using a supercapacitor to manage your power
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14 Dec 2009 | WorldWide
Using a supercapacitor to manage your power
Guest article by Pierre Mars, VP Applications Engineering,
CAP-XX (Australia) Pty Ltd.
This article will explain some of the key properties of
supercapacitors that design engineers creating energy
harvesting circuits need to be aware of, and explore how to
use supercapacitors in these circuits.
Why Super?
Why do supercapacitors have such high capacitance with such small volumes? Supercapacitor
electrodes are nano porous carbon coated on a current collector substrate such as aluminium. The
porous carbon has a surface area in the order of 2,500m2/gm. This gives a massive charge
storage area. Supercapacitors do not have a dielectric - they are electrical double layer capacitors.
Ions dissolved in an electrolyte provide charge transport. These ions nestle against the surface of
the porous carbon, so the charge separation distance is effectively the molecular width of the ions.
Since capacitance is proportional to charge storage area/charge separation distance, and thestorage area is 1000s of square meters, and separation distance is in nanometers supercapacitors
have enormous energy density. As an example, the CAP-XX HS230, which is 39mm x 17mm x
3.8mm, is 1.2F and has very low ESR, or Equivalent Series Resistance of 50mOhms, and is rated
to 5.5V. This results in an energy density of x 1.2F x 5.5V2/(39x17x3.8x10-6L) = 7.2KJ/L or
2Wh/L.
Since supercapacitors do not have a dielectric, their maximum operating voltage is limited by the
voltage at which the electrolyte starts undergoing electrochemical reactions. There are two types
of supercapacitor chemistries: those with organic electrolytes and those with aqueous electrolytes.
The maximum voltage for supercapacitor cells with aqueous electrolytes is the breakdown voltage
of water, ~1.1V, so these supercapacitors typically have a maximum of 0.9V/cell. Organic
electrolyte supercapacitors are rated in the range 2.3V - 2.7V cell, depending on the electrolyteused and the maximum rated operating temperature. Several supercapacitor cells are connected
in series to attain the working voltage needed. Although organic electrolyte supercapacitors have
superior energy density because they have a higher rated voltage, they are more difficult to
produce since they must be filled in a completely dry environment and hermetically sealed against
moisture. Aqueous electrolyte supercapacitors, having a water based electrolyte, have no such
problems. Supercapacitors have a porous separator to prevent the positive and negative
electrodes from shorting against each other, but allowing ions to pass through it for charge
transport.
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Supercapacitors have been around for years, but were initially very low current devices such as
the Panasonic gold cap, with high ESR, suitable for RTC and memory backup. The breakthrough in
the last 10 years or so has to be reduce the ESR so supercapacitors can deliver high power.
When current is drawn from a supercapacitor, there is an instantaneous voltage drop = ILOAD
x
ESR. Hence ESR limits the amount of current that can be usefully drawn from the supercapacitor.
Again, consider the CAP- XX HS230 as an example: if a 2A load is drawn from this supercapacitor,
the instantaneous voltage drop will only be 2A x 50m = 100mV. The maximum power transfer
occurs when the load resistance = source resistance = ESR, so for an HS203 this = V2/(4 x ESR)
= 5.52/200m = 151.25W, so power density = 151.25W/0.0025L = 60KW/L.
An Ideal Power Buffer
The supercapacitor's high energy storage and high power delivery make it ideal to buffer a high
power load from a low power energy harvesting source, as shown in Fig 1.
Fig 1: Block diagram of energy harvesting power architecture with a supercapacitor
The source sees the average load, which with appropriate interface electronics, will be a low power
constant load set at the maximum power point. The load sees a low impedance source that can
deliver the power needed for the duration of the high power event. Consider a sensor thattransmits data at 100mW for 1 second once an hour. If an HS230 is charged to 3.3V just prior to
the transmission, then during the transmission it will only discharge to 3.27V. The average power
is 0.1W/3600 = 28W. If the circuit is 60% efficient, then the source only needs to deliver - 1.8V in order for U1, Q1 to operate and charge the
supercapacitor, otherwise a boost converter is needed.
Conclusions
Supercapacitors offer an important benefit for energy harvesting applications - the ability to buffer
a high power load from a low power source in a small form factor, but they do not behave like
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example circuit that can be used as a reference design and modified for other applications.
About the Author
Pierre Mars is the VP of Applications Engineering for CAP-XX Ltd. He jointly holds three patents on
supercapacitor applications. Mr. Mars has a BE electrical (1st class hons) and an MEng Sc from the
University of NSW, Australia, in addition to an MBA from INSEAD, France. He is also a member ofthe IEEE. Based in Sydney, Australia; the company can be reached at [email protected]. Design
tools, application notes and other details are available at http://www.cap-xx.com.
Top image: example of a supercapacitor from Cap XX
For more read: Energy Harvesting and Storage for Electronic Devices 2009-2019
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