to an AC only ground through capacitor C15.
The headphone circuit's 2.2k and 100 ohm resistors form a voltage divider which
cuts the amp's output to the headphone by 96%. The headphone output suffers from
the lack of speaker tone shaping
and breakup. I recommend anyone owning a Standard 12 try a 12AY7 in V1 for a
more authentic 5E3 tone.
The 5E3P tweed Proluxe features a dual 6L6 tube push-pull output
stage and fixed bias. It uses a higher voltage output GZ34 rectifier tube to give
the 6L6 power tubes the higher voltage they like. The signal flow is identical to the 5E3 and is shown using
orange arrows. Red arrows show the power flow. My first amp build was a
BootHillAmps.com 5E3P.
By Rob Robinette
References
RCA Corporation,
RCA Receiving Tube Manual,
RC30.
Merlin Blencowe,
Designing Tube Preamps for Guitar and Bass, 2nd Edition. This is my personal
favorite tube amp book.
Richard Kuehnel,
Vacuum Tube Circuit Design: Guitar Amplifier Power Amps
Robert C. Megantz,
Design and Construction of Tube Guitar Amplifiers
Neumann &
Irving,
Guitar Amplifier Overdrive, A Visual Tour It's
fairly technical but it's the only book written specifically about guitar
amplifier overdrive. It includes many graphs to help make the material
easier to understand.