Demonstrating Electrostatics

Demonstrating Electrostatics
Image courtesy of WikimediaImages via Pixabay.

Prerequisites Required- None

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Be certain to read the Some Comments on Accuracy section at the end of this article to ensure that historically out of date theories presented here do not circulate in modern contexts.

Today, we set out to demonstrate one of mankind's first experiences with electricity; electrostatics. If you've ever observed your hair behaves strangely after it's been rubbed by a balloon, you've experienced electrostatics.

This demonstration requires some fur, silk, two glass rods, some string, and a stand to hold one of the rods.

Figure 1: An electrostatics demonstration can be performed with two glass rods, some fur, silk and a stand.

The fur, silk, and glass rods can be easily purchased online. The stand was laser cut from clear acrylic but could be 3D printed, made using a building set, or otherwise improvised. The stand model is available here: Rod Stand

As a control, we start by bringing the two glass rods near each other. As expected, nothing particularly interesting happens.

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Figure 3: Glass rods don't normally interact

For the first part of our demonstration, we rub both glass rods with silk.

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Figure 4: Glass rods being rubbed with silk

After rubbing them, we again bring them near each other. Surprisingly, we find that the rod in our hand repels the other rod! By following along with the rotating rod, we can actually get it to spin pretty fast.

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Figure 5: After rubbing glass rods with silk, they repel each other.

During the 1700's, steam engines, advanced metallurgy, and mass manufacturing methods began to revolutionize society. Careful observations of physics led to deep and reliable models for designing new machinery. Though this rubbing phenomena was well known as far back as 600 BC (Greek philosopher Thales rubbed amber with silk to attract small objects), the idea of being able to move objects around without even touching them was very compelling for scientists.

American philosopher Benjamin Franklin observed this rubbing behavior and theorized that by rubbing the glass rods with the silk, an invisible fluid was transferred from the silk onto the glass during the rubbing. He called the glass positive as his theory predicted that the silk deposited some kind invisible electrical fluid onto the rod. He also theorized that this electrical fluid repels itself so that when both rods are rubbed with silk, they also repel each other.

For the second part of our demonstration, we rub one of the glass rods with fur.

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Figure 6: Glass rod being rubbed with fur

After rubbing with fur, we bring the two rods close together and observe the hanging rod is attracted to the rod in our hand. This is the opposite behavior from when both rods had been rubbed with silk!

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Figure 7: If one rod is rubbed with silk and the other with fur, they attract each other.

Here, we might theorize that the invisible electrical fluid was transferred from the rod to the fur so that the fur rubbed rod has a deficiency of electrical fluid. We call this negative. Perhaps as the extra electrical fluid on the silk rubbed rod is repelling itself, it is attracted to the lack of electrical fluid on the fur rubbed rod because the fluid has a tendency to transfer and equalize between two objects.

If we rub both rods with fur, we once again find that they repel.

We therefore conclude that if two objects both have excess or deficient electrical fluids they repel each other while if one object has excess and the second object is deficient, they attract. Benjamin Franklin called this fluid charge and defined glass rubbed with silk as positive and glass rubbed with fur as negative.

Finally, we test what happens if we've rubbed only one of the rods with a material while leaving the other neutral. We first bring the rods back to neutral by rubbing them together until we find that they once again do not influence each other when brought close together. We can depict this neutral condition (where both rods have the same amount of fluid) by the below diagram.

Figure 8: A diagram of two rods with normal neutral amounts of electrical fluid (shown by the droplet icons). The rods to not attract or repel each other.

We rub the rod in our hand with silk and observe that the two rods attract! We might theorize that the excess fluid on the positively charged rod in our hand has repelled the fluid on the hanging rod to the backside, which causes the front side of the hanging rod be negative so that the hanging rod is attracted to the rod in our hand.

Figure 9: Theory of induced attraction between positive hand rod and neutral hanging rod.

We now rub the rod in our hand with fur, bring it near the hanging rod and observe that they still attract! We might theorize that the negatively charged rod in our hand has attracted the fluid on the hanging rod to the front side, which causes the front side to be positive so that the hanging rod is attracted to the rod in our hand.

Figure 10: Theory of induced attraction between negative hand rod and neutral hanging rod.

Below is a table of the results for our demonstration:

Hanging Rod Rubbed Material Held Rod Rubbed Material Effect
None None No Interaction
Silk Silk Repel
Silk Fur Attract
Fur Fur Repel
None Fur Attract
None Silk Attract

The below diagrams show Franklin's electrical fluid theory for several different situations:

Figure 11: A diagram of two rods with normal neutral amounts of electrical fluid (shown by the droplet icons). The rods to not attract or repel each other.

Some Comments On Accuracy

In this article we demonstrated how glass rods repel and attract when rubbed with different materials and interpreted the results through the lens of Benjamin Franklin's theories. I've intentionally presented electrostatics in this context to help build an intuition for the electrical phenomena.

Though observing phenomena through the lens of historical figures helps us to sympathize with their journey many of these theories are deficient. For example, we now know that the 'invisible fluid' Franklin described are electrons and that when rubbed with silk, the glass rod actually loses electrons rather than gaining them.

As we continue into more advanced experiments, our theories for the underlying behavior of electrostatics will become more correct. Franklin's electrical fluid theory should not be applied to modern contexts.