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Aluminum Electrolytic Capacitor Application Guide
This guide is a full handbook on aluminum electrolytic capacitors, of course with emphasis on Cornell Dubilier’s types. It covers
construction in depth and discloses the latest information on performance and application for the major aluminum electrolytic
types made worldwide. We encourage you to tell us what more you’d like to know, so we can improve this guide.
CONTENTS PAGE
Capacitor Construction 2
Other Types of Capacitors Comparison 4
Characterization and Circuit Model 5 TABLES PAGE
Temperature Range 6 Capacitor Parameter Formulas 6
Capacitance 7 Base Lives and Max Core Temperatures 14
Dissipation Factor (DF) 7 Thermal Resistance Screw Terminal Capacitors 17
Equivalent Series Resistance (ESR) 8 Thermal Resistance for Snap-in Capacitors 19
Impedance (Z) 8 Pressure Relief Devise Clearance 21
Low-Temperature Impedance 8 Screw Tightening Torque for Screw Terminals 21
DC Leakage Current (DCL) 8 Maximum Currents for Screw Terminals 21
Voltage Withstanding 9 Tightening Torque for Nylon Mounting Nuts 22
Ripple Current 10
Inductance 10
Self-Resonant Frequency 10
Dielectric Absorption 11
Insulation and Grounding 11
Elevation & External Pressure 11
Vibration Withstanding Capability 11
Safety Considerations 11
Capacitor Bank Configurations 12
Non-Polar and Motor Start Capacitors 13
Reliability and Lifetime 13
Cooling and Thermal Resistance 16
Process Considerations 19
Mounting 20
Disposal of Capacitors 22
ALUMINUM ELECTROLYTIC CAPACITOR OVERVIEW
Except for a few surface-mount technology (SMT) aluminum
electrolytic capacitor types with solid electrolyte systems an
aluminum electrolytic capacitor consists of a wound capacitor
element, impregnated with liquid electrolyte, connected to
terminals and sealed in a can. The element is comprised of an
anode foil, paper separators saturated with electrolyte and a
cathode foil. The foils are high-purity aluminum and are etched
with billions of microscopic tunnels to increase the surface area
in contact with the electrolyte.
While it may appear that the capacitance is between the two
foils, actually the capacitance is between the anode foil and the
electrolyte. The positive plate is the anode foil; the dielectric is the
insulating aluminum oxide on the anode foil; the true negative
plate is the conductive, liquid electrolyte, and the cathode foil
connects to the electrolyte. However, just as the anodic-oxide
dielectric insulates the anode foil from the electrolyte, so too the
cathode is insulated from the electrolyte by the low voltage air
oxide on the cathode foil and the double-layer ionic barrier. This
makes the cathode a capacitor in series with the anode. In high
voltage capacitors the cathode capacitance is hundreds of times
the anode capacitance and does not measurably affect the
overall capacitance, but in capacitors of less than about 50 V the
anode capacitance begins to approach the value of the cathode
capacitance and requires use of higher capacitance cathode to
avoid needing to increase the anode length to achieve the rated
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Miniature, Radial-Leaded Type
Lead Wire
Aluminum
Tabs
Rubber
Sleeve over
Aluminum Can
Capacitor
Element
Snap-in Type
Sleeve over
Aluminum Can
Terminal
Aluminum
Tabs
Phenolic/
Rubber Disc
Capacitor
Element
Rivet
Tape
capacitance. Aluminum electrolytic capacitor construction
delivers colossal capacitance because etching the foils can
increase surface area more than 100 times and the aluminum-
oxide dielectric is less than a micrometer thick. Thus the
resulting capacitor has very large plate area and the plates are
intensely close together.
These capacitors routinely off er capacitance values from 0.1 µF
to 3 F and voltage ratings from 5 V to 550 V. Up to 700 V are
commercially available. They are polar devices, having distinct
positive and negative terminals, and are off ered in an enormous
variety of styles which include molded and can-style SMT
devices, axial- and radial-leaded can styles, snap-in terminals
styles and large-can, screw-terminal styles. Representative
capacitance-voltage combinations include:
330 µF at 100 V and 6,800 µF at 10 V for SMT devices,
100 µF at 450 V, 6,800 µF at 50 V and 10,000 µF at 10 V
for miniature-can styles,
1200 µF at 450 V and 39,000 µF at 50 V for snap-in can
styles and
9000 µF at 450 V and 390,000 µF at 50 V for large-can,
screw-terminal styles.
If two, same-value, aluminum electrolytic capacitors are
connected in series with the positive terminals or the negative
terminals connected together, the resulting single capacitor
is a non-polar capacitor with half the capacitance. The two
capacitors rectify the applied voltage and act as if they had
been bypassed by diodes. When voltage is applied, the correct-
polarity capacitor gets the full voltage. In non-polar aluminum
electrolytic capacitors and motor-start aluminum electrolyte
capacitors a second anode foil substitutes for the cathode foil to
achieve a non-polar capacitor in a single case.
Snap-in Type
CAPACITOR CONSTRUCTION
Tabs
Phenolic / Nylon
Cover w/
Centering Peg
Aluminum
Centering Peg
Sleeve
Over
Aluminum
Can
Extended
Cathode
Terminals
Centering Peg
Aluminum
Centering Peg
Rills
Rubber Gasket
Tape
Aluminum
Stiffening
Ribs
Tabs
Phenolic / Nylon
Cover w/
Centering Peg
Aluminum
Centering Peg
Sleeve
Over
Aluminum
Can
Extended
Cathode
Terminals
Rubber Gasket
Tape
Aluminum
Stiffening
Ribs
Thermal Pak Construction Rilled Construction
Thermal Pak Construction Rilled Construction
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These fi gures show typical constructions of the non-surface-
mount aluminum electrolytic capacitors. All Cornell Dubilier
capacitors use compression-fi t construction so there is no
thermoplastic potting compound to interfere with safety-
vent operation. Thermal Pak™ and Rilled are Cornell Dubilier’s
exceptional constructions for screw terminal capacitors.
Compared to conventional, potted construction, Thermal Pak
operates cooler, provides longer life, withstands higher shock
and vibration, delivers more reliable safety vent operation and
is lighter weight. Rilled off ers superior shock and vibration
withstanding, typically withstanding more than 15 g acceleration
forces.
ETCHING
The anode and cathode foils are made of high purity, thin
aluminum foil, 0.02 to 0.1 mm thick. To increase the plate area and
the capacitance, the surface area in contact with the electrolyte
is increased by etching the foils to dissolve aluminum and create
a dense network of billions of microscopic tunnels penetrating
through the foil. For maximum increase in surface area in
higher voltage capacitors the anode foil is 99.99% high purity,
high cubicity aluminum that allows the billions of microscopic
etch tunnels to be parallel and mostly perpendicular to the foil
surface.
Etching involves pulling the aluminum foil on rollers through a
chloride solution while applying an AC, DC or AC-and-DC voltage
between the etch solution and the aluminum foil. Surface
area can increase as much as 200 times for foil in low-voltage
capacitors and up to 60 times for high-voltage capacitors.
FORMING
The anode foil carries the capacitor’s dielectric. The dielectric
is a thin layer of aluminum oxide, Al2O3, which is chemically
grown on the anode foil during a process called “formation.”
Formation is accomplished by pulling the anode foil on rollers
through an electrolyte bath and continuously applying a DC
voltage between the bath and the foil. The voltage is 135% to
200% of the fi nal capacitor’s rated voltage. The thickness of
the aluminum oxide is about 1.4 to 1.5 nm for each volt of the
formation voltage, e.g., the anode foil in a 450 V capacitor may
get a formation voltage in excess of 600 V and have an oxide
thickness of about 900 nm. That’s about a hundredth of the
thickness of a human hair.
Formation reduces the eff ective foil surface area because the
microscopic tunnels are partially occluded by the oxide. The
tunnel etch pattern is adjusted by choice of foil and etching
process so that low-voltage anodes have dense tunnel patterns
compatible with thin oxide and high-voltage anodes have coarse
tunnel patterns compatible with thick oxide. The cathode foil is
not formed and it retains its high surface area and dense etch
pattern.
SLITTING
Foil is etched and formed in jumbo rolls of 40 to 50 cm wide and
then slit into various widths according to the lengths of the fi nal
capacitors.
WINDING
The capacitor element is wound on a winding machine with
spindles for one-to-four separator papers, the anode foil,
another set of one-to-four separator papers and the cathode
foil. These are wound into a cylinder and wrapped with a strip
of pressure-sensitive tape to prevent unwinding. The separators
prevent the foils from touching and shorting, and the separators
later hold the reservoir of electrolyte.
Before or during winding aluminum tabs are attached to the
foils for later connection to the capacitor terminals. The best
method is by cold-welding of the tabs to the foils with tab
locations microprocessor controlled during winding so that
the capacitor element’s inductance can be less than 2 nH. The
older method of attachment is by staking, a process of punching
the tab through the foil and folding down the punched metal.
Cold welding reduces short-circuit failures and performs better
in high-ripple current and discharge applications in which the
individual stakes may fail from high current like buttons popping
off one at a time from a fat-man’s vest.
CONNECTING TERMINALS
In SMT capacitors and miniature capacitors with rubber-bungs,
extensions of the tabs are the capacitor terminals. But in large-
can capacitors like snap-ins and screw-terminal styles, the
tabs are riveted or welded on the underside of the capacitor
tops to terminal inserts. Welding produces the lowest contact
resistance and highest current handling. Both resistive welding
and ultrasonic welding are used. The up to 12 tab pairs that
may be used in large screw-terminal capacitors often require
more mechanical support during assembly so the tabs in such
capacitors may be both riveted to post extensions on the
terminals and then welded. In an axial-leaded capacitor the
cathode tab is welded to the can before sealing.
IMPREGNATION
The capacitor element is impregnated with electrolyte to
saturate the paper separators and penetrate the etch tunnels.
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The method of impregnation may involve immersion of the
elements and application of vacuum-pressure cycles with
or without heat or, in the case of small units, just simple
absorption. The electrolyte is a complex blend of ingredients
with different formulations according to voltage and operating
temperature range. The principal ingredients are a solvent and
a conductive salt – a solute – to produce electrical conduction.
The common solvent is ethylene glycol (EG) and is typically used
for capacitors rated –20 ºC or –40 ºC. Dimethylformamide (DMF)
and gammabutyrolactone (GBL) are often used for capacitors
rated –55 ºC. Common solutes are ammonium borate and other
ammonium salts.
Water in the electrolyte plays a big role. It increases conductivity
thereby reducing the capacitor’s resistance, but it reduces the
boiling point so it interferes with high temperature performance,
and it reduces shelf life. A few percent of water is necessary
because the electrolyte maintains the integrity of the aluminum
oxide dielectric. When leakage current flows, water is broken
into hydrogen and oxygen by hydrolysis, and the oxygen is
bonded to the anode foil to heal leakage sites by growing more
oxide. The hydrogen escapes by passing through the capacitor’s
rubber seal.
SEALING
The capacitor element is sealed into a can. While most cans
are aluminum, phenolic cans are often used for motor-start
capacitors. In order to release the hydrogen the seal is not
hermetic and it is usually a pressure closure made by rolling the
can edge into a rubber gasket, a rubber end-plug or into rubber
laminated to a phenolic board. In small capacitors molded
phenolic resin or polyphenylene sulfide may replace the rubber.
Too tight a seal causes pressure build up, and too loose a seal
shortens the life by permitting drying out, loss of electrolyte.
AGING
Here the capacitor assembly comes full circle. The last
manufacturing step is “aging” during which a DC voltage greater
than the rated voltage but less than the formation voltage is
applied to the capacitor. Usually the voltage is applied at the
capacitor’s rated temperature, but other temperatures and even
room temperature may be used. This step reforms the cut edges
and any damaged spots on the anode foil and covers any bare
aluminum with aluminum oxide dielectric. Aging acts as burn-
in and reduces or eliminates early life failures (infant mortals).
Low, initial DC leakage current is a sign of effective aging.
COMPARISON TO OTHER TYPES OF
CAPACITORS
CERAMIC CAPACITORS
Ceramic capacitors have become the preeminent, general-
purpose capacitor, especially in SMT chip devices where their
low cost makes them especially attractive. With the emergence
of thinner-dielectric, multilayer units with rated voltages of less
than 10 V capacitance values in the hundreds of microfarads
have become available. This intrudes on the traditional, high-
capacitance province of aluminum electrolytic capacitors.
Ceramic capacitors are available in three classes according to
dielectric constant and temperature performance. Class 1 (NPO,
COG) is suitable for low capacitance, tight tolerance applications
in the range of 1 pF to a few mF. Class 2 (X7R, X5R, Y5V) has 20
to 70 times as much capacitance per case size, but capacitance
typically varies about ± 10% over its –55 to 125 ºC temperature
range. The maximum change is +15 % to –25%. Class 3 (Z5U)
with about 5 times the capacitance of Class 3 has wild swings
of capacitance with voltage and temperature. The temperature
range is –25 ºC to 85 ºC, and capacitance varies about +20%
–65% over the range. All classes of ceramic capacitors are
available in a variety of physical forms, ranging from round disc
or rectangular single layer to multilayer types as well as tubular
and feed-through types. Ceramic chip capacitors are brittle and
sensitive to thermal shock, so precautions need to be taken to
avoid cracking during mounting, especially for high-capacitance
large sizes.
The typical temperature range for aluminum electrolytic
capacitors is –40 ºC to 85 ºC or 105 ºC. Capacitance varies about
+5% –40% over the range with the capacitance loss all at cold
temperatures. Capacitors rated –55 ºC generally only have
–10 % to –20 % capacitance loss at –40 ºC. Cold temperature
performance for rated voltages of 300 V and higher is often
worse, and temperature performance varies by manufacturer.
Thus Class 1 and 2 ceramic capacitors perform better than
aluminum electrolytic capacitors at cold temperatures, and
Class 3 ceramic capacitors perform worse at all temperatures.
Aluminum electrolytic capacitors readily deliver much more
capacitance. Aluminum electrolytic capacitors give more
capacitance and energy storage per unit volume than ceramic
capacitors for all types except for low-voltage, Class 3 ceramic
SMT chip capacitors. While tolerances of ±5% and ±10% are
routine for ceramic capacitors, ± 20% and –10% +50% are
the norms for aluminum electrolytic. This makes aluminum
electrolytics the choice for high-capacitance applications like
rectification filters and power hold up where more capacitance
is a bonus.
Ceramic capacitors are not polarized and therefore can be used
in AC applications. The low DF and high capacitance stability of
Class 1 and 2 are especially suited to AC and RF applications. By
comparison, aluminum electrolytic capacitors are polarized and
cannot withstand voltage reversal in excess of 1.5 V. While non-
polar aluminum electrolytics are available for momentary-duty
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AC applications like motor starting and voltage-reversing
applications, the high DF of aluminum electrolytic capacitors –
from 2% to 150% – causes excess heating and short life in most
AC applications.
Ceramic capacitors are generally no more reliable than aluminum
electrolytic capacitors because aluminum electrolytics self
heal. Since high-capacitance ceramic capacitors may develop
micro-cracks, aluminum electrolytic capacitors are preferred
for high capacitance values. However, small sizes of aluminum
electrolytic capacitors may have limited life due to dry out, and
so consider reliability in your choice for applications operating
at high temperatures, over 65 ºC.
FILM CAPACITORS
Film capacitors offer tight capacitance tolerances, very
low leakage currents and small capacitance change with
temperature. They are especially suited to AC applications
through their combination of high capacitance and low DF that
permits high AC currents. However, they have relatively large
sizes and weights.
The popular polymers used for plastic-film dielectric capacitors
are polyester and polypropylene. The popular polymer for
SMT devices is polyphenylene sulfide (PPS). While film/foil
construction is often used for small capacitance values – less
than 0.01 µF – and for high-current applications, metallized-film
is usually preferred because it gives smaller size, lower cost and
is self healing. Film capacitors are general-purpose capacitors
for through-hole applications and have special uses for tight-
tolerance, AC voltage, high voltage and snubbing.
Polyester film capacitors operate from –55 ºC to 85 ºC at rated
voltage; 85 ºC to 125 ºC with linear voltage derating to 50%
rated voltage. The typical capacitance change over the entire
range is less than –5% +15% with ±1% from 0 ºC to 50 ºC.
Capacitance values are readily available up to 10 µF with special
large sections to 100 µF. Generally available voltages are 50 to
1000 Vdc and 35 to 600 Vac. AC current handling is limited by
polyester’s high-temperature DF of about 1%.
Polypropylene film capacitors operate from is –55 ºC to 85 ºC
at rated voltage; 85 ºC to 105 ºC with linear voltage derating
to 50% rated voltage. The typical capacitance change over the
entire range is less than +2% –4% with ±1% from –20 ºC to 60 ºC.
Capacitance values are readily available up to 65 µF with special
large sections to 1000 µF. Generally available voltages are 100 to
3000 Vdc and 70 to 500 Vac. AC current handling permits use in
motor-run and other continuous duty AC applications.
Compared to aluminum electrolytic capacitors, film capacitors
take the lead in high voltage, AC voltage and tight tolerance
applications. Aluminum electrolytics excel in capacitance and
energy storage. However, there is growing use of power film
capacitors as replacements for aluminum electrolytic capacitors
as dc-link, bus capacitors in high-voltage inverter power systems.
While generally power film capacitors are more than four times
the price for capacitance as aluminum electrolytic capacitors,
film capacitors are perceived as more reliable because failures
are relatively benign and without the incidence of explosion and
ignition that can accompany aluminum electrolytic capacitor
failures in large high-voltage banks of 10 or more capacitors.
Cornell Dubilier now provides special aluminum electrolytic
capacitors with improved self-healing to deliver the needed
reliability for these applications.
SOLID TANTALUM CAPACITORS
Like aluminum electrolytic capacitors solid tantalum capacitors
are polar devices (1 V maximum reverse vo
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