'Energy-sucking' Radio Antennas,
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HOW DO ATOMS DO IT?I stumbled across the answer to my questions in a paper about VLF/ELF loop antennas. Apparently Quantum Mechanics does not supply the answer. Instead the question of small antenna behavior is resolved by a little-known section of classical electromagnetism. It involves resonance, but more importantly, it involves the magnetic and electric fields which surround any antenna. (I guess I should have expected this. After all, much of physics works fine with classical concepts, with photons and EM waves both explaining the same phenomena.)
An "electrically small" antenna is one where the physical antenna size is
far smaller than the EM wavelength being received. At first glance,
electrically small antennas aren't all that strange. If we use them to
transmit radio waves, they work just as you'd expect. In order to
force a tiny antenna to send out a large amount of EM energy, we can
simply give it a huge driving signal (high voltage on a tiny dipole, or
high current on a tiny loop antenna.) If the EM fields are strong at a
distance of 1-wavelength from the small antenna, then the total EM
radiation sent out by the antenna will be significant. It's almost as if
the EM fields themselves are acting as the antenna. Weak fields act
"small," while intense fields behave as a "large" antenna. This explains
how a tiny antenna can transmit lots of EM. But what about reception?
It turns out that a similar idea works for reception; for "input" as
opposed to "output." By manipulating the EM fields, we can force an
electrically-small receiving antenna to behave as if it was very,
VERY large. The secret is to intentionally impress an artificial
AC field upon the receiving antenna. We'll transmit in order to receive,
as it were. Conventional half-wave antennas already do exactly this
because their electrons can slosh back and forth, generating their own EM
fields. For example, the thin wires of a half-wave antenna are far too
thin to block any incoming radio waves and absorb them. However, the
current in such an antenna, as well as the voltage between the two wires,
these send out large, wide, volume-filling EM fields which have a constant
phase relative to the incoming waves. Because of the constant phase,
these fields interact very strongly with those incoming waves. They create
the lobes of an interference pattern, and this pattern has an odd
characteristic: some of the incoming energy has apparently vanished. The
fields produced by the antenna have cancelled out some of the energy of
the impinging EM waves.
TRANSMIT IN ORDER TO RECEIVE?!!!Rather than relying upon the wiggling electrons in the wires of the large half-wave antenna to generate EM fields... what if we used use a power supply instead? If an antenna is 1/10,000 wavelength across, we should be able to force it to behave as if it's huge; perhaps 1/3 wavelength across. We simply have to drive it hard with an RF source. We must drive it at the *same* frequency as the incoming waves, then adjust the phase and amplitude of the power supply to a special value. At one particular value, our transmissions will cause the antenna to be best at absorbing the incoming waves.
Take a loop antenna as an example. If we want our little loop-antenna to
receive far more radio energy than it normally would, then we need to
produce a large AC
current in the antenna coil, where the phase of this current is locked
synch with the waves we wish to receive, and is lagging by 90 degrees.
The voltage across the antenna terminals stays about the same as when an
undriven antenna receives those waves. However, since the current is much
higher in the driven antenna, the energy received per second is much
higher as well. This seems like engineering blasphemy, no? How can
adding a larger current increase the RECEIVED power? And won't our
receiving antenna start transmitting? Yet this actually does work.
Power equals volts times amps. To increase the RF power received from
distant sources, we increase the antenna's amperes intentionally.
This sounds really silly. How can we improve the reception of an
electrically small antenna by using it to *transmit*? The secret involves
the cancellation of magnetic or electric fields in the near-field region of the
antenna. The physics of the nearfield region of antennas has a kind of
nonlinearity because conductors are present. In the electromagnetic
nearfield region, it's possible to change the "E" of a wave without
changing the "M" (change the antenna's voltage without changing the
current), and vice versa. Superposition of EM traveling waves does not
quite apply here because the ruling equations for energy propagation near
conductors depends upon V^2 or I^2 separately. In addition, V is almost
independent of I in the near-field region. If a very small loop antenna
(a coil) should happen to receive a radio wave as a very small signal, we
can increase the received *energy* by artificially increasing the current.
Or if we're using a tiny dipole antenna (a capacitor,) we can increase the
short dipole's received energy by applying a large AC voltage across the
NOT CRACKPOTTY AFTER ALLNote that this does not violate any rules of conventional physics. If we add stronger EM fields, they sum with the incoming EM plane waves and cause these radio waves to bend towards the tiny antenna, and the antenna absorbs them. This increases the antenna's EA (effective area, or effective aperture.) We can use this process to alter the coupling between the antenna and the surrounding space, but the total energy still follows the conservation law. The altered fields only change the "virtual size" or EA of the antenna.
More importantly, the phenomenon is quite limited. We can only
with electrically "small"
antennas. We cannot increase the "virtual size" much beyond a quarter
wavelength for the waves involved. If we already have a large 1/2-wave
dipole, then no matter how large is our artificially-add AC voltage,
we cannot make it absorb more incoming waves.
However, if we have an extremely small antenna, say, a
10KHz loop antenna the size of a pie
plate, we can make that antenna seem very, very large indeed. Think like
this: how large is the diameter of the antenna's nearfield region at
10KHz? Around 10 kilometers? What if we could extract half of the
incoming energy from that entire volume?!! In theory we can: half can be
absorbed, and the other half scattered. In theory a tiny loop antenna
sitting on your lab bench can intercept just as much energy as a longwire
1/2-wave antenna which is 10KM long. Bizarre, eh?
Here's a way to look at the process. If I can create a field which
CANCELS OUT some of the energy in an extended region surrounding a tiny
antenna, this violates the law of Conservation of Energy. Field energy
cannot just vanish! That's correct: if we cancel out the energy in the
nearfield of an antenna, this is actually an absorption process, and the
energy winds up inside the antenna circuitry. By emitting an EM field, a
receiving antenna sucks EM energy into itself. If we ACTIVELY DRIVE an
antenna with an "anti-wave", we will force the antenna to produce stronger
fields which cancel the incoming waves, and simultaneously the antenna
absorbs more energy from the EM fields in the surrounding region of space
than it ordinarily would. It also emits some waves of its own. But in
antenna theory these waves are identical to the received signals, and they
are considered to be reflected or "scattered" from the antenna. It's a
general law that we cannot receive EM waves without scattering half of the
energy away again.
Here's the interesting part. If we wish to receive power rather than
signals, a critical issue arises.
Driving a tiny antenna with a large signal will create large currents and
heat the antenna. Small antennas are inefficient when compared to
half-wave dipoles. If we wish to maximize the virtual aperature of a
really tiny antenna (e.g. make our 10KHz pie-plate coil act 10KM across,)
we'll quickly be frustrated by wire heating. All the extra received
energy will go into warming the copper. Possible solutions: use
superconductor loops, or at low frequencies use the nearest equivalent to
an AC-driven superconductor: a rotating permanent magnet or rotating
BUT HOW DO ATOMS DO IT?OK, if this supposedly explains how tiny atoms can receive long light waves, how can we increase the voltage signal to a SINGLE ATOM?! Actually it's not difficult. No angstrom-sized radio transmitter is needed. The key is to use EM energy stored as oscillating fields; i.e. resonance.
If an atom resonates electromagnetically at the same frequency as the
incident light waves, then, from a Classical standpoint, that atom's
internal resonator will store EM energy accumulated from the incoming
waves. It will then behave as an oscillator, becoming surrounded by an
increasingly strong AC electromagnetic field as time goes by. (Quantum
Mechanics might say that the atom is surrounded by virtual photons at the
resonant frequency.) If this alternating field is locked into the correct
phase with the incoming light wave, then the atom's fields can interact
with the light waves' fields and cancel out quite a bit of the light
energy present in the nearfield region around the atom. The energy
doesn't vanish, instead it ends up INSIDE the atom. Half of the energy
goes into kicking an electron to a higher level, and the other half is
re-emitted as "scattered" waves.
By resonantly creating an "anti-wave", which superposes with incoming
waves and bends them towards the atom, the tiny atom has "sucked energy"
out of the enormously long light waves as they go by. And since the atom
has no conventional copper coils inside it wasting energy, it can build up
some really strong fields which allow it to behave extremely "large" when
compared to it's physical diameter.
Impossible? Please track down the C. Bohren paper in the
below. He analyzes the behavior of small metal particles and dielectric
particles exposed to long-wave EM radiation, and rigorously shows
with semi-Classical analysis that
the presance of a resonator can cause dust motes to "act larger than
they really are."
How can this stuff be true?! After all, electric and magnetic fields
cannot BEND other fields. They cannot affect each other directly. They
work by superposition. For the same reason, a light wave cannot deflect
another light wave. Ah, but as I said before, the mathematics of the
fields around a coil or a capacitor are not the same as the mathematics of
freely-propagating EM waves. If we add the field of a bar magnet to the
field of a radio wave, and if the bar magnet is in the right place (at a
spot where the phase of the b-field of the radio wave is reversing
polarity,) then the radio wave becomes distorted in such a way that it
momentarily bends towards the bar magnet. And then, as the EM wave
progresses, we must flip the magnet over and over in order to keep the
field pattern from bending away again during the following half-cycle.
The energy flow continues to "funnel in" towards the rotating magnet.
Now replace the bar magnet with an AC coil, and vary the coil current so
the fields stay locked to the traveling radio wave in the same way. In
that case the wave energy will ALWAYS bend towards the coil and be
absorbed. Superposition still applies, but this is a COHERENT
superposition, so it acts like a static field pattern: as if a permanent
magnet can bend a radio wave inwards and absorb its energy rather than
simply having the fields sum together without interesting results.
Note that the coil will also emit its own EM ripple. This emission is
well known: atoms ideally will scatter half the light they absorb, and
dipole antennas behave similarly: they scatterer incoming EM waves as they
absorb part of the energy. When all is said and done, our oscillating
coil has absorbed half of the incoming EM energy and re-emitted (or
"scattered") the rest. In a phase-locked system, we cannot tell the
difference between reflection and transmission.
A "HOLE" IN PHYSICSWhen viewed as a halfwave receiving antenna, a resonant atom acts as if it has expanded in size to fill its entire nearfield region. In terms of Quantum Mechanics, it does so by locally creating a large virtual-photon AC field which normally would not exist. Because of coherent superposition, in a sense this new field BECOMES THE ANTENNA. The significant part of this new field extends to (Pi*wavelength)/2 distance around the atom, and this distance can be thousands of times larger than the atom's radius. A 1-angstrom atom with a large AC field can behave as a 1/3-wave antenna at optical frequencies. Though tiny, the atom can absorb "longwave" radiation such as light. Our 1-angstrom atom becomes a black sphere 2000 angstroms across, and efficiently absorbs 6000-Angstrom light waves. Very strange, no? I've certainly never encountered such a thing during my physics training. Apparently the missing details of the absorption of light wave by atoms is a "hole" in physics education, and it has only been treated in a couple of contemporary physics papers in the 1980s. Here's another hole: when an atom absorbs waves, it has to scatter away half the energy. Does this mean that when an atom absorbs a photon, it must always interact with TWO photons, eating one and reflecting the other?!!!! I've never heard of such a requirement. It flys in the face of the usual description of atoms and photons. (Is it mentioned in Feynman's QED book?)
This "energy suction" effect is not limited to atoms. We can easily
build a device to demonstrate the phenomenon. Below is
a simple physics analogy to show how tiny atoms can "suck
energy" from long light waves. Suppose we transmit a VLF radio signal at
Let's arbitrarily set the signal strength so it's about the same strength
as the Earth's weak
e-field: 100 Volt/meter. If the transmitter's e-field is contained
below the conductive ionosphere, and if the bottom of the ionosphere is
high, then the Earth's entire vertical field is about 10 megavolts top to
bottom. Our transmitter must produce such a field.
These values aren't totally ridiculous. Large, well-designed Tesla coils
commonly produce 10 megavolts. If such a coil was erected outdoors and
connected to an insulated metal tower, it would fill the Earth's entire
atmosphere with 1KHz radiation. The Earth's atmosphere would be like a
microwave oven cavity. Such an AC voltage field would produce
100V/M field everywhere on the Earth's surface. This field would be
detectable by instruments, but otherwise it would be too small for humans
to notice, and we
certainly would not expect to be able to get significant power out of it.
CAPACITIVE-PLATE ANTENNAOK, we've got a feeble AC e-field in the outdoor environment. How will a simple antenna-plate perform as an energy receiver? See fig.2 below. If it's a large horizontal metal plate about one meter off the ground, it will give out a 100 volt signal at 1KHz, but this one hundred volt "power source" has an extremely large capacitive series impedance. Let's say that the plate/ground capacitance is 10pF. To draw energy with the maximum possible voltage, the load resistor should be approximately equal to the series impedance. This impedance is dominated by the 10pF capacitor value, so this gives 1/(2*PI*F*C) = 16 megohm load resistor, and it drags the antenna's voltage down from 100V to 70.7V. The received energy in the resistor is 300 microwatts, and the current in the resistor is in the microamp range. Just as we might expect, everything here is similar to a conventional radio antenna. The weak e-field from the incoming EM waves behaves only as a "signal", and it is not a source of significant power. It can't drive a motor or light an LED.
__________ --> | 10 MVolt |_______ | @ 1KHz | | |__________| | | ___|___ Capacitance from ionosphere to plate _|_ ( very small, say 1/10,000 pF ) //// _______ | | |______________ <--- 70.7V @ 1KHz antenna | | (metal plate) ___|___ \ 10pF / 16.7 Megohm _______ \ | / |______________| _|_ //// FIGURE 2
The fundamental problem with the above system is that the empty space
around our metal plate is acting like a voltage divider. If the sky has
10 Megavolts compared to ground, and if the metal plate is a few feet
above the surface of the ground, then the plate only has a relatively tiny
voltage. Current is tiny, so wattage is also tiny. Maybe we could power
an LED flasher with this antenna... but only if we set it to flash every
few minutes. Maybe if we erected an enormous antenna tower we could do
better by lifting the plate higher from the ground (but with such a huge
antenna, we could easily steal more power by ignoring our 1KHz broadcast,
because many high-power conventional AM radio stations exist: BBC
shortwave, Voice of America, etc.)
RESONANT ANTENNANow lets add a tuned circuit to the above schematic and see what happens:
__________ --> | 10 MVolt |_______ | @ 1KHz | | |__________| | | ___|___ Capacitance from ionosphere to plate _|_ ( very small, say 1/10,000 pF ) //// _______ | | |_____________ <--- 10 Megavolts! | | antenna | \_ (metal plate) ___|___ (_) 10pF (_) Coil _______ (_) | (_) | / |____________| | _|_ 1KHz resonant, infinite Q //// FIGURE 3At resonance, the 10pF capacitance of our metal plate effectively vanishes. At resonance, an ideal parallel-resonant circuit behaves like an infinite resistor. If the LC circuit is exactly at resonance, and neglecting the resistance of the wires involved, how high will the voltage on the metal plate rise? It rises to ten megavolts!!!! The resonant circuit will continuously accumulate EM energy until the voltage at the antenna-plate rises to the same value of voltage as the transmitter. Weird!
Keep in mind that this device is a relatively small affair sitting in your
back yard. It's not a 1KHz quarter-wave dipole tower 25 miles tall.
There's no huge antenna, so we would not expect to find any huge level of
electric power appearing in the circuit. If we weren't aware of the
mechanism behind this, all we'd see is a passive LC resonator which seems
to burst into oscillation of its own accord, and the voltage grows higher
and higher until the darned thing suffers a corona outbreak or something.
Lightning bolts shoot out! The EM fields near the metal plate grow FAR
STRONGER than the weak fields already present in the environment. The
device in our back yard resembles an impossible "perpetual motion"
machine, which might make physicists suspect a hoax. However, the real
explanation is completely conventional, and the source of the energy is a
feeble, unnoticed AC e-field field produced by the very distant
10-megavolt transmitter tower.
Note: the above phenomenon can only occur for an ideal LC circuit,
where the resistance of the coil is zero and where the Q of the circuit is
infinite. If our antenna plate were connected to the resonant "secondary"
of a superconductive Tesla coil, we might in fact see the output voltage
grow to the megavolt range. However, in most real-world tuned circuits it
wouldn't reach such heights.
But remember, voltage is not energy. What will be the realistic behavior
of such a device? Perhaps the incoming power is still small (maybe like
300 microwatts we saw earlier), or perhaps it works well, yet it takes
months to build up so much voltage across even a superconductor resonator
Just what is the actual received energy flow? Let's put a resistor across
the tuned circuit so we create a flow of real energy and drag the voltage
down to, say, .707 of the unloaded voltage. The resistance should equal
the impedance of the series capacitor: 10 ^ -16 Farads, giving 1600
giga-ohms. (A huge resistor. Clearly it makes sense to try instead to
extract energy using a low-value resistor in series with the inductor
coil, rather than using a huge parallel resistor across the tuned circuit.
A 1.6 tera-ohm power-resistor might be hard to find in the surplus parts
catalogs! That is, if you don't have the parts- catalog featured in THIS
ISLAND EARTH, that old SF movie where the two engineers build an
"Interociter" from parts sold by mail-order in a strange electronics
catalog. Obviously the Interociter is Alien Tesla coil technology, aha!)
HUGE RECEIVED POWERWith our 1.6 giga-megohm resistor in place, the RF power intercepted by the small metal plate is now 30 watts. That's ONE HUNDRED THOUSAND TIMES HIGHER than the power from the simple non-resonant antenna plate. Our tiny antenna has essentially reached out and made a kind of "direct contact" with the distant transmitter. By changing its own impedance, it has converted the femtofarad "sky capacitor" into an efficient coupling device. It has sent out a cancelling wave and pulled in energy from an enormous volume encompassing the surrounding fields. It has become a "matching transformer" which steps down the 10MV sky voltage and steps up the "sky current." If we either increase the receiver plate's size, or lift it up high on an antenna tower, or connect it to a beam of x-rays which produce an ionized pathway extending vertically upwards, then the received power rises proportionally.
So, connect a high-Q resonator to a small antenna, and you'll drag in far
more wave energy. Simple?
[The engineers on SCI.ELECTRONICS.DESIGN forum have pointed out that
10MV voltage limit on the above resonator is wrong. In reality, it can
grow much higher than the voltage on the transmitter. The system is
actually series-resonant, so the output voltage is limited only by the Q
of the system (by
the resistance of the wires in the resonator coil) and is not limited by
the 10MV drive voltage of the distant transmitter.]
In our earlier antenna, (the nonresonant, resistor-only version,) a small
amount of "real power" did take a path through the capacitance of the sky
while on its way to the metal plate and to the load resistor. If the
voltage across that resistor could be forced to oscillate hugely, and if
it had the right phase compared to the tiny displacement current coming
from the transmitter, then we'd obtain a major increase in energy flow.
The tiny sky-current would remain about the same, but with the much larger
voltage on the antenna, the value for V*I is increased and wattage is
increased. Remember the unwanted capacitive-voltage-divider effect in
figure 2? With a resonant system, that effect would no longer apply, and
the output voltage would no longer be so low. Things would behave
differently. The displacement-current going through the "sky capacitor"
might still be microamps, but if the tuned circuit can alter the high
voltage at our end of the transmission system, then it can drastically
change the energy throughput. As with any power-transmission system, we
can put more power through it by raising the line voltage while keeping
the current the same.
CONCLUSIONTo sum up: we see that by putting a big AC voltage on the tuned circuit and by adjusting its phase in relation to the tiny incoming current, we can "suck" the E x M wattage from the enormously broad wavefronts of the incoming waves. It also works this way inside a simple circuit using conventional voltage dividers: add a resonant circuit, and the series impedance of the power source behaves smaller. See this example circuit. It should still work this way even when a part of the antenna circuit contains a series capacitor whose dielectric is made up of many feet (or even tens of km) of empty space. It's very much like building a high-voltage power line: to transmit high wattage on a thin wire, we use high voltage at low current, and then we put a step-down transformer at the far end of the power line. However, in the "power line" shown in the above diagram, we then put a tiny capacitor in series with the high-voltage line. Then we increase the thickness of the capacitor's air-dielectric until dielectric is miles thick and the current in the system is mostly composed of displacement current in the empty space between the pair of widely-separated capacitor plates. To transmit significant power, step the voltage up to astronomical levels at one end, then step it back down at the other end. Rather than using only a step-down transformer in the receiver, instead we use a hi-Q resonator, and we allow the resonant voltage to rise to a huge value. As a result, EM energy will be "sucked" into the receiver.
THE TESLA CONNECTIONNote that all of this stuff comes directly from Nikola Tesla's "Wireless power" transmission scheme. If we can flood the atmosphere with VLF 2KHz standing waves, and if the ionosphere keeps most of this EM energy from escaping into space, then a small, high-Q resonator can grab significant wattage right out of the air. A small resonator can produce an extensive and intense AC field of its own, and can act as an "EM funnel" which grabs significant wattage right out of the ambient radiation field. It can do so even when the ambient field is quite feeble, and even when the transmitter is thousands of KM away. This is not "radio," where wavelength is the same size as the components. This is "circuitry", where wavelength is huge, and circuits are small, and the antenna operation more resembles "AC wiring" rather than "EM radiation." This is probably the concept that put that "Mona Lisa grin" on photographs of old Nikola. And that twinkle in his eye...
If we use a metal loop-antenna instead of a metal capacitor plate, then
the current in the loop can perform a similar task as the voltage on the
plate in figure 3: the oscillating current should grow huge and surround
the coil with an intense,
volume-filling AC magnetic. If the phase is correct, this
b-field should "suck energy" from the transmitter (or from the local
b-fields of the incoming electromagnetic waves.) Keep in mind that all
this applies to SMALL ANTENNAS. If your wavelength is 150MHz and your
antenna is 1 meter across, then "energy sucking antennas" cannot be used
reception. The idea applies to the longwave bands, to longwire antennas,
and to VLF
power transmission using the Earth-ionosphere Schumann resonant cavity.
These sorts of antennas obey circuit-physics, not the physics of EM waves
in space. The region of space adjacent to ANY antenna obeys a
of circuit-physics and wave-physics, (the near-field and far-field EM
equations,) and I've never quite visualized exactly how this works. Now it
looks like there are several interesting things hidden between the
near-field and the far-field mathematics. For example, simple crystal
"energy suckers" instead of "tuners." And everyone owns invisible
antennas a thousand
meters across... generated by every AM portable radio! Cool.
NOT SO USEFUL?The "energy grabbing" effect is very limited. It's a weird laboratory curiousity. It's useful for physics education, and you can build a "Selectenna" AM/shortwave product. But to do the really impressive things you'd need almost astronomical values of "Q." Large superconducting loops. A small coil made from cheap everyday materials won't be very impressive. To perform the apparent magic you'd need massive superconductor devices and really immense AC magnetic fields. (Perhaps large heavy arrays of rotary Rare Earth magnets might substitute? Levitate and spin 'em in a vacuum chamber.)
It's also limited because it's a nearfield
effect. It could only operate within about a 1/6- or 1/4-wavelength
radius around a coil or capacitor antenna, or in the region between the
peaks of a propagating EM wave. In other words, when we add a tuned
circuit, we can increase the "effective size" of a tiny antenna until it
resembles a half-wave dipole antenna. It usually would be easier to
simply build a half-wave dipole in the first place. Normally we would do
At VHF or UHF frequencies, a hi-Q "energy sucking" resonator antenna would
not gather any more energy than a normal antenna, since the hi-Q antenna
would be electrically large. But whenever the conventional dipole antenna
might end up being too large to construct (like at 1KHz frequency or even
550KHz), then a high-voltage capacitor plate antenna, (or perhaps a
tuned-coil antenna, both with a very high Q-factor, with inductors wound
from thick copper pipe?) ...these would behave like far larger antennas
than anyone could possibly imagine.
NOT IN YOUR PHYSICS BOOKS?In hindsight, the above stuff seems somewhat obvious, but why have I never heard of it before? Atoms must transmit before they can receive photons? (Laser/Einstein insights!) RESONATING ANTENNAS BECOME ABNORMALLY EFFICIENT RECEIVERS?! And perhaps the reverse must also be true: high-field, high-Q resonant antennas will leak radio waves, even if their size is very small compared to the wavelength. If resistive losses don't halt them, their AC fields will grow in intensity until the signal finally does escape. Do most radio designers realize that all small resonant antennas with huge EM fields act like long-wire antennas having fields of the usual strength? Do Ham radio operators currently use 80-meter transmission antennas having high-Q resonators and enormous magnetic or electrostatic fields? Do AM radio companies know that their antenna towers are really not necessary, and could be replaced with a cryo-coil in a small shed? Do science teachers realize that even the simplest "crystal radio" can only drive a pair of headphones when a tuned circuit present? (The tuned circuit in a crystal radio is *not* a bandpass filter: it is an energy-suction device!) Do physicists really grasp, at a gut level, just how those tiny atoms can absorb and radiate the huge wavelengths associated with light waves? And are physicists aware that two photons are needed for atomic interaction: one to be absorbed, and one to be scattered?
Portable AM radios already employ tuned resonant-loop antennas, and
they've always been this way. We've been carrying around Nikola Tesla's
power-receiver in our back pockets since the 1960s. Also, in bygone
decades, those old "regenerative" and "superregen" receivers were not
what they seemed. They were transmitting in order to receive, they were
harnessing the same bizarre "energy sucking" process. Regeneration isn't
just a fancy way to amplify a small signal, instead it increases the
incoming signal intercepted by a short antenna via some weird EM physics.
Do the designers of 90 years ago know something that modern scientists do
UPDATE 9/6/99In thinking more on this (and while talking to people on the email lists) a couple of new thoughts have occurred to me. One: try to give your receiver's tank circuit as high a Q as possible, and then connect it to a load through a zener diode or other nonlinear device. This will allow the voltage/current of the tuned circuit to rise to a huge level and produce an intense AC field, but without the load interfering. Only after the AC field has reached the appropriate level will we extract any energy and deliver it to the load. [NO, NOT A ZENER! A zener would just act as a series RESISTANCE, dissipate heat, and throw away energy uselessly. Instead, just use a detector diode, and charge up a DC capacitor. 11/1/99]
Two: try using an FM detector circuit to force the receiver to "lock on"
to the transmit frequency. If we do this, we could still use immensely
high q-factors, but without making our frequency-match adjustments be so
sensitive. We could even send out modulated signals (broadband, not
narrowband), and still use them to power distant motors. I don't have a
solid idea of how FM detectors work, so this might not be straighforward.
Might need an active PLL driving a variable capacitor...
Three: once the receiver is oscillating and energy is being transferred,
try suddenly changing the voltage of the transmitter. Since the entire
system acts like a well-coupled transformer, I suspect that fast changes
in transmitter voltage will appear as fast changes at the receiver. Maybe
it only takes a single AC cycle for the change to appear. Weird thought:
if the transmitter is modulated *faster* than the transmission frequency,
would the fast modulation signal appear at the receiver?!!! That would be
impossible, since it would violate Shannon and the rules of AM
However, the coupled-resonator system more resembles a pair of atoms
transferring photons, rather than resembling an RF transmit/receive system.
If the device behaves like a quantum-mechanical coherent system, then
perhaps we can modulate the transmitter at a faster rate than the carrier
frequency! If it worked, that would REALLY be weird, no? Imagine
transmitting at the 59Hz earth resonant overtone frequency, then
amplitude-modulating the 59Hz carrier at 1 KHz, and having the signal
appear at the receiver's resonator! We wouldn't really be transmitting
radio energy. The signal would more resemble QM "wavefunction collapses"
which propagate throughout the Earth's ionospheric resonant cavity.
Four: 11/1/99 This circuit mimics atomic absorption, and it also should mimic stimulated emission. Once the circuit is oscillating, it's absorbing the incoming waves because of its phase. The phase relationship causes it to couple to the transmitter. If the transmitter was suddenly turned off, then maybe the circuit would not be able to radiate, since without the waves from the transmitter it could not perform the "poynting-flux emission" process. The phenomenon is definitely not linear! So... what happens when the waves from a transmitter should suddenly encounter the fields of a short antenna? If the phase is right, the short antenna should change from an oscillator to an emitter, and begin emitting energy! This is the reverse of the "energy sucking effect," because while "energy suction" can only occur when the short antenna is surrounded by a powerful field, "energy emission" can only occur when the powerful fields around a short antenna are given a traveling-wave field to provide the "stimulation" for stimulated emission to occur. Absorption/emission requires both the trapped fields at the antenna, as well as the traveling fields from a distant transmitter. If my reasoning isn't faulty (it probably is,) this means that it should be possible to build a sort of radio-freq laser, where a distant transmitter causes a small loop-antenna resonator to add its energy to the transmitted wave.
Also, my crackpot side is starting to yammer at me. It's saying that this
particular "hole in physics" might seriously damage contemporary Quantum
Electrodynamics, and might even show that Einstein's original
photoelectric experiment might be interpreted incorrectly. Hey, if
Einstein was wrong, does that mean that the Nobel is withdrawn
retroactively and awarded to whoever can show rigorously that "energy
sucking antennas" are a better explanation for QM phenomena of all kinds?
Or does it just mean that my "crackpot half" is just trying to make
certain that no conventional scientist will dare to experiment with this
BEWARE: ODDBALL IMPLICATIONSIf EM resonance is extremely important, and if mainstream science doesn't recognize the effects, then god only knows how many unusual phenomena are awaiting exploration by amateurs. The professional explorers with their well-funded troops haven't yet arrived on this particular "new continent." There are still mysteries to be experienced, and it could be many years before the whole thing is paved over with well-traveled highways built through NSF funding.
Ears as antisound-emittersWhenever any type of "small" receiver seems to be generating an AC field around itself spontaneously, perhaps we should suspect that the receiver is employing the above concepts; that it is actively generating an "anti-signal," and as a result is receiving more wave energy than it's physical size would suggest. THIS MIGHT APPLY TO ACOUSTIC SYSTEMS! If we illuminate a tiny resonant chamber with long-wave sound of the right frequency, standing waves will build up within the chamber, and it will become an emitter. If there is an acoustic analogy for the above antenna physics, the resonant chamber should "bend" the incoming sound towards itself. When the emitted sound superposes with the 3D incoming waves, the wavefronts of incoming sound will be distorted so they they impact on the resonator and thereby increase the area of its "virtual intake orifice". In EM physics this is well known, it's just the Effective Aperture concept.
Might biological evolution have "discovered" this energy-sucking resonator
effect in regards to ears? A collection of programmable resonators
might work far better than a broadband receiver, even an amplified one.
It turns out that human ears are known to generate their own signals.
Much about this is still a mystery, and proposed theories do not match
experimental findings. I note that at frequencies below a few KHz, the
wavelength of sound is physically larger than the external ear. Perhaps
our human hearing system increases its gain by emitting signals which are
phase-locked with the incoming sound? This could be easily missed, since
the emitted sound would greatly resemble the incoming sound, and could be
mistaken as a reflection.
I've heard that human ears have an unexplained property: they can detect
signals which are far below any logical noise level. Their detection
capability supposedly even exceeds the QUANTUM MECHANICAL noise level.
Perhaps ears increase their net received acoustic energy via an
"anti-sound" feedback process resembling resonance? Might there be other
situations where small acoustic resonators can receive abnormally large
amounts of energy? Shades of Ernst
Worrel Keely! Hey, maybe I finally have a clear explanation for that
Hole" phenomenon with the soda straws. And... and... once again the
Thomas Gold is vindicated, and his detractors are shown to be a bit,
shall we say, "deaf" to his words.
Side note: How might the inner ear generate sound? Maybe it does not.
Maybe it rapidly modulates the stiffness of its parts and therefore uses
nonlinear physics to take energy from other frequency bands and use it to
power an oscillation at the frequency it wishes to emit. Sort of like
using one crystal radio as a "battery" to power the audio amplifier of
another crystal radio tuned to a different station. Or like striking a
bell with slow blows, while the bell emits a fast oscillation.
Oooo, Very Weird Idea! If ears generate sound only when sound is being
received, then perhaps we can detect this. Perhaps it's even under
conscious control. When we listen intently to a particular frequency,
obviously we're tuning the brain's internal signal processing algorithms.
But what if our conscious action actually changes our inner ear mechanics,
it "sucks energy" at that frequency? If so, then just flood the room with
white noise, stick a tiny microphone near your ear, display a realtime
spectrogram of the detected noise from the microphone, then try to
concentrate on listening to the "high" tones in the noise, and later
listen to the
"low" tones. Will your ear change (will the spectrogram of the
microphone's signal change?)
Or, if you try to pick up a constant tone in the noise, will a small
absorption band appear in the spectrum of energy near your ear? Easier
test: subtract (null out) the noise-generator's signal from the
microphone's signal and observe this difference signal. (an electronic
delay line would probably be needed.) Now concentrate on listening to the
highs or the lows. Will the observed difference-signal change? If so,
build a circuit which detects this change and turns on a light bulb.
Stick a microphone in your ear, decode the alterations in the sound
spectrum, and run your appliances by "thinking" about a tone-sequence!!
If THAT works, then try this next one.
Set up the above system. Listen to the white noise, and imagine that you
hear the word "yes". Do it many times. Now play back the recording of
the difference signal (or even the raw signal from the microphone.) Can
you hear the word "yes" being transmitted by your *EARS*? If so, then you
now know how to speak through your ears. This only works when you are
listening to white-noise. Imagine that you hear music in the noise, then
see if it appears
in the recording from the tiny microphone. Perhaps composers can "think
music" right onto the tape recorder. "Think aloud" to yourself, and see
if your "verbal thoughts" can be heard issuing from your ears as they...
of your head? Perhaps one form of telepathy is... acoustic? Can a blind
person navigate via a sort of whitenoise-correlation "acoustic radar?"
OK, now hire a schitzophrenic who hears voices, and see if you can record
the "voices" via whitenoise environment and ear-canal microphones. Ask
disconnected personality fragments some questions, see if they answer.
You've invented the Ousiograph!
Now go interview the "Voices" on the Tonight Show ...with or without the
cooperation of the victim.
Who'll be the first to explore this silly idea and find out if I'm full of
BALL LIGHTNINGBall lightning is not yet explained. One of the orthodox explanations is the Storm Maser theory: if thunderstorms emit microwave energy, and if something can somehow focus this energy, then a nitrogen electrical-plasma could feed off the intense microwave flux. The "Energy sucking" theory gives us a second option. Suppose thunderstorms emit weak ELF/VLF e-fields instead of supposedly emitting intense microwaves? If a plasma happened to be resonant with the coherent AC e-field being created by the storm, and if the Q of the resonant plasma system was high, then that plasma would develop an enormous high-frequency e-field around itself. It would suck energy from the fields of the storm and remain "alight." Do nitrogen/oxygen (or carbon?) plasmas have any high-Q resonances in the ELF/VLF spectrum? The plasmas in coronas in the storm clouds might emit the same frequency that a nitrogen plasma-ball would absorb. What about carbon-fiber networks composed of condensing soot? [CORUM & CORUM] Or rather than the plasma-balls extracting energy via pure resonances, do they have self-organization which can communicate with the self-organized lightning plasmas within the thunderstorm and "agree" between themselves to create a "Tesla Power System"? We'd mistake the Ball Lightning's energy source for feeble EM white-noise. The storm becomes the transmitter and the ball-lightning plasma-glob acts as the hi-Q "frequency hopping" receiver.
Do storms create any coherent VLF e-fields? VLF radios certainly don't
detect such things, so we normally would assume that such signals don't
exist. But hold on! There could be a nearfield effect, where there is no
RF radiation, and where e-fields and b-fields aren't directly connected
together via the impedance of free space. A loop-antenna in a radio
receiver is used with the assumption that incoming EM waves have an E and
an M component, and we should just as easily receive the M component as
receiving the E. (And so a loop antenna would work just as well as a
dipole antenna.) Maybe this is not true of environmental VLF e-fields.
Suppose that a storm (or even the entire Earth) has a very strong vertical
AC electrostatic field. The loop antennas on VLF radios would not detect
it. Horizontal dipoles would not detect it. However, a resonant circuit
connected to a suspended wire (and to ground) certainly would. With a
high-Q resonant circuit, the antenna might even receive significant power.
Call it the "artificial ball-lightning" analogy.
RF TRANSFORMERS: TIGHT COUPLING BETWEEN TWO DISTANT COILSIron-core transformers are examples of tight magnetic coupling, and significant power can be transferred between the coils of a 60Hz transformer. Capacitors are similar: they are examples of tight electrostatic coupling. Resonant circuits give us two new options for tightly-coupled power systems: pairs of high-amperage resonant loop-antennas, and pairs of high-voltage resonant dipole antennas. The spacing of each of these must be below 1/4 wavelength for the phenomenon to appear, and the e- or b-field strength must be very high. Now that I'm speaking of this, I know I've seen such things in common use. Air-core transformers in ham-radio antenna tuners and high-power HF and VHF radio transmitters employ this effect. If both sides of an air-core transformer are tuned to the same frequency, then the b-field surrounding the transformer will build up to a very high level, and the throughput of energy will be very high, even though there's no closed iron-ring magnetic circuit, and coupling between the coils is *apparently* very loose. Note that this sort of thing would limit the transmission bandwidth. Good for low-quality AM radio or for transmitted power, but not for broadband fast data.
MECHANICAL "ENERGY SUCTION"Rick M. points out that mechanical forces might become significant in resonant EM systems. Normal transformers and capacitors certainly do display significant mechanical forces. If a transformer can be made into an induction motor, and if a capacitor can be made into an electrostatic motor, what kind of motor can be built from a loose/tight coupled high-frequency resonant EM device? I have no idea. Perhaps some strange and interesting hobbyist projects are lurking in these particular "undergrowths." Imagine a radio-frequency induction motor built without iron, whose (resonant) stator is at a great distance from the (resonant) rotor, yet the torque between them is still immense. Imagine a high-Q capacitor-based high voltage motor with huge torque, and with all of its parts embedded within plastic (to eliminate the corona problems associated with DC electrostatic motors.) Imagine a carefully-balanced supermagnet that's spinning at 60Hz in a vacuum chamber out in the woods, driven by the feeble environmental 60Hz magnetic field.
ELECTROMAGNETIC PRANKSTERSAn evil though: if we built a resonant antenna within a 1/4-wave distance of an AM radio tower, we might be able to "suck energy" at such a high rate that we could run motors and light lightbulbs! The resonant antenna might be very small, but it would have an intense e-field (or magnetic field if it was a loop antenna), and would reach out and touch the AM tower electrically. I've heard of people using "inductive coupling" to steal 60Hz AC electrical energy. Resonant energy-theft. The addition of a resonant circuit would vastly increase the ability of a pickup coil to suck in energy from any distant conductors as long as the frequency was fairly low. In physicist-speak, "If the world is already full of Sodium light, build some artificial Sodium atoms as absorbers."
Now I guess I need to go make a high-Q tuned circuit and set it to the
same frequency as an AM radio station. Dunk the coil in liquid nitrogen.
Maybe I can light up an LED! I
know that longwire antennas can do this. I also know that an AM
tuned to a weak station, can be affected when an adjacent unpowered AM
radio is tuned to the same station. Untuned inductive pickup coils can
receive "inductively coupled" energy if the b-field in the area is
strong. Instead, with a small coil which resonates at 60Hz, maybe I can
magnetically grab some AC power out of the wiring in my walls? It would
be cool to have a wireless lightbulb connected to nothing but a high-value
60Hz inductor and capacitor. Maybe it would work a bit better if I wrap a
couple of turns of "transmit loop" around my house and drive it with
10KHZ from my stereo. With thick wire and hi-Q resonance, it wouldn't
take much to put
many amperes into such a coil. Rats, now I wish I still lived next to a
big AM transmitting tower like I did when I was a kid.
L.O.S., THE CREATIVITY DRUGIn conclusion, I must answer the obvious question: is Bill Beaty on drugs or WHAT?!!! No, instead I'm on deadline. I'm staying up all night for many nights in a row while beating my head on this interwoven industrial application interrupt-driven cludgy embedded set of C-code background tasks. Lack of sleep is itself a drug. Not LSD, use LOS! College students at exam time are well aware of this phenomenon. Stay up all night for a few too many nights, and you find that philosophy gains entirely new meaning, your wife starts looking at you funny, you are in danger of following Heinlein/Hubbard/Wilson and attempting to start your own religion... and the shades of Tesla and Feynman start subspace-idly coupling some 'Special Ideas' into your throbbing demented neuronal subprocessor networks.
So what do *YOU* do for fun?
Bill b article: Light without photons (NEW 9/99)
REFERENCES: 1. W. Beaty web-article, "Acoustic Black Hole" phenomenon. 2. J. F. Sutton and C. C. Spaniol, "The Black Hole Antenna", PROCEEDINGS OF THE INTERNATIONAL TESLA SYMPOSIUM, 1992, International Tesla Society 3. J. F. Sutton and C. C. Spaniol, "An Active Antenna for ELF Magnetic Fields", PROCEEDINGS OF THE INTERNATIONAL TESLA SYMPOSIUM, 1990, International Tesla Society, 1990 4. C. F. Bohren, "How can a particle absorb more than the light incident on it?", Am J Phys, 51 #4, pp323 Apr 1983 5. H. Paul and R. Fischer "Light Absorption by a dipole", SOV. PHYS. USP., 26(10) Oct. 1983 pp 923-926 6. K. Corum and J. Corum, "Fire Balls, Fractals, and Colorado Springs: A Rediscovery of Tesla's RF Techniques," PROCEEDINGS OF THE INTERNATIONAL TESLA SYMPOSIUM, 1990 Suggested by A. Boswell, regarding small-antenna physics: Chu, J.Appl.Phys. Dec. 1948 Hansen, Proc.IEEE Feb. 1981.