We'll determine the potential
difference (voltage) between a point deep in the soil (b) and a point
close to the grounding electrode (a).
Here's the remainder of the calculation. A grounding
resistance of 40 ohms would be pretty good for Tucson.
What sort of an over voltage might you expect on an incoming power
line? Uman addresses that question in his book "The Art and
Science of Lightning Protection." Apparently the insulation
levels on the AC wiring in a typical home are 5000 to 10,000
volts. This includes insulation on the wiring, in wall outlets,
lamp fixtures, switches, and that sort of thing. So in one
respect this acts as a Surge Protection Device (SPD also formerly known
as a Transient Voltage Surge Supressor). Transients on power
lines are usually a few 100s of volts. In the upper 1% of cases
overvoltages might range from 300 volts to a few 1000s of volts (the
latter coming from a nearby strike).
One of the first protection considerations is the concept of
topological shielding. The idea is shown on a figure handed out
in class and reproduced below (source: "Applications of
Advances in Lightning Research to Lightning Protection," M.A.
Uman, Ch. 5 in The Earth's Electrical Environment, National Academy
Press, 1986. available
online)
Power and signal connections to a building (a) before and (b)
after topological shielding principles are applied.
Schematic representation of
topological shielding. Basically a signal from outdoors (Zone 0)
must pass through a SPD before entering the building. This surge
surpressor is mounted and grounded on the outside of the
building. The signal cable then probably goes to electronics that
is in a metal rack or cabinet. The signal passes through another
SPD before entering the rack or cabinet. The exterior surface of
the rack or cabinet is bonded to the inside wall of the building; this
is the Zone 1 ground. The same scenario is repeated at each
additional enclosure. You end up with nested zones or volumes of
protection.
What might the transient protection look like. In the most
general terms it will probably consist of a blocking impedance followed
by a shunt impedance.
The blocking impedance tries to keep the transient from reaching
the electronics. The shunt attempts to divert the transient
signal to ground.
For the signal of interest, Z1 should appear as a low impedance.
You might use an inductor if the incoming signal is low frequency (60
Hz power for example) and you want to block high frequency
transients. If the incoming signal is high frequency, a capacitor
would block low frequency transients.
The shunt resistance should appear as a high impedance for the signal
of interest.
I've always thought it was a good idea to provide an alternate path to
an incoming signal that encounters a blocking impedance. I.e.
something like the following:
The first impedance is often a gas discharge tube.
A gas discharge tube or "spark gap" is an example of a "crowbar"
device. It attempts to short circuit the signal once a voltage
threshold is reached (like putting a crowbar across the signal
leads). The figure below (from Uman's lightning protection book)
was on a class handout and shows the operating characteristics of a gas
discharge tube.