Electric Wind
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Electrostatics
Imagine a sphere made of a highly conductive material. In such a case, the charge on its surface will distribute itself evenly, as there is no reason for any region to have a higher concentration than another.
Now, let's conduct a thought experiment and consider a conductor with a shape other than a sphere. The electric potential must be equal at every point on its surface. As a result, charge density becomes inversely proportional to the radius of curvature at a given point. The smaller the radius of curvature, the higher the charge density.
A charged conductor with sharp edges tends to lose its charge easily. This occurs because the sharp edges have an extremely small radius of curvature, leading to a very high charge density. At such high densities, the surrounding air molecules become ionized, allowing charge to be transferred to air particles. This process generates what is known as an electric wind.
The principle behind this phenomenon applies to both positive and negative charges. It is illustrated in the following diagram:

At the tip of the sharp edge, charge density reaches its maximum. When it becomes high enough, neutral gas molecules near the tip are ionized, meaning they gain an electric charge. Since like charges repel, these charged gas molecules are pushed away from the tip, creating a directed airflow known as the electric wind.
We can attempt to observe this phenomenon ourselves.
Experiment
To generate high voltage, we can use a Van de Graaff generator, a school electrostatic machine, or a ZVS high-voltage generator. For details on how to build a ZVS generator, I encourage interested readers to visit my dedicated page on this device. In addition, we will need a candle and a thin, sharply pointed wire to serve as the tip.
Warning: I do not recommend using a ZVS system for beginners who lack experience with high-voltage circuits. The output of this device can reach several thousand volts (kV), posing a serious risk of electric shock. Mishandling it could result in severe injury. The author assumes no responsibility for any damage or harm that may occur. Proceed at your own risk!
One output terminal of the ZVS should be grounded, while the other is connected to the sharp tip, positioned facing the candle flame:

When the power supply is turned on, high voltage is applied to the tip. As a result, an electric wind emerges from the tip. This wind can push the flame to the side or even extinguish it, as shown in the following video:
The tip is positioned on the right side. The airflow is strong enough to be felt by hand as a cool breeze. Additionally, you may notice the distinct smell of ozone, a byproduct of ionization.
The force of the electrostatic wind in this setup is so strong that it can easily blow away small Styrofoam particles:
During the electric wind phenomenon, corona discharge also occurs. You can read more about this effect on this page.
This principle is applied in ionocrafts (electrostatic lifters) and corona spinner (described here). More recently, the concept of electrostatic wind propulsion has been investigated as a potential means of propulsion for small spacecraft and interplanetary probes.
Enjoy experimenting and have fun learning! :)
Further readings:
- Gębura G., Metodyka eksperymentu fizycznego w szkole podstawowej, PWN, Warszawa, 1978
- Griffiths D.J., Introduction to Electrodynamics, Prentice Hall, Nowy Jork, 1999
- Perelomov A.M., Popov V.S., Terent'ev M.V., Ionization of Atoms in an Alternating Electric Field, Soviet Physics JETP, 1966, 23(5), pp. 924
Marek Ples