A supercapacitor (SC)
(also electric double-layer capacitor (EDLC), also called supercap, ultracapacitor
or Goldcap) is a high-capacity capacitor with capacitance values much
higher than other capacitors (but lower voltage limits) that bridge the gap
between electrolytic capacitors and rechargeable batteries. They typically
store 10 to 100 times more energy per unit volume or mass than electrolytic
capacitors, can accept and deliver charge much faster than batteries, and
tolerate many more charge and discharge cycles than rechargeable batteries.
Supercapacitors are used in
applications requiring many rapid charge/discharge cycles rather than long term
compact energy storage: within cars, buses, trains, cranes and elevators, where
they are used for regenerative braking, short-term energy storage or burst-mode
power delivery. Smaller units are used as memory backup for static
random-access memory (SRAM).
Supercapacitors do not use the
conventional solid dielectric of ordinary capacitors. They use electrostatic double-layer
capacitance and electrochemical pseudocapacitance, both of which contribute to
the total capacitance of the capacitor, however, with different amounts:
- Electrostatic double-layer capacitors use carbon
electrodes or derivatives with much higher electrostatic double-layer
capacitance than electrochemical pseudocapacitance, achieving separation
of charge in a Helmholtz double layer at the interface between the surface
of a conductive electrode and an electrolyte. The separation of charge is
of the order of a few ångströms (0.3–0.8 nm), much smaller than in a
conventional capacitor.
- Electrochemical pseudocapacitors use metal
oxide or conducting polymer electrodes with a high amount of
electrochemical pseudocapacitance additional to the double-layer capacitance.
Pseudocapacitance is achieved by Faradaic electron charge-transfer with redox
reactions, intercalation or electrosorption.
- Hybrid capacitors, such as the lithium-ion
capacitor, use electrodes with differing characteristics: one exhibiting
mostly electrostatic capacitance and the other mostly electrochemical
capacitance.
The electrolyte forms an ionic
conductive connection between the two electrodes which distinguishes them from
conventional electrolytic capacitors where a dielectric layer always exists,
and the so-called electrolyte (e.g. MnO2 or conducting polymer) is in fact part of the
second electrode (the cathode, or more correctly the positive electrode).
Supercapacitors are polarized by design with asymmetric electrodes, or, for
symmetric electrodes, by a potential applied during manufacture.
Lifetime of Supercapacitors
Since supercapacitors do not rely
on chemical changes in the electrodes (except for those with polymer
electrodes) lifetimes depend mostly on the rate of evaporation of the liquid
electrolyte. This evaporation in general is a function of temperature, of
current load, current cycle frequency and voltage. Current load and cycle
frequency generate internal heat, so that the evaporation-determining
temperature is the sum of ambient and internal heat. This temperature is
measurable as core temperature in the center of a capacitor body. The higher
the core temperature the faster the evaporation and the shorter the lifetime.
Evaporation generally results in
decreasing capacitance and increasing internal resistance. According to IEC/EN
62391-2 capacitance reductions of over 30% or internal resistance exceeding
four times its data sheet specifications are considered "wear-out
failures", implying that the component has reached end-of-life. The
capacitors are operable, but with reduced capabilities. Whether the aberration
of the parameters have any influence on the proper functionality or not depends
on the application of the capacitors.
Such large changes of electrical
parameters specified in IEC/EN 62391-2 are usually unacceptable for high
current load applications. Components that support high current loads use much
smaller limits, e.g., 20% loss of capacitance or double the internal
resistance.[83] The narrower definition is important for
such applications, since heat increases linearly with increasing internal
resistance and the maximum temperature should not be exceeded. Temperatures
higher than specified can destroy the capacitor.
The real application lifetime of
supercapacitors, also called "service life", "life
expectancy" or "load life", can reach 10 to 15 years or more at
room temperature. Such long periods cannot be tested by manufacturers. Hence,
they specify the expected capacitor lifetime at the maximum temperature and
voltage conditions. The results are specified in datasheets using the notation
"tested time (hours)/max. temperature (°C)", such as
"5000 h/65 °C". With this value and expressions derived
from historical data, lifetimes can be estimated for lower temperature
conditions.
Datasheet lifetime specification
is tested by the manufactures using an accelerated aging test called
"endurance test" with maximum temperature and voltage over a
specified time. For a "zero defect" product policy during this test
no wear out or total failure may occur.
The lifetime specification from
datasheets can be used to estimate the expected lifetime for a given design.
The "10-degrees-rule" used for electrolytic capacitors with non-solid
electrolyte is used in those estimations and can be used for supercapacitors.
This rule employs the Arrhenius equation, a simple formula for the temperature
dependence of reaction rates. For every 10 °C reduction in operating
temperature, the estimated life doubles.
Market for Supercapacitors
As of 2016 worldwide sales of
supercapacitors is about US$400 million.
The market for batteries
(estimated by Frost & Sullivan) grew from US$47.5 billion, (76.4% or
US$36.3 billion of which was rechargeable batteries) to US$95 billion. The market for
supercapacitors is still a small niche market that is not keeping pace with its
larger rival.
In 2016, IDTechEx forecast sales
to grow from $240 million to $2 billion by 2026, an annual increase of about
24%.
Supercapacitor costs in 2006 were
US$0.01 per farad or US$2.85 per kilojoule, moving in 2008 below US$0.01 per
farad, and were expected to drop further in the medium term.
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