I had the luxury of testing out my “lightning probe,” if you will, the day after I installed it. I was, needless to say, very disappointed with the results. I did not notice any arcing and I did not pick up any measurable DC voltages on the probe. In light of these disappointments I figure its a good time to go back to the drawing board and think of another way that I can potentially get some vaguely interesting results from this experiment.
First, I must find a way to calculate the amount of charge that will pass the airgap, and the rate at which this happens. It is possible for charges to flow through an airgap without causing a visible arc. In fact, in any material where an electric field is present, there is always some amount of charge flow. This has a lot to do with probability. I will not claim to understand these processes, but I will say that they can only be explained by quantum mechanics. It is not a fully understood process since the theory involved is largely dependent on quantum tunneling. But that’s about as far as I’ll go with that. Let’s take baby steps here.
Since I do not have a PhD in electrodynamics, nor access to the research data I need, I will have to do some experimentation. It adds to the fun! I think I have a pretty good idea of what I must do now, but it will present some practical challenges.
In order to get the biggest spark possible, I must find a way to maximize the amount of charge flow through the gap. Charge flow is limited because as charge flows, it will neutralize the electric field between the gap. However, by increasing the CAPACITANCE of the gap, this will increase the amount of charge flow before the electric field gets neutralized.
By definition, Q = V*C, which means that the amount of charge present on a capacitive surface is equal to the voltage times the capacitance. I’m going to assume that 10kV is a fairly common voltage to expect while using my probe during a thunderstorm. I also expect that the arc will end when the voltage drops down to about 5kV. This is purely an approximation from observations on YouTube. As far as charge flow, I’m thinking that I want to see at least 1mA for 1ms. This creates a pretty decent arc. Should be visible enough. 1mA for 1ms is a total charge flow of 1µC. So, now to use the formula:
Q = (dV)*Capacitance
1µC = (10kV – 5kV)*Capacitance
Capacitance = 200pF
This means that the minimum capacitance required to create a 1mA spark for 1ms is 200pF. But, there’s a catch. The capacitor also has to be rated for about 100kV minimum, which drastically changes the picture. I’ll either have to buy a $100 capacitor, or create my own. Creating my own shouldn’t be too hard, but it would have to be HUGE….
C = εA/d
A capacitor is essentially two flat conducting surfaces that are separated by an insulating material. If I were to build one, it would most likely be foam or something similar. This formula means capacitance is equal to the permittivity of the insulating material times the surface area of the capacitor divided by the distance between the two surfaces.
Let’s consider an airgap capacitor:
ε = 8.854pF/m
d ≥ 1cm (must be high enough to prevent dielectric breakdown within the capacitor)
C = εA/d
200pF = (8.854pF)*A/(3cm)
A = .672m2
So this means that I have to place two plates of metal with an area of .672m2 adjacent to each other, separated by 3cm. The area of the plates is about the size of a bike wheel… fairly large. One capacitor plate must be connected to the lightning rod terminal, and the other must be connected to ground.
However, if I use pyrex glass, which has a permittivity of 30 times that of air, plus a much higher dielectric breakdown voltage, I can construct a capacitor that’s roughly the size of a dinner plate. Wow… captain obvious, what should I do?
I can leave my airgap the way it is. The only difference is the addition of the capacitor in parallel to the airgap, which allows the system to capture more of the atmospheric energy. There’s plenty to go around… the discharge of lightning in itself is about 100MJ, which is enough to power about 1 homes for a day.
Here’s the planned setup:
Basically, the capacitor is just in parallel to the airgap for the purpose of increasing the amount of energy captured by the system. The hardest part will be constructing the capacitor, and yet, it’s possible using things around the house… as soon as I get some time, I’m going to construct this. Hopefully I’ll get a good thunderstorm before I have to leave for Purdue.