Electricity Out of Thin Air: The Aluminium-Oxygen Battery
| Polish version is here |
The following article was originally published in the journal for educators Chemia w Szkole (eng. Chemistry in School) (5/2016):

Aluminum–air battery
The modern era can certainly be described as the age of electricity. Much of our civilization's technology relies primarily on this form of energy.
But what exactly is electric current? It is defined as the orderly movement of electrically charged particles, known as charge carriers. The flow of current in a circuit is made possible by the presence of an electromotive force (EMF), which is produced by various types of electrical energy sources. In electrochemical cells, the EMF arises from chemical reactions occurring within the cell. Closing the external circuit creates a potential difference (voltage, U) that drives the movement of charge, which results in the flow of electric current.
Sources of electric current must create a potential difference by converting other forms of energy. Galvanic cells, which rely on chemical energy, date back to the late 18th century and the work of Luigi Galvani, who observed that dissected frog muscles contracted upon contact with metal instruments [1]. Inspired by these observations, Alessandro Volta demonstrated that two dissimilar metals immersed in an electrolyte could generate an electric current [2].
Today, one of the most commonly used cells, although increasingly replaced by newer technologies, is the type developed in 1866 by French chemist Georges Leclanché. A schematic of its dry-cell version (i.e., without a liquid electrolyte) is shown in Fig. 1.

In addition to Leclanché (zinc-carbon) cells, many other types of electrochemical cells are widely used today, including alkaline, lithium, and others.
In most cases, constructing efficient galvanic cells involves the use of hazardous materials, including toxic or corrosive substances. This makes them less suitable for educational environments, such as classrooms or school laboratories. For this reason, I’d like to introduce the aluminum-air cell, a system that does not rely on toxic chemicals. It is also quite unique in that one of its electrodes is atmospheric oxygen. In a way, we’ll be generating electricity from the air!
Experiment
To build the aluminum air cell described here, you only need a few easily accessible materials:
- aluminum Al
- activated carbon C
- sodium chloride NaCl
Aluminum is a silvery-white metal with relatively low density (2.7 g/cm3 or 0.0975 lb/in3), as well as excellent malleability and ductility. It is also a good conductor of electricity [3]. For this experiment, ordinary household aluminum foil works well (Photo 1a).
Activated carbon consists mostly of amorphous elemental carbon, along with traces of microcrystalline graphite and ash. Its most notable property is its extremely large surface area. Surprisingly, just one gram (0.035 oz) of activated carbon can have a total surface area of up to 3,300 m2 (35,520 ft2) [4]. This makes it a highly effective adsorbent for many chemical substances.
Activated carbon has a wide range of uses. In medicine, it is used to treat poisoning caused by drugs or other chemical substances. In the chemical industry, it serves as a catalyst and carrier, and it is also commonly used in various types of filters. For our experiment, activated carbon works best in the form of small grains or pellets (Photo 1b).
c – table salt
Sodium chloride is simply regular table salt, which can be purchased at any grocery store (Photo 1c).
Building the cell is straightforward. The anode, which functions as the negative terminal, is made from a sheet of aluminum foil (Photo 2A).
Next, place a sheet of filter paper over the aluminum foil. Paper towels or laboratory filters work well for this purpose. Saturate the paper with a concentrated aqueous solution of sodium chloride (Photo 2B). Then, spread an even layer of activated carbon over the paper, just thick enough to cover it. Finally, place another sheet of aluminum foil on top of the carbon layer. Make sure the top and bottom foil layers do not come into direct contact.
It's a good idea to place the entire cell on a waterproof, non-absorbent surface, since the electrolyte may leak through the layers.
In this setup, the bottom sheet of aluminum foil serves as the negative terminal, while the top sheet functions as the positive terminal.
Now let’s see whether the cell actually generates electric current. To ensure good contact between the carbon layer and the top aluminum foil, it’s best to press it down with a heavy object, such as a large beaker filled with water (Photo 3, top).
top: general view, bottom: measured voltage and current output
A voltage measurement taken with only the multimeter as the load showed a value of 0.8 V. The short-circuit current was slightly above 22 mA. These aren’t particularly high values, but they clearly demonstrate that the cell is functioning, converting chemical energy into usable electrical energy.
But can this energy actually be useful? Let’s try to put it to work. Photo 4 shows a small DC electric motor, typically used in toys, connected to the cell. For demonstration purposes, a propeller has been mounted on its shaft.
When the cell components are firmly pressed together, either by hand or with a heavy object, the cell begins to deliver electric current to the motor, causing it to spin (Photo 5). To ensure the experiment works, the motor must be designed for low-voltage operation.
Attempts to power miniature light bulbs with this cell often fail. Most of these bulbs require a current of at least several hundred milliamps and a voltage between 2 and 6 volts, which exceeds the output of a single aluminum air cell. Increasing the surface area of the electrodes can improve performance, but doing so may be impractical in a classroom setting.
Still, powering a light source with this type of cell would be very useful. Light is a clear and instantly visible indicator of energy conversion, making it ideal for demonstrations, even in front of larger groups.
While looking for a suitable option, I turned to a now-common light source: the LED, or light-emitting diode. LEDs are optoelectronic semiconductor devices that produce light through a process called radiative recombination, which converts electrical energy directly into light [5].
LEDs require much less current to operate than traditional light bulbs. However, their minimum forward voltage is typically around 2 volts for infrared and red LEDs, and often exceeds 3 volts for white and blue ones. Because of this, it's not possible to power an LED directly from a single aluminum-air cell. Of course, you could build multiple cells and connect them in series, which also has educational value. But there’s another option: you can build a simple circuit that boosts the voltage to a level suitable for powering an LED.
Figure 2 shows the schematic of such a device.

As shown, the circuit uses only a few inexpensive and widely available electronic components. It’s a very basic step-up converter [6]. Compared to more common designs, the resistor value has been reduced to 1kΩ to allow the circuit to operate more effectively at the very low voltage and current levels provided by this type of cell.
The transformer used deserves a more detailed explanation. It’s best to wind the coils bifilar (using two wires wound simultaneously) on a small toroidal core. In the prototype, a core with an outer diameter of 12 mm (0.47 in), salvaged from a damaged computer motherboard, was used. Each winding has 27 turns of 0.3 mm (0.012 in) enameled magnet wire. The winding specifications are not critical, so feel free to experiment. I assembled my circuit on a small square piece of universal printed circuit board (Photo 6). The board measures about 2 cm (0.79 in) on each side, making the converter truly miniature. For good visibility, a white LED was used.
This converter operates as a simple inductively coupled generator, where, thanks to magnetic induction, a voltage higher than the supply voltage is applied to the LED. This is easy to verify. A white LED connected directly to the cell will obviously not light up. However, when using this circuit, the LED shines brightly (Photo 7). If the converter does not work, try swapping the leads of one of the windings.
The circuit built by the author works so efficiently that an attempt was made to create a highly miniaturized version of the cell. In this version, the anode is a strip of aluminum foil about 1 cm (0.39 in) wide and 4 cm (1.57 in) long. Regarding activated carbon, a single grain is enough! I suggest pressing it through the filter paper onto the foil using a needle held in pliers, which then serves as the cell’s positive terminal. A ready setup before moistening the paper with electrolyte is shown in Photo 8.
Of course, the cell only starts working after the filter paper is moistened with the electrolyte (Photo 9).
It is surprising that even such a simplified cell, when connected to the converter, generated a current of about 1.2 mA at 0.6 V for at least 15 minutes.
The operating time of the cell depends on several factors, primarily the amount of aluminum used for the anode, as it is gradually consumed during operation. This can be observed by examining the anode after use; the foil becomes noticeably thinner and may eventually develop holes. The filter paper separating the anode from the activated carbon must also remain moist at all times; if the electrolyte dries out, the cell will cease to function.
As you can see, this simple galvanic cell can be used for a variety of interesting experiments.
Explanation
Figure 3 shows a cross-section of the aluminum-air cell’s construction.

The cell generates electrical energy through chemical reactions involving the electrode materials: aluminum from the foil and oxygen from the air adsorbed onto the activated carbon granules.
In summary, the cell undergoes an overall reaction in which aluminum is oxidized by atmospheric oxygen in the presence of water:
This is, of course, a redox reaction. The key to the cell’s operation is the spatial separation of the oxidation and reduction reactions, known as half-reactions. At the anode, the oxidation of aluminum takes place:
At the cathode, oxygen from the air is reduced to hydroxide ions:
The electrode are, of course, consumed during the reaction as they are converted into products [7].
Because electrons are released at the anode and accepted at the cathode, a potential difference develops between the electrodes. When the electrodes are connected by a conductor, an electric current begins to flow.
You will likely agree, my dear reader, that oxygen seems like an unconventional choice for a cell’s electrode. It is important to remember that gaseous oxygen is essentially a poor conductor of electricity. This is where activated carbon plays a vital role. Thanks to its large surface area and adsorption capabilities, it acts as an effective gas reservoir. It also conducts electricity well enough to collect charges, which are then transferred to the upper layer of aluminum foil. The foil’s sole purpose is to serve as a charge collector from the carbon particles and does not participate in the chemical reactions.
A cell built this way has relatively high internal resistance, partly due to the limited contact area between the activated carbon grains and the collector. Compressing the cell improves contact and lowers resistance, enabling higher current output.
Is oxygen really consumed in the reaction? This is easy to observe in the miniature cell version (Photo 8, Photo 9) by coating the activated carbon grain with something like paraffin. This blocks access to air so the oxygen supply is quickly used up and the cell stops working.
The aluminum air cell is not just a laboratory curiosity. With modifications, it is being considered as a potential energy source for applications such as electric vehicles [8].
References:
- [1] Galvani L., De viribus electricitatis in motu musculari commentarius, De Bononiensi Scientiarum et Artium Instituto atque Academia Commentarii, 1791, vol. VII, pp. 363-418 back
- [2] Pancaldi G., The Battery, w: Volta: Science And Culture In The Age Of Enlightenment, Princeton Universyty Press, 2005, pp. 178-189 back
- [3] Lide D.R., CRC Handbook of Chemistry and Physics, CRC Press, 2009, pp. 40-44 back
- [4] Dillon E.C., Wilton J.H., Barlow J.C., Watson W.A., Large surface area activated charcoal and the inhibition of aspirin absorption, Annals of Emergency Medicine, 1989, 18(5), pp. 547-552 back
- [5] Moss S.J., Ledwith A., The Chemistry of the Semiconductor Industry, Springer, 1987 back
- [6] Ples M., Joule thief, online: http://weirdscience.eu/Joule%20thief.html [access: 22.09.2016] back
- [7] Fitzpatrick N., Smith F., Jeffrey P., The Aluminum-Air Battery, SAE Technical Paper, 1983 back
- [8] Yang S., Design and analysis of aluminum/air battery system for electric vehicles, Journal of Power Sources, 2002, 112, pp. 162-201 back
All photographs and illustrations were created by the author.
Marek Ples