Capacitors
There seems to be a lot of hype and mystery
concerning the sound of capacitors, the quality of capacitors and what
capacitors actually do in a circuit. There are many types of capacitors
including ceramic, polyester, polypropylene, polycarbonate silver mica,
tantalum and electrolytic. Each has its own area of “expertise”. One type of
capacitor will perform well in a particular application and perform poorly in
another. A capacitor is simply two metal plates separated by a dielectric. An
electrical charge is stored between these two plates. The plates and dielectric
can be made form several different types of material. The closer the plates are,
the higher the capacitance and the larger the area of the plates, the larger
the capacitance. The dielectric material affects the capacitance as well. Here
is some brief information about the particular types.
Note: The unit of capacitance is the
Farad. It is a very large unit and so we use the following to express
capacitance
Microfarad is one millionth of a farad.
Picofarad
is one millionth of a microfarad
So 0.001mfd is equal to 1000 picofarad (pF)

The above diagram shows a simple
representation of a capacitor.
The capacitor is shown in RED.
In parallel with the plates of the
capacitor is a resistance, Ins-Res of the
insulation. Teflon has the highest resistance with polystyrene, polypropylene
and polycarbonate coming in second. Third is polyester
and then the ceramics COG, Z5U and XR7 with tantalum and aluminium
last.
Dap is the Dielectric Absorption. All
capacitors when charged to a particular voltage and then the leads are shorted,
will recover some of their charge after the short is removed. The ratio of the
initial voltage to the recovered voltage is expressed as a percentage. In
general, electrolytics are the worst and film types
are the best.
The series inductance is shown simply in series
with the capacitor itself. Electrolytics have the
highest inductance mainly due to how the capacitor is made. The higher the
frequency the higher this inductance becomes.
The ESR of the
capacitor is the resistance that appears in series with the actual capacitor.
The higher the voltage and value the lower the ESR. This resistance is made up of dielectric
loss, lead termination resistance and the electrode resistance. This is nearly
constant with frequency.
The dissipation factor or DF is the ratio of ESR divided by the capacitive reactance(Xc) which is given by this formula (Xc = 1/6.28 x F x C) where F is frequency and C is the value in Farads. Normally of course we have values in “Mfd” and so the the value of C can be in Mfd and then the numerator becomes 1,000,000 instead of just 1.
Ceramic capacitors
are used in high frequency circuits such as RF. They are also the best choice for high
frequency compensation in audio circuits. Now some may snub their noses when
hearing this. We used to manufacture some high end amps for a Japanese company
and they demanded that NO ceramics be used in the amplifiers. Pretty much all
amplifiers have some sort of high frequency compensation to prevent them from
oscillating and instability. The frequency at which these ceramics were doing
their work was at 240KHz. Now I do not know about all of you out there but my
hearing does not go out THAT high. Maybe these guys were distant relatives of
the bat!
They come in values from a few picofarads to 1 microfarad. The voltage range is from a few
volts up to many thousands of volts. Ceramics are inexpensive to manufacture
and they come with several dielectric types. Types XR7 and Z5U are the least
stable as far as temperature is concerned. They have a higher dielectric
constant than the higher stability types like COG. The tolerance of ceramics is
not great but for their intended role in life they work just fine.
Tantalum capacitors
are made by depositing a film of oxide on tantalum. These are polarized types
and are smaller than their aluminium counterparts.
They are low voltage types only with a maximum rating of about 40 volts. We at
zed do NOT use these as they are notoriously unreliable. They have a bad
tendency to go leaky. I will NEVER EVER use a tantalum capacitor as they are so
unreliable and my experience many years ago bears that out.
Aluminium Electrolytic capacitors
are made by depositing a film of oxide on aluminium
foil. The foil is formed for a specific voltage rating. These are polarized and
of courser do not tolerate having reverse voltage applied to them. (Anyone been
around when one of these larger value babies explodes – it is not a pretty
sight?) They are also not happy campers if the rated voltage is exceeded (same
thing, they will make a mess of the equipment and your face if you are too
close) BUT higher quality types will tolerate about 5% over voltage. What
happens in these capacitors that if one applies say 37 volts to a 35 volt
capacitor it will actually reform its foil over time to the new applied voltage
but its value will drop to keep CV a constant. Conversely if a lower voltage is
applied it will reform to this new voltage and the capacitance will increase.
Now do not get all excited and take your 10,000mfd 50v capacitor and use it at
25 volts and expect to get 20,000mfd out of it. There are limits to what these
guys will do. It is also not a great idea to run electrolytics
at voltages well below their rated voltage. A rule of thumb is about 25% lower
voltage than rated is OK. They are normally made by winding the foils around in
each other in a cylindrical way. High capacitance is easily obtained.
The ESR is the Equivalent Series Resistance
and the higher the value and voltage the lower the ESR. The lower the ESR the
less heat the capacitor will generate when current is drawn from it. Also
closely related to the ESR is the available ripple current that a capacitor can
tolerate. This is mainly of concern in power supplies. Most manufacturers offer
many grades and sizes of electrolytic capacitors. There are of course both through
hole and surface mount types. Within each category there are sub categories.
Through hole types offer many more variations than surface mount. There are 85
deg C and 105 deg C versions leaded, snap in and screw type terminations. Electrolytics, especially those used in high current power
supplies have a fixed lifespan and once a electrolytic
decides it is tired of living, then it is off to “the pie in the sky”.
Typically their life span is from 1,000 to 3,000 hours depending on the
quality.
Their tolerance is not good but then again
a low tolerance component is not essential. Typically the value can vary from
-50% to +100% of the nominal value.
There are non-polar electrolytics
and these are mainly used in passive speaker crossovers.
Silver Mica
Capacitors are one of the best types of capacitors.
They have excellent stability and are available in low tolerance values down to
less than 0.1%. They ARE sensitive to heat and are now used mainly in RF and
tuned circuits. I like them in RIAA preamplifiers as I think they do sound
better in that application.
Film capacitors
encompass polyester, polypropylene, polycarbonate and others. Each has its own
strengths and weakness. These are normally used in audio for filters,
equalizers and power supply bypass duty. They are available in almost any value
and voltages as high as 1,500 volts. They come in any tolerance from 10% to
0.01%.
Well now that you almost know all there is
to know about capacitors (Only kidding) it is time to discuss how they sound
and why we use certain types in particular applications.
Power supplies
generally demand the use of electrolytic capacitors because they have high
values in small packages. The value is determined by how much ripple can be
tolerated and the voltage is determined by the voltage of the power supply
(Duh!). Because this type of capacitor has inductance, it is normal practice to
bypass them with film type capacitors in order to improve the high frequency
characteristics. In 50/60Hz supplies I have never found these bypass film
capacitors do anything to improve the sound.
Coupling capacitors
are usually electrolytic (Yes this is not a typo error) and film types. The
value of the coupling capacitor is usually determined by the load impedance
which the capacitor “sees”. If the value is too small for a given load
impedance then the low frequencies will be attenuated at a rate of 6dB/octave.

Let us examine the circuit above. The
capacitor has a reactance which forms a potential divided with the 10K ohm
resistor. This circuit may represent the coupling of one circuit block
delivering “Vin” at 1 volt to another circuit block
shown as “Vout”. We can consider the capacitor as a
resistor whose value changes with frequency which is really its reactance (Xc).
So the formula for Vout
is [Vout/Vin = 10,000/10,000+Xc]
and [Xc = 1/6.28xFxC]
We can now throw some numbers into our
formulas and see what comes out. Let us pick a frequency of say 1KHz and a capacitor value of 0.22mfd as a first example.
Solving for Xc we get Xc = 723 ohms. Solving for Vout we get 0.932 volt. This means that at a
frequency of 1KHz a 0.22mfd capacitor will cause the
output voltage to drop to 0.932 (a 0.61dB drop). The frequency at which Xc = 10K ohm is 72.37Hz (I simply
solved for F in the formula above)
As a coupling capacitor in a full range
circuit the 0.22mfd is clearly inadequate since it rolls off the response from
over 1KHz and is 3dB down at 72.37Hz. What do we do to
calculate the value of C which will allow decent low end response? We shall
pick a frequency at which we want the signal level at Vout
to drop to -3dB as low as we desire. We shall choose 2Hz. Solving again for C
in the Xc formula above we get 7.96mfd. We would
then use a 10mfd. This 10mfd can be a regular polarized electrolytic, two
electrolytic capacitors wired back to back with common polarity terminals
joined, a non-polar version or a film type. The film type will be large and
expensive. In op-amp circuits where the DC supplies are less than 20 volts, a
film type rated at 25 or 63v is not that large. In tube circuits however where
there are hundreds of volts, a 10mfd 450v capacitor is a large specimen. At Zed
we go one step further and increase the value fivefold so the -3dB break
frequency goes down well below 1Hz. My opinion is that if the value of the
capacitor is so large so as to make a break point well below 1Hz the
electrolytic capacitor does not degrade the sound.
An amusing story: About 14 years ago Zed Audio
was building subwoofer amplifiers for a large well known speaker company in
Chatsworth
The gurus put their favourite
album on the turntable and away we went. One of their technicians was flipping
the switch at the listeners’ command. Back and forth we went for over ten
minutes with all saying “Yes that’s the capacitor, no that’s the wire”. So we
stopped and I called all these gurus over to the switch and showed them the
dead short across the capacitor. Red faces, curses etc and I was a bad boy and
they were fools. Most of this “component” sound is in one’s head. You have to hear the difference
after you have spent $55.00 on your new coupling capacitors!
Power supply bypass
capacitors are sometimes required in low level circuits.
These should be a pair of ceramic capacitors (Yes ceramic as they perform best
at high frequencies) placed as close to the power supply pins of the integrated
circuit or discrete circuit block and some electrolytic capacitors placed
reasonably close. Film capacitors will work fine but as they are more expensive
than their ceramic counterparts I see no reason to use them.
Switching power
supplies require the use of either low ESR
capacitors or a larger quantity of “regular” ESR capacitors. It makes absolutely
no difference which method is employed as long as the final ESR and ripple
values are arrived at.
High frequency
compensation capacitors in audio circuits always operate at
very high frequencies. In our opinion the best type to use are ceramic capacitors.
Some disagree and claim that film types are better. Since these compensation
capacitors are used to roll off extremely high frequencies I seriously doubt
that one could hear the difference. Unless you are of course a relative of our
beloved little bats.
Listening to
different capacitors is a time consuming. In order to
compare two different types of say coupling capacitors in an audio circuit
requires that you install the two types and a double pole double throw switch
(DPDT) so that a direct A-B comparison may be done. The switch should be a gold
plated low contact resistance type.
Ideally you must install the switch at the point in the circuit where
the capacitors live. This may sometimes be difficult to do because it may not
always be simple to solder in the parts. The “crook” method is to do the
switching between two pieces of equipment like a head unit or preamplifier and
the power amplifier. The simple circuit is shown below with only one channel
shown for clarity.

The two capacitors marked C1 and C2 are to
be compared. The double pole double throw switch (DPDT) is toggled between the
two capacitors. The Resistor shown as “x” ohm is what the capacitors “see” as
their load impedance and this resistor is normally the input resistor of the
next circuit block or equipment.
Copyright Information – This document including all text, diagrams and pictures, is the property of Zed Audio Corporation and is Copyright © 2005.