A classic Tesla coil consists of two inductive-capacitive
(LC) oscillators, loosely coupled to one another. An LC oscillator has two main
components, an inductor (which has inductance, L measured in Henrys) and a
capacitor (with capacitance C measured in Farads). An inductor converts an
electrical current (symbol I, measured in Amperes) into a magnetic field
(symbol B, measured in Tesla [yes, named in honor of Nikola Tesla]), or a
magnetic field into a current. Inductors are formed from electrical conductors
wound into coils. Capacitors consist of two or more conductors separated by an
insulator. A capacitor converts current into an electric field (symbol V,
measured in Volts) or an electric field into current. Both magnetic fields and
electric fields are forms of stored energy (symbol U, measured in Joules). When
a charged capacitor (U=CV2/2) is connected to an inductor an
electric current will flow from the capacitor through the inductor creating a
magnetic field (U=LI2/2). When the electric field in the capacitor
is exhausted the current stops and the magnetic field collapses. As the
magnetic field collapses, it induces a current to flow in the inductor in the
opposite direction to the original current. This new current charges the
capacitor, creating a new electric field, equal but opposite to the original
field. As long as the inductor and capacitor are connected the energy in the
system will oscillate between the magnetic field and the electric field as the
current constantly reverses. The rate (symbol [Greek nu], cycles per second or
Hertz) at which the system oscillates is given by (the square root of
1/LC)/2pi. One full cycle of oscillation is shown in the drawing below. In the
real world the oscillation will eventually damp out due to resistive losses in
the conductors (the energy will be dissipated as heat). In a Tesla coil, the two inductors share the same axis and
are located close to one another. In this manner the magnetic field produced by
one inductor can generate a current in the other. The schematic below shows the
basic components of a Tesla coil. The primary oscillator consists of a flat
spiral inductor with only a few turns, a capacitor, a voltage source to charge
the capacitor and a switch to connect the capacitor to the inductor. The
secondary oscillator contains a large, tightly wound inductor with many turns
and a capacitor formed by the earth on one end (the base) and an output
terminal (usually a sphere or toroid) on the other.
While the switch is open, a low current (limited by the
source) flows through the primary inductor, charging the capacitor. When the
switch is closed a much higher current flows from the capacitor through the
primary inductor. The resulting magnetic field induces a corresponding current
in the secondary. Because the secondary contains many more turns than the
primary a very high electric field is established in the secondary capacitor.
The output of a Tesla coil is maximized when two conditions are met. First,
both the primary and secondary must oscillate at the same frequency. And
secondly, the total length of conductor in the secondary must be equal to one
quarter of the oscillator's wave length. Wave length (Greek lambda, in meters)
is equal to the speed of light (300,000,000 meters per second) divided by the
frequency of the oscillator.
Tesla
coils differ in the type of switch used, the physical size of the components
and the input voltage. Automotive ignition coils typically have a twelve volt
input and are switched by a distributor, with moving contacts. They provide an
output of 15-20,000 volts. Television fly-back transformers produce lower
outputs but usually have 120 volt inputs and are switched by transistors or, in
very old sets, vacuum tubes. The classic Tesla coil is switched by a spark gap.
In this case, the primary circuit is known as a tank circuit. In its simplest
form, the spark gap switch has two conductors separated by an air gap. When the
electric field stored in the capacitor reaches a level sufficient to ionize the
air within the gap a highly conductive plasma is formed, effectively closing
the switch. Spark gap switched coils operate with inputs of about 5-20,000
volts and produce outputs of 100,000 to several million volts. For the spark
gap to be effective, it must be able to open rapidly after the primary
oscillation has damped out, in order that the capacitor may recharge. This is
achieved by several methods, all of which amount to ways of cooling and
dissipating the hot plasma formed during conduction. The simple gap can switch
a few hundred watts of input power. Forced air cooling of the gap and, or using
a number of gaps in series can increase power handling to several thousand
watts. Higher power levels usually require a rotary gap, which mechanically
moves gap electrodes rapidly into and out of conduction range. I should note
here that even at input power levels of a thousand watts, the instantaneous
power levels during gap firing can reach a million watts or more.
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