Hertz Resonator
electromagnetic energy - LC oscillators - radio waves
What it shows:
The transmission and detection of radio frequency electromagnetic radiation by use of LC oscillator circuits
recreates the discovery by Hertz of a method to generate and detect electromagnetic waves.
How it works:
The core of the apparatus (figure 1) is a series LRC circuit (the R provided by the circuit resistance). The
inductor L is a 1m diameter loop made of 1 inch copper tubing which also serves as the radiating antenna.
A transformer
1
supplies 15kV to charge up the capacitor
2
until the breakdown voltage of the air between the spark gap is reached. At breakdown, a spark completes
the LC circuit which oscillates at its resonant frequency ϛ given by
For L=2 μH and C1=1.28 nF the oscillating frequency is 3 MHz. During each oscillating
cycle, a percentage of the electrical energy (around 15-20%
3
) is radiated as RF by the loop antenna so the oscillations die off after five or six cycles. Of course, the spark
gap discharge is occurring with a frequency of 60 Hz, fast enough to appear continuous to our eye but much
slower than the decay time of the LC oscillations.
Figure 1. Oscillator / radiator circuit
The detector (figure 2) is a tuned receiver with the same resonant frequency as the transmitter. It too consists
of 1m copper loop, a series capacitor C2=1.28nF and neon bulb.
4
Because the neon conducts when the potential across the cap is 60V, there's no need for a high voltage cap in
the receiver. At a distance of up to few meters, the detector circuit will ring and the bulb will light. Although
this is the range limit for a bulb detector, a CRO in its place will detect the RF signal across the lecture hall.
Figure 2. Receiver / detector circuit
Setting it up:
The transmitter has a dedicated (waist height) wooden cart, with the components laid out pretty much as in the
figure. The detector loop is hand-held - be careful where it is placed when not in use; the bulb is exposed and
fragile (as we've found out!).
Caution: Be very careful not to touch the exposed LETHAL 15kV of the transmitting coil antenna!
Comments:
A variation on the original experiments performed by Heinrich Hertz between 1886 and 1891 to transmit and
detect radio frequency electromagnetic radiation. Hertz's original apparatus used a dipole E field antenna as
transmitter and square loop receiver with spark gap instead of the neon bulb. Here our transmitter is a loop B
field antenna Remember to point out how critical the orientation of the detector loop is to the dipole field.
If its plane is perpendicular to the filed, the bulb won't light. A magnificent setup just to light a puny neon bulb,
but the spark discharge makes up for it! Rating****
References:
H. Hertz, Electric Waves, translation by D. E. Jones, Dover Publications, New York, 1962
J. H. Bryant, Heinrich Hertz: The Beginning of Microwaves, IEEE Service Center, Piscataway NJ 08854, 1988
1
Jefferson Electric Company Luminous Tube Transformer (Bellwood, Ill.)
2
2 x Sprague (6626) 3900mmF 30kV capacitors in series
3
A value quoted for a Hertzian dipole antenna; we haven't the data for a loop antenna.
4
Bulb is, was, a GE type R1A
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