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Relevant Part From Argon Project Wich Togheder With Ego Where Covertly Taken by (nsa in aborted self 69 armagedon project )

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MarianMa...@hotmail.com

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Oct 29, 2006, 4:47:09 AM10/29/06
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http://www.t3rbo.com/photo/view.php?img=9c098e103fcdb26d08379498bb73e22b
http://www.t3rbo.com/photo/view.php?img=f509d22032f710dded5562e33a7c0c88
http://www.t3rbo.com/photo/view.php?img=b11ff9b758eb6dc28fb1fa023ec3bffb
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GAIA

MarianMa...@hotmail.com

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Oct 30, 2006, 4:55:03 AM10/30/06
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MarianMa...@hotmail.com

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Oct 30, 2006, 5:01:58 AM10/30/06
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Booth half zvastica and half earth are visible in clear mode within
repaired
ideal circuit model simulated on an 386 with an student constrained
pspice
version . aka (nsa circuit analog enigma machine )

MarianMa...@hotmail.com

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Oct 30, 2006, 5:37:31 AM10/30/06
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So Argon broke your double secret understandings codes by mistake not
knowing that an circuit and an article is used as an (enigma) machine .
This is when you started to sp around and took the EGO text etc

> >
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GAIA

MarianMa...@hotmail.com

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Nov 1, 2006, 2:38:11 AM11/1/06
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MarianMa...@hotmail.com

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Nov 1, 2006, 2:50:10 AM11/1/06
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The above image is purposedly missleading and is hiding another purpose
made
mistake within the circuit .
The Frequency axe symulation prove the symulation truthfullness .

> http://www.t3rbo.com/photo/view.php?img=7f772074405fdd7c495810f37a01f245
> http://groups.google.com/group/soc.culture.romanian/browse_thread/thread/9acd30df9356e230/2eb5437f9bf837fd?hl=en#2eb5437f9bf837fd


All data aborted inclusiv data encoded in pictures links or any other
mode .
2002 digital version for the original 1993 Scientific American Geting
Chaos In Sincronization
(
http://www.t3rbo.com/photo/img/b01109314014d7d936cf50daa3a0cd2a/1993_08_.GIF
http://www.t3rbo.com/photo/img/ddf674c84b23850f394e255bdd714e15/1993_082.GIF
http://www.t3rbo.com/photo/img/9e78ed43a16e44724d2c0380a123beb6/1993_083.GIF
http://www.t3rbo.com/photo/img/ed740bd0a0fcacd244b390ba23615c6f/1993_084.GIF
)


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MarianMa...@hotmail.com

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Nov 2, 2006, 3:16:33 AM11/2/06
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(RSR UNIREA Diploma) all (nsa sp plans millenium managing odessa planet
new american century etc etc )
http://server6.theimagehosting.com/image.php?img=aa1.19e.JPG
http://img128.imagevenue.com/img.php?image=39755_aa1_122_553lo.JPG

Repairing -(Radio)-(Television) Diploma
http://img155.imagevenue.com/img.php?image=55185_msn_122_405lo.JPG
http://server6.theimagehosting.com/image.php?img=msn.045.JPG


Jewish Comunity Bucharest Romania Coded Names

Mosses Rosen Chief Rabai
Argon Bar Mitsva Teacher Segal

Above circuit has two levels aka one as published in order to misslead
Another hiden level wich was uncovered after finding the purposedly
introduced
mistake repair that mistake and simulate the circuit .
Argon was not supoused to find the real hiden key within the (analog
enigma 2 levels machine ) .

RSR = (Double Roumanian NSACIA)

Since above is 22 this is another proff they atempted to wipe out
during take over all semites .
Again (rf terrorist holocaust ) only an reality hack to distract
atention during take over the planet .

Also this prove they wanted to blame all on semites !
The fact they run away on scr on all went on flames purposedly and trow
all on Argon in hope all
will burne etc togheder with war on so sp called (Fascist) Islam aka an
new mode to be antisemitic
proves that .

Since they repeated the atempt to take Argon out of Israel several
times = absolute shure their pupets (planed revolution)
behind wich was hiden the (black agenda)

*Yaron Dror Words Toward Argon !
You penetrated an unpenetrababal computer you "should'nt have done that
".
= Yaron Dror (nsa) = mossad (nsa) = local (intel colonial trojan horse)
ment (to bring to an end)= till now Israel an (tv) colony!


Argon keeping out from any systems data and hiden all his life since
age 6 including training .
Early knowledge at BrightCom aborted Raul Valenberg (sp Plan) and
Ilan Sharon Yaron Dror Alon Tsafrir they will put Argon in an psy
hospital .

> > > > > > *******************************************************************************************************************

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MarianMa...@hotmail.com

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Nov 21, 2006, 9:21:55 AM11/21/06
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*An Working Police Complain Was Filed In This NonAccident Since More
Photos+ Exist
In this designed place in oposite direction an Army Commando Officer
was killed before .
The place is ("designed ")

In this place the road from Tel Aviv to North have an 90 deg right and
an second 90 deg left turn aka half HORIZONTAL ZVASTICA
In the back there is the Hadera Power Station with the Rabin Iron Cut
Statue

Road was treated + !

An simulatan 3 cars accident was made in the exact time on the oposite
direction .


Just as tribunals preliminary data
http://server6.theimagehosting.com/image.php?img=PIC_0003.37a.jpg
http://www.t3rbo.com/photo/view.php?img=2d9b61f3bc9d5e26ae70f41e1ba7e9c6
http://img9.imagevenue.com/img.php?image=18426_PIC_0003_122_438lo.jpg

Sombody sp make one all issues advertisment trip small accident and
triple accident on the other side
for show etc

Interesting that at SII Hadera works code name Dany of Romanian origin
etc

> > > > > > > *******************************************************************************************************************

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MarianMa...@hotmail.com

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Nov 22, 2006, 3:55:26 AM11/22/06
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garbage...@hotmail.com

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Nov 22, 2006, 4:08:48 AM11/22/06
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> > > > > > > > > *******************************************************************************************************************

nongating is used now due to terrorist ilegal cenzoring and has no
meaning .


Explanations provided to troll AIG insurance company.


> > > > > > > > > *******************************************************************************************************************


GAIA

garbage...@hotmail.com

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Nov 22, 2006, 4:11:54 AM11/22/06
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Ilans Conection to PM Office aka Clear Intel Conection To All Issues
Ilan CV


Ilan Sharon 22 Rambam St., Ra’anana, Israel
Tel: (972-9)-7417315 Mobile: (972-52)-558660
Date of birth: 06.12.70
Email: Cros...@bezeqint.net

Profile:
• R&D Hardware and System Integration Engineer
• Extensive experience in communication systems projects, design and
development
• Experienced in multi-disciplinary development environments
• Good interaction with other team members


Education:
1996 – 2000: B.Sc. in Electrical engineering, Tel-Aviv University.
Major subjects: communication, computers, DSP, bioelectronics.
1988 – 1989: Electronic Technician, “Lady Davis” College
(Military oriented).
1985 – 1988: Full Graduation Diploma, “Lady Davis” High School,
Tel-Aviv. Major subject: Electronics.


Professional Experience:
BrightCom Technologies Ltd. 2000 – 2003

BrightCom is a startup designing and manufacturing Bluetooth Chips
System Integration Engineer
• Leading new projects originating from initial idea, through project
definition, execution and solving the engineering problems until
completion, while integrating several domains:
 Board design using digital, analog and RF components, including
layout and manufacturing in collaboration with sub-contractors.
 Participation in the architectural design of 2 ASIC platforms.
 Design of wide-ranging system architecture that includes various
interface such as Ethernet, USB, RS232, Centronix, audio.
 Defining hardware and software requirements per project, each
optimized for the relevant niche (power, working frequency, size,
cost).
 Design of diverse modes of operation for different applications,
debugging and developing tools for link quality improvement.
• ASIC emulation on large Xilinx FPGA platforms (XCV1600E), using
various software tools:
 Floor Planning – emphasis on speed/size/structure for getting the
required results.
 Verilog designing and modifying existing code for the FPGA
platform.
• RF modules characterizing. Defining feasible modes of operation,
hardware interface and software drivers.
• Performed joint projects and application integrations with
strategic partners in Europe and USA.
• Performed inter-operability and FCC tests.


Israeli Prime Minister’s Office, 1993-2000
Computing & Communication Department

Working in the R&D section within the Computing & Communication
Department (WAN oriented)
WAN and LAN development and maintenance team
• Designed WAN block level architecture while supporting protocols
such as TDM and X25.
• Operated wireless and satellite communication systems.
• Developed immediate and short-term end user applications.
• Problem solving and support in Israel and abroad.
• Supported 4W and fiber optic, Novell based, local area networks.

Desk Electronics Ltd. 1992-1993

Desk Electronics develops, manufactures and sells multi-disciplinary
tracking and alarm systems that include: micro-controllers, RF, sensory
and telephony modules.
Electronics Technician
• Performed acceptance tests after manufacture.
• Responsible for maintenance of multi-disciplinary systems.

Knowledge of Software Programs:
Orcad Capture, Xilinx ISE, Synplicity Amplify and Synplify Pro, FPGA
Express, Matlab.

Army Service:
1989 – 2001: Full 3 years service in IDF Intelligence Corps as a
technician in the development section.

Languages:
Hebrew – mother tongue, English – fluent


> > > > > > > > > > *******************************************************************************************************************


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MarianMa...@hotmail.com

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Nov 22, 2006, 8:31:06 AM11/22/06
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http://groups.google.com/group/internalterrorism/browse_frm/thread/c654dd140037909c/?hl=en#
AIG has no value was simply the lowest cost for standard car insurance
on the market .
If now that was purposedly was made as such for painting reasons that
issue need to be checked .
Especialy in conection to Aliza see Olmert coded Wife Name and made to
look like Ziva Patir and
Ramat Aviv horizontal half zvastica after exiting Aialon North
highway an 90 degrees left turn around the Ramat Aviv intel facility
and then another 90 degrees right turn on Haim Lebanon SII MATI Street
and accidentaly in the rear an purposedly total stop in
an car free road without a reason Vadim from SII when Argon worked at
SII .
Another fabricated accident and lies .

Intel sp .

Hiden Codes Included In Ilan Sharon CV are all null and aborted .
We will speak in tribunals about all related issues .

MarianMa...@hotmail.com

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Dec 5, 2006, 3:41:14 AM12/5/06
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This is the same encoded value as the half earth encoded in the
decripted (analog enigma machine )
and after decription that is by any mode an Tribunal level aditional
proof .
http://groups.google.com/group/soc.culture.romanian/search?q=codes&start=0&scoring=d&hl=en&
http://groups.google.com/group/soc.culture.romanian/search?hl=en&group=soc.culture.romanian&q=codes+1977+&qt_g=1
http://groups.google.com/group/soc.culture.israel/browse_thread/thread/ca662020ed0d169/ce52ca62658e649e?lnk=gst&q=codes+1977+vrancea&rnum=1&hl=en#ce52ca62658e649e
http://groups.google.com/group/soc.culture.romanian/browse_thread/thread/e3f258d347334dbd/357019e1b3d89f31?lnk=gst&q=codes+1977+vrancea&rnum=2&hl=en#357019e1b3d89f31
http://groups.google.com/group/soc.culture.romanian/browse_thread/thread/639d7bbbe4520617/ef9485bb68bd5b19?lnk=gst&q=codes+1977+vrancea&rnum=3&hl=en#ef9485bb68bd5b19
http://groups.google.com/group/soc.culture.israel/browse_thread/thread/ca662020ed0d169/ce52ca62658e649e?lnk=gst&q=codes+1947+1977&rnum=1&hl=en#ce52ca62658e649e
http://groups.google.com/group/soc.culture.romanian/browse_thread/thread/639d7bbbe4520617/ef9485bb68bd5b19?lnk=gst&q=codes+1947+1977&rnum=2&hl=en#ef9485bb68bd5b19
All data only for read and Tribunals


This is the entire(odessa 60 years plan culminating in 1977 2007)
period.
(PERIOD DOUBLING AND CHAOTIC BEHAVIOR IN A DRIVEN ANHARMONIC
OSCILLATOR. Paul A. Linsay in Physical Review Letters, Vol. 47, No. 19,
pages 1349-1352; November 9,1981.)

http://server6.theimagehosting.com/image.php?img=1992_01_.GIF
http://server6.theimagehosting.com/image.php?img=1992_012.GIF
http://server6.theimagehosting.com/image.php?img=1992_013.GIF


Cost: $0-100
About These Ratings Difficulty: Danger 1: (No Hazards) Utility:

------------------------

How to Generate Chaos At Home


---------------------

by Douglas Smith
January, 1992

---------------------


MOST PEOPLE TRY TO AVOID chaos. After all, who wants to be stuck in an
airport on a snowy afternoon before Christmas? But I find chaos
relaxing, particularly when I can observe and control it. Chaos is part
of the beauty of nature. It can be observed in the flow of a river, the
swing of a pendulum or the dynamics of a cloud [see "Quantum Chaos," by
Martin C. Gutzwiller, page 78].


Figure 1: A circuit that produces chaos
One of the best ways to experiment with chaos is to build an electronic
circuit such as the one depicted in the diagram below. The circuit
serves as a paradigm for chaotic systems. When the circuit is subjected
to certain voltages, it produces a signal that is chaotic.

In 1981 Paul S. Linsay of the Massachusetts Institute of Technology was
the first to study rigorously the circuit's behavior. Since then, many
physicists have attempted to explain how the circuit generates chaos.

When I learned about Linsay's experiments, I was struck by the fact
that a simple circuit could produce such complicated and interesting
behavior. I had seen computer simulations of chaotic systems, but here
was a chance to study the chaotic dynamics of nature firsthand. As an
amateur scientist, I decided I wanted to see chaos for myself. And with
a little bit of effort, I even found a way to listen to it.

To construct the circuit, all you need is some basic electronic
components: a resistor, an inductor and a diode. I recommend that you
start with a resistor of 200 ohms and an inductor of 100 millionths of
a henry, the unit of inductance. I have found that many different
diodes will work, including lN4001,lN4004,lN4005 and lN4007.

You can buy a handful of resistors, inductors and diodes for less than
$20. I purchased the components from a mail-order company. You can also
try a hobby store that carries electronics. The circuit can be
assembled on a breadboard, which is a plastic block with rows of holes
to accommodate components. The board costs about $10. To supply the
input signal, you will need a function generator, which can be bought
for around $200. To measure and view the output of the circuit, you are
best off using an oscilloscope. If you do not own an oscilloscope and a
function generator, you can probably arrange to use them at a
department of physics or engineering at a local college.

I wanted to have a scope of my own so that I could perform experiments
at home, but I could not afford to pay the $1,000 for a new one. Hoping
to buy a used scope, I posted a notice on a bulletin board at Argonne
National Laboratory. A week later I was contacted by someone who
repairs fire alarms and happened to have an oscilloscope for sale. He
invited me to his workshop to take a look. The room was filled with
electronic parts: dismantled computers, old antennas, disassembled
radios, stacks of power supplies. I knew I was in the right place. He
sold me a 15 year-old oscilloscope for $100.

Once you have obtained all the equipment, it will not take long to
assemble the circuit. The components are connected in series: first the
function generator, then the resistor, then the inductor and finally
the diode.

You might be aware that the orientation of a diode is an important
consideration when building a circuit. A diode has two terminals, known
as the cathode and the anode. The cathode terminal is almost always
marked by a band on the diode. Ideally, a diode allows current to flow
only from cathode to the anode and not the other way.

When you build the chaos circuit for the first time, I recommend that
you connect the cathode terminal to the inductor and the anode to
ground. But if you do insert the diode the other way, you will find
that it makes very little difference.

To monitor the output of the circuit, clip an oscilloscope probe
between the resistor and the inductor. If your scope has a second
probe, use it to measure the input. Check all connections and make sure
that all components are firmly seated in the breadboard.


Figure 2: Response of chaos circuit
You are now ready to explore chaos. Set the function generator so that
it produces sine waves whose frequency is about two million cycles per
second (hertz) and whose amplitude varies from 0.1 to - 0.1 volt. The
output signal should have a lower amplitude than the input but the same
frequency. Slowly increase the amplitude of the input signal. At a
certain amplitude between one and two volts, the circuit will suddenly
produce an output signal with peaks of two different heights. The
signal actually consists of two components, each having a different
frequency. The point at which new components are introduced is known as
a bifurcation.

As you continue to increase the amplitude by small discrete amounts,
the signal bifurcates again and again. If you record the amplitude at
which each bifurcation occurs, you will notice that change in amplitude
between bifurcations decreases geometrically. At a certain amplitude,
the system will have bifurcated an infinite number of times, thereby
achieving chaos. The signal is not random but a complicated mixture of
components.

By increasing the amplitude beyond the onset of chaos, you should be
able to produce an output signal with three or even five frequency
components This effect is typical of chaotic systems.

If your circuit is not generating chaos, tune the function generator to
a different frequency and try again. If you still don't see it and if
you are sure everything else is working properly, you should try a
different kind of diode. I have learned that the diodes that work best
are ones that have a high capacitance. You can find out the capacitance
of the diode by calling the manufacturer or by obtaining a copy of the
diode's "data sheet."

You might also find it difficult to experiment at frequencies of a few
million hertz because of the limitations of your function generator or
oscilloscope. By changing the basic components, you can work at lower
frequencies. If you use a 1N2858 diode, a resistor of 25 ohms and an
inductor of 0.1 henry, you can drive the circuit into chaos around
75,000 hertz. You may be forced to order the 0.1-henry inductor from a
catalogue since they are rarely used by hobbyists.

The source of the chaotic behavior in the circuit is the diode.
Ideally, a diode would conduct current in only one direction. Current
will flow through the diode only if the voltage at the cathode is lower
than that at the anode. In the circuit the anode is connected to ground
(zero volts); therefore, if the cathode has a negative voltage with
respect to ground, the diode will conduct.

Real diodes differ from the ideal. If the voltage at the cathode is
positive, the diode acts somewhat like a capacitor, that is, the
voltage across the capacitor is proportional to the rate of change of
the current. It will continue to act in this manner until the voltage
at the cathode reaches about -0.5 volt. Then it will freely conduct
current, but it will still resist the flow somewhat, maintaining the
voltage at about -0.5 volt. If the voltage at the cathode then drops
below zero volts, it does not shut off immediately. For a short time,
the diode allows the current to flow and then acts like a capacitor
again.


Figure 3: DIODE CONDUCTS CURRENT when the voltage at the cathode is
lower than that at the anode. The graph shows the response of a typical
diode.
Circuits that require diodes are usually designed so that the non-ideal
properties of the diode are suppressed. But our experimental circuit
brings out the full character of the diode.

First consider what happens if the input of the circuit is a sine wave
whose amplitude varies from 0.1 to -0.1 volt. Under these conditions,
the voltage at the cathode does not go below-0.5 volt, and therefore
the diode behaves like a capacitor. In this case, the behavior of the
circuit is predictable. When the input is set to a low-frequency sine
wave, the capacitor and the inductor will act like a large resistor,
preventing current from flowing through them. The amplitude of the
input wave will thus equal that of the output wave.

As the frequency of the input is increased to some critical value, the
inductor and diode will provide little resistance, thereby allowing
current to flow through them to ground. The output voltage will then
approach zero. As the frequency is increased or decreased from the
critical value, the amplitude of the output increases until it equals
that of the input.

The critical frequency depends on the capacitance of the diode and the
inductance of the circuit. It equals

where the inductance is measured in henries and the capacitance is
given in farads. If the inductance is 100 millionths of a henry and the
capacitance is 50 trillionths of a farad, then the critical frequency
equals about 2.3 million hertz.

Now if the amplitude varies from + 2 to - 2 volts, the diode may be
behaving in one of two ways. It may allow current through. Or it may
behave like a capacitor. Which behavior it chooses now depends on the
voltage at its cathode and how long that voltage has been applied. In
turn, the applied voltage at the cathode is related to how the inductor
reacts to the input voltage. Then again, how the inductor reacts also
depends on whether the diode is charging up like a capacitor or is
holding at -0.5 volt.

In simple terms, the inductor is receiving one set of instructions from
the input signal and another set from the diode. If the sequence and
timing of the instructions are just right, the circuit may continue to
produce a periodic signal. But if the natural rhythm of the
instructions is broken, the circuit produces chaos. During the past
decade, Roger W. Rollins and Earle R. Hunt of Ohio University have been
working on a computer simulation that describes the behavior of the
circuit exactly.

After you get a good grasp of how the components work, I encourage you
to experiment with the circuit. For instance, you can insert different
diodes and observe how the chaotic behavior changes. Or you might try
changing the frequency, shape or DC offset of the input signal.

You might also find it interesting to visualize the output signal in a
different way. You can plot the input signal versus the output by using
the oscilloscope in the x-y mode. (One oscilloscope probe should
monitor the input; the other should record the output.) You should see
one or more loops on the screen of the scope. In this mode the number
of loops increases as the number of frequency components rises.

For those readers who like dramatic demonstrations and who do not have
an oscilloscope at hand, I recommend a different sort of experiment. It
is possible to listen to chaos by hooking the circuit up to your stereo
system. Before you do so, you should think about whether the input to
your receiver can handle the output of the circuit. You don't want to
blast too much current or voltage into the receiver.

You should first confirm that your function generator is producing the
voltages that you desire. If the input voltage to the circuit is five
volts and the resistor is 200 ohms, the maximum current should be 25
milliamps. (The current equals voltage divided by resistance.) By
consulting the owner's manual to your stereo, you should be able to
discover whether the input channels can handle five volts and 25
milliamps. If not, you can increase the resistance of the circuit.

To connect the circuit to the stereo, use a patch cord. If you cut off
an end of the cord and strip it, you will see a wire and either a
metallic shielding or a second wire. Connect the first wire to the
output of the circuit. Then attach a wire from the shielding to the
ground of the circuit, or connect the second wire to ground. Make sure
the stereo is turned off and then insert the plug into an input channel
of the stereo.

First, set the function generator to sine waves of one volt at about
1,000 hertz. Turn the volume to a low setting and then switch on the
stereo. You should hear a tone about two octaves above middle C. As you
increase the frequency, the tone should rise in pitch But when you
reach about 20,000 hertz, the tone will be out of your hearing range.
Next turn the frequency up to two million hertz. You should not hear a
tone.

To drive the circuit into chaos, increase the amplitude of the input
slowly. Do not turn up the voltage beyond five volts unless your stereo
can handle more than 25 milliamps. As the amplitude increases, the
circuit will produce a signal with two frequency components, then four,
then eight and so on. You should still hear no sound. When the
amplitude increases beyond the onset of chaos, however, the stereo
should hiss loudly. When the circuit behaves chaotically, it generates
a wide range of frequency components, including some that you can hear.

You can now explore chaos with your ears. In general, the greater the
amplitude of the input signal, the more frequency components you will
hear. At certain amplitudes, however, the circuit will generate a
signal with only three or five frequency components, and the noise will
stop.

I do not think the chaotic circuit has much of a future as a musical
instrument. But who knows? Composers have written symphonies using
electronic synthesizers. Why not a concerto for chaotic circuit in C
major?

Bibliography

PERIOD DOUBLING AND CHAOTIC BEHAVIOR IN A DRIVEN ANHARMONIC OSCILLATOR.
Paul A. Linsay in Physical Review Letters, Vol. 47, No. 19, pages
1349-1352; November 9,1981.

CHAOS: MAKING A NEW SCIENCE. James Gleick. Viking Penguin, 1987.

THE ART OF ELECTRONICS. Paul Horowitz and Winfield Hill. Cambridge
University Press, 1989.

Suppliers and Organizations

The Society for Amateur Scientists (SAS) is a nonprofit research and
educational organization dedicated to helping people enrich their lives
by following their passion to take part in scientific adventures of all
kinds.

The Society for Amateur Scientists
5600 Post Road, #114-341
East Greenwich, RI 02818
Phone: 1-401-823-7800

Internet: http://www.sas.org/

*******************************************************************************************************************


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garbage...@hotmail.com

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Dec 5, 2006, 6:21:00 AM12/5/06
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Since the storm is out and Gates are allready open :
Argon Project Felix Kaushansky Partner Was Military Police !
http://groups.google.com/group/soc.culture.israel/browse_frm/thread/6c1366c8d1edfb00/b34d3d4c9e5643e5?lnk=gst&q=felix&rnum=1&hl=en#b34d3d4c9e5643e5


> *******************************************************************************************************************

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garbage...@hotmail.com

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Dec 5, 2006, 6:28:43 AM12/5/06
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http://groups.google.com/group/soc.culture.israel/browse_frm/thread/6c1366c8d1edfb00/b34d3d4c9e5643e5?lnk=gst&q=felix&rnum=1&hl=en#b34d3d4c9e5643e5

According to (odessa nsacia codes ) the following conclusions can be
reached :
Felix is encoded as following :
Millitary Police
R_US_SIA_N
UK_R_AIN_IAN
See Ha Shavua Be Ashdod Allready Published
He & His Girl Friend got Mela_got
Argon & His Exit Not

Thouse :
Ilan Sharon again (nsacia)

> > *******************************************************************************************************************


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Dec 5, 2006, 6:32:48 AM12/5/06
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Pictures will be reposted .
http://groups.google.com/group/soc.culture.romanian/browse_frm/thread/acf87ada5d76c8a7/2fc81f460175dbb4?lnk=gst&q=ashdod+student&rnum=2&hl=en#2fc81f460175dbb4

> > > *******************************************************************************************************************


GAIA

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Cost: $0-100
About These Ratings Difficulty: Danger 2: (Minor injury possible)
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------------------------

Circuits That Get Chaos in Sync


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by Joseph Neff and Thomas L. Carroll
August, 1993

---------------------


CHAOS IS NOT ALWAYS SO chaotic. In some sense, it can be predictable:
two systems can be designed so that one exhibits exactly the same
chaotic behavior as the other. In other words, the systems would be
synchronized. Such devices might be useful for encrypted
communications. For example, one of the systems could conceal a message
within the chaotic signal. Only someone who possesses the second system
would be able to decode the transmission, by subtracting the chaotic
signal and leaving behind the message [see "Mastering Chaos," by
William L. Ditto and Louis M. Pecora, page 78].


Figure 1: CHAOTIC CIRCUITS produce the same output. They draw current
from a 12-volt power supply and are probed by an oscilloscope (left).
The values for the components used should match those shown in the
schematics (right) to within about 1 percent.
Louis M. Pecora of the U.S. Naval Research Laboratory first came up
with the idea of synchronized chaotic systems. He and one of us
(Carroll) used a computer simulation to show that such a phenomenon can
exist. The next step was to demonstrate the idea using physical
systems-specifically, electrical circuits, which are accessible and
inexpensive. The first circuit that Carroll built to display
synchronized chaos was based on a design devised by Robert Newcomb of
the University of Maryland.

Although the circuits described here are simplified versions of
Newcomb's, experience with circuit assembly might be helpful. A good
introduction to chaos in electrical circuits, using only a diode, an
inductor and a resistor, appeared in this column last year [see "How to
Generate Chaos at Home," conducted by Douglas Smith; SCIENTIFIC
AMERICAN, January 1992].

Basically, the setup will consist of two circuits: a driving circuit
and a synchronized circuit [see illustration below]. The two are
identical except for an important component missing in the synchronized
circuit. The two circuits are connected at a single point. The chaotic
output of the synchronized circuit will match that generated by the
driving circuit if both circuits are correctly built.

Before buying the electronics parts and constructing the two circuits,
make sure you have an oscilloscope, breadboards and a power supply that
can deliver 12 to 15 volts of direct current. (Breadboards are thin
sheets of plastic that have holes to accommodate electronic components;
purchase ones that will hold the positive, negative and ground
terminals from the power supply.) The power supply and breadboards are
cheap and easy to come by. Oscilloscopes, unfortunately, are expensive;
they start at about $500. You can sometimes buy a cheap, used
oscilloscope at a "hamfest"-a flea market for ham radio enthusiasts. If
you do not wish to purchase an oscilloscope, you might be able to get
access to one at a local college laboratory. The device should provide
two channels and be able to plot the input to the channels against each
other.

For the circuits themselves, you will need various resistors,
capacitors and integrated chips called operational amplifiers
(op-amps). A list of such items and the minimum quantity you need
appears below. We recommend buying more than the minimum, because it is
easy to make connection errors that can burn out the components,
especially the op-amps.


Figure 2: OSCILLOSCOPE PATTERNS typically found in working synchronized
circuits are shown above. The chaotic output from one circuit is
revealed by a plot of output voltage over time (a); several sweeps are
shown. Plotting the output from A2 against that from A3 yields a
chaotic attractor (b). Comparing the output of both circuits at Xs
shows the circuits are prefectly synchronized (c) or partially so (d).
Because the two circuits must be as similar as possible, it is
essential to use resistors and capacitors that have high tolerances.
Look for resistors rated to be accurate within 1 percent and capacitors
made from polypropylene, which do not leak much current. All but two of
the op-amps are generic type 741. The exceptions, labeled "A4" on the
schematic [see right illustration in Figure 1], are so-called
high-frequency uncompensated op-amps. The particular ones used here
were type NE5539N. These two are the most critical components of the
circuits, as they are ultimately responsible for keeping the circuits
synchronized.

The components we used were purchased from Digi-Key Corporation in
Thief River Falls, Minn. The total price was less than $30. When
ordering, remember to ask for the pin diagrams for the op-amps, which
contain several connections that all look alike. The specification
sheet describes the configuration of the pins so that you will know
which ones to use.

To decrease the possibility of wiring error, it is best to lay out the
circuits according to the schematics before connecting them. Start with
the op-amps, using one breadboard for each circuit Observe that the
synchronizing circuit is identical to the driving circuit, minus an
op-amp and its ancillary components.

The next step is to make the power connections (be sure the power
supply is unplugged before beginning). Only the op-amps draw current.
Attach wires from the positive, negative and ground terminals to
separate rows that run along the top and bottom of the breadboard.
These rows are dedicated solely to providing voltage to the electronic
components. Use the op-amp spec sheet to determine the appropriate
connections from the pins to the rows. The ground wires should be as
short as possible because long ground connections can pick up noise,
which would keep the circuits from synchronizing.

After hooking up the power supply, begin connecting the components
systematically. Although the schematics are simple, it is easy to
create a mess. Short, color-coded wires make the circuit convenient to
read and check over. Take several different visual walks through the
circuits to verify that all of the connections are correct. Writing
down the color codes of the resistors next to their values on the
schematic may speed up this process.

Once you are satisfied that your circuits are correct, connect the
synchronizing circuit to the driving circuit at the points marked "Xl"
on the schematic. Notice that as a result of the connection, the two
circuits have the same nonlinear driving component (the subsystem that
uses the A2 op-amp). Connect each channel of the oscilloscope to the
points marked "Xs" on the schematic. Each such point is located just
after the A1 op-amp. Make sure that the circuits and the oscilloscope
all have the same ground-that is, the grounding wire attached to the
oscilloscope's probes should be hooked up to the same ground line as
the circuit Check the circuits several times before plugging in the
power. If you burn out one of the op-amps, you can plan to spend at
least a few minutes trying to figure out which component is broken and
replacing it.


Figure 3: Component shopping list
You can verify that the circuits are producing chaos by displaying
information from one channel only. If that circuit's output is chaotic,
the oscilloscope image will not remain stable on any setting. Instead
it produces a pattern similar to a sine wave that rapidly changes in
amplitude.

A detailed explanation of why chaos arrives in the driving circuit is
rather complex. Briefly, the two integrating op-amp components (the
op-amps that have capacitors, labeled "A2" and "A3") are connected in a
loop to generate a sine wave. The op-amp components A4 and A5 amplify
this sine wave, causing its amplitude to increase exponentially over
time. Once the signal reaches a certain amplitude, the high-frequency
op-amp (A1) brings the amplitude to zero and starts the process all
over again. Chaos creeps in during the switching, when A1 resets the
circuit.

You can see if your circuits are producing synchronized chaos by
plotting the output of one circuit at Xs with that of the other. If the
circuits are perfectly synchronized, the oscilloscope will produce a
straight line angled at 45 degrees. Because of the switching, the
synchronization will probably not be exact. Two broadened, parallel
lines may be the result instead.

Do not be disappointed if the circuits fail to synchronize on the first
try. Check for faulty connections. The circuits are rather fussy, so
any poorly made connections could wreck the synchronicity. A faulty
op-amp could be the culprit. You might find that both circuits generate
chaos but are not synchronized. There are two possible explanations.
One, components that are supposed to be nearly the same may differ too
much; for example, two resistors designated as 1,000 ohms may turn out
to be 950 and 1,050 ohms. Two, the response time of the high-frequency
op-amps may be insufficient, in which case the op-amps should be
replaced.

Once the synchronizing chaotic circuits are working properly, you can
create the form of message encryption envisioned by Pecora and Carroll.
You will need two more op-amps and several large (high-impedance)
resistors. With these components, you can easily build two
"summing-amplifier" circuits Such circuits add two signals together and
then invert them. These two circuits are connected to the driving and
synchronizing circuits [see illustration below]. The message we encoded
was a simple sine wave created by a function generator. The sine wave
is fed to one of the summing-amplifier circuits, which combines the
sine wave with the chaos generated by the driving circuit and inverts
the total signal. Amid the chaos, the sine wave is almost impossible to
decipher.


Figure 4: SUMMING-AMPLIFIER CIRCUIT (top) marries an input signal with
a chaotic signal and then inverts the combination. Two such circuits,
when connected to the synchronized chaotic circuits, produce a form of
encrypted communication (bottom).
The synchronizing circuit, however, can readily extract the message
from the chaos. Because the synchronizing circuit produces the same
chaotic pattern as the driving circuit, all one has to do is add the
synchronizing circuit's chaotic signal to the driving circuit's total
(inverted) signal. What is left is the message. The second
summing-amplifier circuit does this job and reinverts the sine wave to
its original form.

The summing-amplifier circuits may cause the entire system to behave
quite erratically; the image on the oscilloscope may blow up. The
problem is that the external devices drain some current and thereby
jolt the circuits from one so-called chaotic attractor-a pattern around
which the chaotic signals tend to settle-to another.

Large resistors help to alleviate the problem by preventing current
drain. We used resistors of 60 kilo-ohms and one mega-ohm, although 50
kilo-ohms will probably do. Another way to get the circuit back to a
single attractor is to short out an op-amp periodically. Briefly touch
a grounded wire to the output of one of the op-amps (preferably the
ones with capacitors). This process randomly resets the state of the
circuit. The op-amps will not be damaged so long as the shorting is
brief. Turning the power supply off and then on again will also work.

To hear the message, you will need to amplify the output. Op-amps do
not deliver much current (and the high-impedance resistors do not help
matters). A stereo system is a nice solution. Alternatively, a basic
electronics handbook will detail how to build simple amplifying
circuits to drive a small speaker.

You might try to encode signals more complex than sine waves. You can
send audible messages by using a microphone, which converts sound waves
into concealable electrical signals. Or you can try sending Morse code:
each "click" sends a constant voltage signal. On the other end, you can
wire up a small light bulb or a light-emitting diode (known as an LED),
which should z flash in unison with the clicks if the circuits are
working properly.

You can also demonstrate the effects of attractors in chaos by plotting
the output of one of the integrating op-amps versus its neighboring
op-amp. Such an input produces a spectacular pulsating spiral pattern
and is evidence for a single attractor. Feel free to change some of the
components to see what happens. Remember, you are trying to create
chaos.

Bibliography

NONLINEAR CIRCUITS HANDBOOK. Analog Devices Engineering Staff. Analog
Devices, Norwood, Mass., 1976.

DYNAMICS: THE GEOMETRY OF BEHAVIOR, Parts 1-4. Ralph H. Abraham and
Christopher D. Shaw. Aerial Press, 1985.

INTRODUCTORY ELECTRONICS. Robert E. Simpson. Allyn and Bacon, 1987.

THE ART OF ELECTRONICS. Paul Horowitz and Winfield Hill. Cambridge

University Press, 1991.


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