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I've been very interested in electrical engineering and radio
recently. I've been trying to learn how radio waves tie into
electrical engineering. How do we create them? How do we receive them?
the matter, but still do not know exactly how they "work".

For example, a very simple 1 MHz AM transmitter is described here:

I am referring to the image here:

I understand that the top left pin of the crystal oscillator is the
input for some voltage. So assuming that I provide a steady +5 volts
on that pin, what will I see on the output pin (top right)? Will I see
a 1 MHz wave with a peak voltage of +5 volts? Or will it have an RMS
voltage of 5 volts?

How is the radio wave generated in this case? If I stick an
appropriately sized antenna on the output pin, how is the radio wave
generated? Why is it generated? Is it because of the oscillating
potential difference across the output pin and ground?

What governs the output power of the radio wave? How do we generate a
more "powerful" signal? Assuming the photon theory of electromagnetic
radiation (if that is the correct theory to use here), does the output
power refer to the number of photons emitted/time? If so, how do we
increase the power? And why are the photons emitted in the first
place?

On the receiving end, assuming a properly sized antenna, how is the
happens? If I were to have a long, straight piece of wire and clip two
terminals of a sensitive oscilloscope to each end of that wire, will I
be able to see the wave (assuming a powerful enough transmitter)? If
not, why not?

I know bits and pieces of things but I'm still not able to see the big
picture here. I can only understand this stuff if I know the
fundamentals on a very low level.

I'm really trying to learn this stuff, and I have searched in several
books and on the Internet, but it is proving to be a difficult task to
find this information. I know you guys are the best people to ask. So
here I am.
solarwind wrote:
> I am referring to the image here:

Ick. If that TTL oscillator survives having +9V across it, I'll be VERY
surprised...

> I understand that the top left pin of the crystal oscillator is the
> input for some voltage. So assuming that I provide a steady +5 volts
> on that pin, what will I see on the output pin (top right)? Will I see
> a 1 MHz wave with a peak voltage of +5 volts? Or will it have an RMS
> voltage of 5 volts?

A square wave with peaks of 5V and 0V.

Hardly ideal for radio -- it'll work, but you'll get odd harmonics going
right the way up into the GHz range (depending on the oscillator in
question). What you ideally want is a sine wave -- a pure tone --

The circuit as presented is going to use the transformer to vary the
voltage seen by the TTL osc., essentially making a crude AM modulator.
Emphasis on the word "crude". There's a single-transistor AM TX in one
of the Forrest Mims books -- it isn't perfect, but at least it generates
something reasonably close to a sine wave.

> What governs the output power of the radio wave?

AIUI, the "resistance" (more accurately, impedance) of the antenna is
fixed (matched/tuned) to around 50 Ohms. Put more voltage in, get more
power out.

> I'm really trying to learn this stuff, and I have searched in several
> books and on the Internet, but it is proving to be a difficult task to
> find this information.

Join the club...

You might get some benefit out of joining a local amateur radio society
and doing one of the many ham radio courses. In the UK you have three
licence classes:
- Foundation
- Intermediate

Essentially, Foundation teaches you enough to be able to switch on a ham
radio transceiver and use it properly, and some of the theory.
Intermediate expands on this by teaching more of the theory, and covers
some information that's likely to be of use if you're building TX/RX
gear from scratch (i.e. not from a kit). Advanced then expands this
further by teaching some microwave and UHF transmission theory (IIRC).

You might want to look up your country's equivalent of this. If you're
Most of them are more than willing to help explain the theory and

--
Phil.
piclistphilpem.me.uk
http://www.philpem.me.uk/
very simple terms. Most any North American library system should have
numerous copies available ... not terribly expensive to buy though.

RiB

On Wed, Mar 31, 2010 at 13:27, solarwind <x.solarwind.xgmail.com> wrote:

{Quote hidden}

> -
> I have searched in several
books and on the Internet, but it is proving to be a difficult task to
find this information.

Rushing, so
Magic words include

ARRL
RSGB

They do many books and no doubt have much on web..

R
That;s a pretty bad example of an AM "transmitter" and I'll leave that
side of things alone.

If you really want to find out how it all works, it comes down to
Maxwells equations - see wikipedia
<http://en.wikipedia.org/wiki/Maxwells_equations> although it's pretty
heavy going.

Personally I understand it no more now than I did in engineering class in 1976!

Essentially the antenna and ground plane behave like a resistive load
for the correct combination of physical dimensions and frequency. The
power that would be dissipated in the equiv. resistor is radiated
instead (mostly anyway, all going well). The exact situation that
causes the radiation is the complicated part above.

I have my own way of trying to understand how this happens but I won;t
try & explain it  here because it's almost certainly wrong and is
likely to cause more confusion than enlightenment!

Hope this somehow assists.

RP

On 31 March 2010 18:27, solarwind <x.solarwind.xgmail.com> wrote:
{Quote hidden}

> -
solarwind wrote:
> I've been very interested in electrical engineering and radio
> recently. I've been trying to learn how radio waves tie into
> electrical engineering.

They don't.  Radio works on magic.  That's why there are people that
specialize in RF (Radio Frequency).  You usually see them wearing long
robes, tall pointy hats, and carrying stick like things in their hands.

Seriously though.  These are good questions but to answer them properly is
way beyond the scope and size of a PIClist post, and the time anyone can
probably devote to writing one.  Back when I was in high school, I found the
ARRL Handbook a good source for looking up things RF.  I sortof remember it
don't know if it's still around, but if not, try to find a old copy.  It
used to be the size of a medium phone book.  Maybe nowadays its on line.  Go
to your local library and see if you can find one, then maybe get pointers
from there.

I just entered "ARRL Handbook" into Google, and it's alive and well and can
be had for \$50.  There are probably chunks of it on line somewhere.  Follow
the cookie crumbs and you'll probably find some good information, or for \$50
you can have it all for sure.

> How do we create them? How do we receive them?
> the matter, but still do not know exactly how they "work".

Very briefly.  Voltages do not end at the ends of conductors.  A voltage
field, called the E field permeates all space.  If you have two pieces of
aluminum foil 1 meter apart and connect a 12V battery between them, the E
field between will have a strength of 12V/meter.  Yes, it's really that
simple.

The not so simple part comes from when these voltages start changing.  If
you were a few meters away and could sense what's left of the E field at
that distance you would see it change a very short time after the voltage on
the plates changed.  That's because the E field propagates at the speed of
light.  So when you switch on the two plates, you've created a disturbance
in the E field that radiates out from your location at the speed of light.
This effect drops off in magnitude quickly to the point where we can't
measure it anymore, but it actually radiates out inifinitely and forever.  A
year after you did this and your aluminum foil pieces are long gone, the
electric disturbance you created is still propagating outward at the surface
of a sphere a light year in radius.  A little bit of the energy from the 12V
battery has essentially been transmitted into space.

This thought experiment is only to show that any electric change not only
happens in wires, but little bits of its energy leave and propagate away.
Only a very very tiny fraction of the energy in the aluminum foil example
was transmitted.  However, once you know this can happen you can get clever
and design systems to do this deliberately, you can get a good fraction of
the energy or your circuit to radiate.  That's exactly what a RF transmitter
connected to a antenna is.

To do this efficiently, we usually try to get the system to resonate at the
transmitting frequency.  Resonance is a whole other topic I don't have time
for, but is usually important in RF transmitting and receiving systems.
Again, very briefly, simple resonance requires the electric conductors to be
around 1/2 wavelength in size, or multiples of 1/2 wavelength.  At that
size, the propagation delay from one end to the other is such that the wave
sloshes back and forth.  That makes bigger voltages more easily, which makes
bigger E fields, which means the E field disturbance can be detected at
greater distance.  Radio is the art of getting all this right.

I gotta go now.  Maybe more later.

********************************************************************
Embed Inc, Littleton Massachusetts, http://www.embedinc.com/products
(978) 742-9014.  Gold level PIC consultants since 2000.
> I just entered "ARRL Handbook" into Google, and it's alive and well and
> can
> be had for \$50.  There are probably chunks of it on line somewhere.
> Follow
> the cookie crumbs and you'll probably find some good information, or for
> \$50
> you can have it all for sure.

A quick check of ebay.com shows a heap of suitable handbooks at much better
prices than this.

ARRL, RSGB and other books will show you how to make radio things.

Good RF designers can think up new radios and/or aerials and make them work.

But I suspect that no-one actually knows how "radio" (or IR or Light,
all same stuff apparently)  actually  works.

There are theories and  formulas that make  it possible to design
Wireless Sets and  Aerials.

An aerial (wire(s), pin in waveguide, square pad on PCB over a ground
plane) of suitable dimensions connects to an AC signal and the signal in
the wiring becomes "waves" in air or vacuum. There is poor penetration
of liquids and solids, but some.

Below 500kHz it's difficult to have much efficiency in the conversion
process from wires to wave. A 137kHz transmitter with 2kW of power might
only result in 1W of RF waves if an aerial is only 20meters long.  At
10Ghz, you might get over 90% of your electrical energy turned into
radio waves by a connector pin the correct length in a 3/4" copper water
pipe used as a waveguide.

Anyone that thinks they *REALLY* understand radio is not an expert.

Richard Prosser ha scritto:
> That;s a pretty bad example of an AM "transmitter" and I'll leave that
> side of things alone.

For what matters :)
I did a 1MHz AM modulated transmitter using a PIC16.

--

Ciao, Dario
--
Cyberdyne
Dario Greggio wrote:
> For what matters :)
> I did a 1MHz AM modulated transmitter using a PIC16.
>

Back in college I made a 1MHz transmitter that dumped the carrier back onto
the power line.  Best I could tell, it put out about 2 to 3 watts at 1MHz.
We used to play radio station in the dorm on Sunday nights.  One time we had
everyone flush their toilets at the same time.  It took 20 minutes for the
water pressure to come back to the top floors.

solarwind wrote:
> For example, a very simple 1 MHz AM transmitter is described here:

Yucc.  The crystal oscillators I've seen aren't meant for 9V power.  Unless
the data sheet explicitly says so, don't assume it will work at 9V.  If you
believe this bozo's schematic, he's actually running it at 18V, although I
think it's really running on a single 9V battery.

********************************************************************
Embed Inc, Littleton Massachusetts, http://www.embedinc.com/products
(978) 742-9014.  Gold level PIC consultants since 2000.

>
> Back in college I made a 1MHz transmitter that dumped the carrier back onto
> the power line.  Best I could tell, it put out about 2 to 3 watts at 1MHz.
> We used to play radio station in the dorm on Sunday nights.  One time we had
> everyone flush their toilets at the same time.  It took 20 minutes for the
> water pressure to come back to the top floors.
>

Olin was (is?) a wildman.

Rob

http://en.wikipedia.org/wiki/Electromagnetism

is a good a place as any to start. Pointy cap & wand optional :)

Jack
I was going to write something up, but Olin did a very good job so far. I'm
looking forward to seeing more. ;)

Seriously, sit back and think about his example and E field description. Play
with it in your mind. Do that before the ARRL handbook. Although that's a good
resource, you can understand it a little more before you start.

Here are some one-liners to remember that may help pieces fit together as you

- If you hold the end of a string, and wave it up and down, what size makes for
a better 'wave'? It's similar to radio waves, with antenna=string.

- Any conductor interacts with its surroundings, it's just that in most cases
the interaction is insignificant or needs to be reduced out of the situation.
relationship to things around it, and the conductor itself is inductive. Look
at everything in little chunks like that.

- Just like the string-antenna example, it only gets pretty when you get a lot
of waves going on the string. If your wires or antenna are so short that it's
only a small fraction of a wavelength, then it's not interesting ie, it's

- Conversely, you can have something become significant when you don't want it
to - thus, we have EMI, and FCC testing...

- There is also a magnetic component, although not a big deal right now. Keep
in mind capacitance goes with E fields, inductance with M or magnetic fields.

- Again, with the string, there is a certain frequency when the wave seems to
stand still. Why?

- Think of resistance as a reactance, so it has a real resistance and an
imaginary one +/- for the capacitance and inductance under scrutiny. It's just
a good habit. In most cases you can just focus on one part or the other as the
other side might be insignificant, but if you acknowledge it's always there in
changing current, you begin to 'see' more.

- Think of any waveform as a sum of various sine waves. For instance, a square
wave is a sine wave with all its odd harmonics added in (diminishing).

- Filtering happens via capacitance and inductance, and based on the values and
configuration, can attenuate higher frequencies the higher you go, lower ones,
or both (bandpass). Does your model fit one of these configurations? If so,
filtering will happen.

Decompose parts first and get more questions and try to answer them yourself on
what you know. My advice is to not settle with 'cookbook' descriptions if you
really want to learn. You don't really need Maxwell's equations at first
either. Come back and write up how you 'modeled' a part and your analysis and
everyone can discuss.

For instance, just taking a few of the above points and applying to a black box
that produces a square wave output, you attach the signal to some wire and
ground the common from the box. The wire reacts with the ground (earth) via
capacitance. It has inductance since it's a wire. It's producing an E field and
an M field. It does this all along its length, so you can keep thinking smaller
chunks along the line... Decompose the square wave into its frequencies. Each
freq will have a different relationship to your wire 'antenna' here... This
will result in a 'filtered' E field - you won't transmit a square wave! Explain
it further...

Think about that for a while and look for examples that explain it in those
methods, rather than just a simple analogy or such (beyond a simple example
perhaps). You will benefit more that way and not have to 'unlearn' stuff later.

-Skip

On 3/31/2010 2:27 AM, solarwind wrote:
> I've been very interested in electrical engineering and radio
> recently. I've been trying to learn how radio waves tie into
> electrical engineering. How do we create them? How do we receive them?
> the matter, but still do not know exactly how they "work".
>> One time we had everyone flush their toilets at the same time.
>> It took 20 minutes for the water pressure to come back to the top floors.
>>
>
> Olin was (is?) a wildman.

Yes, I still have his story archived somewhere. Made me laugh when he told
it.

Many moons ago I had a dabble with RF..... 27 Mhz children's band and a few
of those really olde things Valves.....

4CX1000A's in class AB1 with 3600V plate voltage at 900mA nearly 3Kw at 27
Mhz...

That's how radio works...Big amplifier... goes anywhere and messed up 405
line tv a treat... well it was 1981... I do micros now less power hungry

Steve

{Original Message removed}
> - If you hold the end of a string, and wave it up and down, what size makes for
> a better 'wave'? It's similar to radio waves, with antenna=string.

Aha. It's The luminiferous aether!
Warning Will Robinson!
Here theyre bee Dragones.

It's like the string but without anything like the string.

Gargoyle 'Michaelson Morley"
Here lmgtfy :-)
(benign as he has no knowledge of MM yet :-) ).

http://en.wikipedia.org/wiki/Michelson%E2%80%93Morley_experiment

http://galileoandeinstein.physics.virginia.edu/lectures/michelson.html

Wow - with flashlets even

http://galileoandeinstein.physics.virginia.edu/more_stuff/flashlets/mmexpt6.htm

But for now it's done with mirrors.

http://scienceworld.wolfram.com/physics/Michelson-MorleyExperiment.html

And Algol and Persus andno ghost stars

http://www.whfreeman.com/modphysics/PDF/1-1c.pdf

So, no string, apparently.
YMMV.

Russell
Russell
> everyone flush their toilets at the same time.  It took 20 minutes for the
> water pressure to come back to the top floors.

Johnny Carson (or was it Letterman?) suggested this on TV 30yrs ago or so.
Interesting to think about on a community or national level... I was talking to
a sewage plant mgr one time and mentioned that show and he remembered. He said
that if even a decent fraction of the city did that there'd be a major sewage
'event' to be cleaned up...

I suspect the top floors could have had some 'fun' with the bottom floors by
doing the same thing, but with a more memorable odor... ;)

> Aha. It's The luminiferous aether!
> Warning Will Robinson!
> Here theyre bee Dragones.
>
> It's like the string but without anything like the string.

Remember, I said not to use simple examples beyond their simplicity... The
string merely showed the ineffectiveness of wire length on a wave, that is all.
It is good for that. Any other use is out of context and will void your warranty...

On 3/31/2010 10:12 AM, Dr Skip wrote:
>> everyone flush their toilets at the same time.  It took 20 minutes for the
>> water pressure to come back to the top floors.
>
> Johnny Carson (or was it Letterman?) suggested this on TV 30yrs ago or so.
> Interesting to think about on a community or national level... I was talking to
> a sewage plant mgr one time and mentioned that show and he remembered. He said
> that if even a decent fraction of the city did that there'd be a major sewage
> 'event' to be cleaned up...
>

Happens all the time.  The water pressure gauges on any US cities water
supply system give perfectly accurate accounting the time and duration
of TV commercials during such events as the Super Bowl.
I think you would be probably better off starting with something veru

The AM demodulator is a simple germanium diode -- in extreme case you do not
even use anything else, only the diode, a long antenna and a head phone.
Then everything else is just an add-on or plug-in if you like it that way.
So you can add as an add-on a resonant for tuning to a specific station,
then a simple audio amp, later on an RF amp so that finally you get a very

Tamas

On Wed, Mar 31, 2010 at 7:27 AM, solarwind <x.solarwind.xgmail.com> wrote:

{Quote hidden}

> -

Dr Skip wrote:

> > One time we had
> > everyone flush their toilets at the same time.  It took 20 minutes for the
> > water pressure to come back to the top floors.

My wife was teaching in a very rough area of town
when the students decided to organize a simultaneous
flush in the school. The 80 year old cast iron sewer pipe
couldn't take the differential pressure and shut the
school down for a day.

w..

Tamas Rudnai wrote:
>I think you would be probably better off starting with something veru
>
> The AM demodulator is a simple germanium diode -- in extreme case you do
> not
> even use anything else, only the diode, a long antenna and a head phone.
> Then everything else is just an add-on or plug-in if you like it that way.
> So you can add as an add-on a resonant for tuning to a specific station,
> then a simple audio amp, later on an RF amp so that finally you get a very

That's how I got started in electronics back in 1993-ish. Well actually
first I was way in over my head, trying to build an acoustic range finder,
but the crystal radio was my first working project. :)

I went on to build a one-valve RF generator, audio amps, and FM bugs.

Vitaliy

On Wed, Mar 31, 2010 at 6:57 PM, Vitaliy <piclistmaksimov.org> wrote:

> That's how I got started in electronics back in 1993-ish. Well actually
> first I was way in over my head, trying to build an acoustic range finder,
> but the crystal radio was my first working project. :)
>
> I went on to build a one-valve RF generator, audio amps, and FM bugs.
>

Good old days :-) I have built a very simple RF oscillator as well to
practise RTTY -- so I was listening the morse code on a real HAM receiver
:-) It had only one transistor and an LC tag something like that, no amp at
the end so I could not interfere with anyone. Later on when I get my HAM

Hmm, my morse key is still somewhere around, I feel like practising again
:-)

Tamas

>
> Vitaliy
>
> -
On Wed, Mar 31, 2010 at 10:45 AM, Olin Lathrop
<olin_piclistembedinc.com> wrote:
> Very briefly.  Voltages do not end at the ends of conductors.  A voltage
> field, called the E field permeates all space.  If you have two pieces of
> aluminum foil 1 meter apart and connect a 12V battery between them, the E
> field between will have a strength of 12V/meter.  Yes, it's really that
> simple.

This is the part I'm having trouble with. I understand that an
electric field is created which propagates at the speed of light. So,
is that propagating field considered the radio wave? Or is it the
propagating electromagnetic field created by an accelerating charge?
Also, if there is no closed circuit, how/why are the electrons
accelerating? Even if there is a potential difference of 12 V, there
is no conductor in between for them to move in?

{Quote hidden}

Ok, I can understand how the field is still propagating at the speed
of light outward. But is that propagating field the radio wave?

{Quote hidden}

Thank you for the explanation.
I just read this from here:
http://cfcp.uchicago.edu/education/explorers/2002summer-YERKES/pdfs-sum02/background.pdf

A radio transmitter whose job it is to move electric charges
rhythmically up and down its antenna sets the signal that is to be
propagated in motion. These waves that are propagated carry
(note: antennas are used both to transmit or and receive signals)
The movement of the electric charges produces a changing electric field--
a structure in space that pushes on electric charges--and a changing
magnetic field--a structure in space that pushes on magnetic poles.
Because the electric field changes with time, it creates the magnetic field
and because the magnetic field changes with time, it creates the electric
field. The two travel off across space as a pair, endlessly recreating one
another in an electromagnetic wave that will continue to the ends of the
its electric field begins to push electric charges up and down on that

This is the part I'm having trouble with:

A radio transmitter whose job it is to move electric charges
rhythmically up and down its antenna sets the signal that is to be
propagated in motion.

How does it "move" charges up and down the antenna if there isn't a
closed circuit?

its electric field begins to push electric charges up and down on that

This makes a little more sense, but I'm still having trouble with this part.
Dr Skip wrote:
> Johnny Carson (or was it Letterman?) suggested this on TV 30yrs ago
> or so.

I did it in the late 1970s, so probably 32 years ago.  Mabye he got the idea
from me ;-)

{Quote hidden}

Guys, you are making this too complicated and confusing.  Mentioning Maxwell
at this point silly and possibly even damaging.  Simplify, but don't make it
inaccurate.  Good presentation is all about keeping the context of the
intended audience in mind.

Now where were we...  Ah yes, we last saw that any voltage change anywhere
causes a little energy to be radiated into space.  Every circuit that
creates a changing voltage is a transmitter, although in most cases a very
useful efficiencies.

Let's think about what transmitting looks like from the circuit's point of
view.  Go back to the example of the two pieces of aluminum foil one meter
apart with a 1/2 meter wire from each to a small circuit board near the
middle.  What would those two connections look like to a driving circuit?
Mostly like a very small capacitor.  The two pieces of aluminum foil make a
capacitor, although at 1m separation a very very small one.  That's the
first order effect.  If you dig deeper, you consider that the wires going to
the two plates have some finite inductance.  This is not because the wires
are imperfect, but because when current travels in a line, it will cause a
circular magnetic field around that line.

So now these aluminum foil pieces with wires to them look like a capacitor
with some inductance in series.  However, remember that neither capacitors
nor inductors (at least perfect ones) can dissipate any energy.  They can
temporarily store energy, but in the long run this has to come out back into
the circuit.  But we saw earlier that this setup transmitted some energy
into space.  Obviously that's not ever coming back to the circuit, so how
can it look like just a capacitor and inductor to the circuit?  Something

It doesn't add up because we left out something.  There is just a little
resistive effect in there that accounts for the energy lost into space.  So
for now we'll add a little resistance in series with the capacitor.  Only a
very small amount of energy is transmitted, so this is a rather high
resistance.

I'm not getting into antenna theory here (that's a few books worth on its
own), but antenna design is usually about ballancing the inherent
inductances and capacitances so that they cancel each other out and what's
left is the apparent resistance from the circuit's point of view.  While it
looks just like a real resistor to the circuit, it doesn't dissipate the
power and turn it into heat, but rather radiates the power into space.

Now we're going to skip over most of antenna theory and get to a simple
result you can reproduce at home on your own.  Take two pieces of wire the
same length, and lay them out end to end in a straight line.  Bring the two
middle ends close but not touching.  Think of them as connecting to two pads
on a small circuit board if that helps.  It so happens that those two points
look like a resistor at a frequency such that the total end to end length of
wire is 1/2 wavelength.  The power that goes into that resistor at that
frequency is quite efficiently radiated into space.  Not only that, the
resistance is well known and is about 75 ohms.  I know this is unintuitive
at the moment, so just believe me for now.

There may have been too much hand waving, so here is a crude attempt at a
picture:

--------------------X--------------------

The X indicates the little circuit board and the dashes are the wires going
out in opposite directions on either side.  The speed of light is about
300Mm/s, so at 300MHz the wavelength is 1 meter, and 1/2 wavelength is 1/2
meter.  So if the end to end length in the picture above is 1/2 meter, the
two wires will look like a 75 ohm resistor at 300MHz.  At 1m total length it
would look like 75 ohms at 150MHz.  Note the important stipulation of this
75 ohm phenomenon happening at a particular frequency.  Clearly it doesn't
happen at DC since there is looks like a open circuit.  The inductive and
capacitive effects are still there, but at the critical frequency they
happen to cancel each other out such that the net current to voltage phase
shift is 0, which makes it look like a pure resistor to the circuit.  That
means this thing draws real power from the circuit (at the critical
frequency).  It doesn't burn up this power as heat like a real resistor
would, but instead radiates it into space.  From the circuit's point of
view, it's the same thing though.

This is what a antenna does, and the type of antenna described above is
probably the most basic of all and is called a "dipole".  There are lots of
different antenna types.  They vary in their radiation pattern (which
direction the energy gets radiated), the resistance at the critical
frequency, how they behave over a larger range of frequencies, etc.  For
example, another type of antenna is called a "folded dipole".  I don't want
to get into that further, but it happens to look like a 300 ohm resistor at
the critical frequency.

So lets say you have a 1 meter dipole as shown above.  We know it will look
like a 75 ohm resistor at 150MHz.  So how do you make a transmitter?  You
feed a 150MHz signal between the two pads on the little circuit board.
Let's say you can produce a 5V peak to peak 150MHz sine wave on that board.
That's about 1.8V RMS.  Feeding 1.8V into a 75 ohm resistor dissipates 43mW,
which would make a ordinary resitor just a little warm.  Feeding the same
1.8V at 150MHz between the two pads on the little circuit board above will
instead radiate the same 43mW into space.  That's actually a fair amount of
power.  Off the shelf receivers could pick up that signal 100s to 1000s of
meters away.

Time to go again.  Maybe more later.

********************************************************************
Embed Inc, Littleton Massachusetts, http://www.embedinc.com/products
(978) 742-9014.  Gold level PIC consultants since 2000.
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On Wed, 2010-03-31 at 10:28 -0700, Marcel Duchamp wrote:

{Quote hidden}

There was a recent graph released of water usage in Edmonton, Canada,
showing the correlation between breaks in the US vs CDN olympic hockey
game:

http://www.patspapers.com/blog/item/what_if_everybody_flushed_at_once_Edmonton_water_gold_medal_hockey_game/

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--=-7FRwFfcqx7KxktyHHyQV--

part 2 35 bytes content-type:text/plain; charset="us-ascii"
(decoded 7bit)

Let's arrange a international "flushing minute" event.
Gus

On Mar 31, 2010, at 11:12 AM, Dr Skip wrote:

> everyone flush their toilets at the same time.  It took 20 minutes
> for the
> water pressure to come back to the top floors.

Johnny Carson (or was it Letterman?) suggested this on TV 30yrs ago or
so.
Interesting to think about on a community or national level... I was
talking to
a sewage plant mgr one time and mentioned that show and he remembered.
He said
that if even a decent fraction of the city did that there'd be a major
sewage
'event' to be cleaned up...

I suspect the top floors could have had some 'fun' with the bottom
floors by
doing the same thing, but with a more memorable odor... ;)

> Aha. It's The luminiferous aether!
> Warning Will Robinson!
> Here theyre bee Dragones.
>
> It's like the string but without anything like the string.

Remember, I said not to use simple examples beyond their simplicity...
The
string merely showed the ineffectiveness of wire length on a wave,
that is all.
It is good for that. Any other use is out of context and will void

> Also, if there is no closed circuit, how/why are the
> electrons accelerating? Even if there is a potential
> difference of 12 V, there is no conductor in between
> for them to move in?

Once it leaves the antenna, it can be helpful to think of radio waves like
light.  In fact, they basically are light; low frequency light.  And the
lower the frequency, the less like light.

At frequencies above about 100 MHz, propagation is pretty much line of
sight, just like light.  At frequencies above about 1 GHz or so, things
like rain and fog interfere with the propagation, much like light.

As you get lower, funny things happen.  In the tens of megahertz range,
the waves sometimes "bounce off" the ionosphere, which is why short wave
propagation works over huge distances.  The waves are still pretty much
line of sight, it's just that there is a huge mirror in the sky.  At still
lower frequencies, there is a tendency to follow the earth's curvature.
This is why you can hear a powerful AM station well beyond line of sight.

Someone earlier in this thread said something along the lines of anyone
who thinks he knows all about radio is fooling himself. This is pretty
much true.  But it isn't too hard to understand enough to use it
effectively, and only a little harder to learn enough to design circuits.

A lot of people mentioned the ARRL Handbook, which has become pretty much
the bible for these things.  The Handbook is published every year, and it
doesn't change a lot from year to year.  For your initial studies, a copy
10 or even 20 years old will be good enough for your purposes, and these
can be found at flea markets or online for far less than the latest copy.
On the other hand, it isn't all THAT expensive new, and an online order
direct from the ARRL or any of dozens of other outlets could be quick and
easy.

--McD

What if everybody in Canada flushed at once:

http://www.patspapers.com/blog/item/what_if_everybody_flushed_at_once_Edmonton_water_gold_medal_hockey_game/

Turns out that during the US/Canada olympic hockey game this was put
to the test inbetween the periods - a game which about 80% of all
canadians were estimated to be watching.

It's a very, very interesting bit of data.

On Wed, Mar 31, 2010 at 3:38 PM, YES NOPE9 <yesnope9.com> wrote:
{Quote hidden}

>
Solarwind wrote:
> I understand that an
> electric field is created which propagates at the speed of light. So,
> is that propagating field considered the radio wave?

Yes.  Actually the magnetic field (B field) is envolved too.  I talked about
voltage only, but a directed propagating wave is actually tightly linked
disturbances in both fields.  This is what happens once radiation has left
its source and is no longer coupled to that source.  In other words, it
takes both the E and B fields to make a propagating wave.  However, don't
confuse that with how you can launch such waves.

> Or is it the
> propagating electromagnetic field created by an accelerating charge?

This makes little sense.  Moving charges create a circular B field
perpendicular to the direction of motion.  I don't think that's what you're
referring too.  There is a special way to create a propagating wave by
accellerating a charge (bremsstrahlen), but that's pretty advanced stuff and
not likely what you are referring to either.  So in short in your context, I
think the answer is "radio waves don't have anything to do with
accellerating charges".

> Also, if there is no closed circuit, how/why are the electrons
> accelerating? Even if there is a potential difference of 12 V, there
> is no conductor in between for them to move in?

Nobody said anything about electrons accellerating.  Electrons sloshing
around may start a electromagnetic wave going, but they have nothing to do
with propagating one.  After all, the propagation can happen in vacuum where
there are no electrons.

> Ok, I can understand how the field is still propagating at the speed
> of light outward. But is that propagating field the radio wave?

Yes.

> A radio transmitter whose job it is to move electric charges
> rhythmically up and down its antenna sets the signal that is to be
> propagated in motion.
>
> How does it "move" charges up and down the antenna if there isn't a
> closed circuit?

That's a good question and a tough one to explain.  In fact there is a
closed circuit, but only at AC.  If you only look at the AC component, and
particularly the carrier frequency, the circuit is a lot different than it
appears by looking at a dead end wire sticking into the air.  For one thing,
there are inductances and capacitances that make it a closed circuit at the
carrier frequency.  But these are not just any inductances and capacitances.
They are specially arranged together with the geometry of the wire so that
energy rythmically sloshes back and forth in different forms from one end of
the wire to the other.  The electrons don't leave, but they are kept
sloshing.  Since this sloshing is at resonance or close to it, the magnitude
of the sloshes are generally much higher than the magnitude of the input
signal needed to keep it sloshing.

Think of a bathtub half full of water.  Leaning over the tub from the
outside, you can put your hand in the middle and move it back and forth a
little bit.  If you do this at just the right frequency, you can get some
pretty dramatic sloshing going on.  It takes very little force to keep the
wave heights at the ends of the tub several times the amount you move your
hand each cycle.  In this case the tub is sortof like a center fed dipole.
The transmitter puts a little bit of energy into the middle, which causes a
lot of sloshing back and forth.  That means the AC voltage at the ends is
high, and the AC current in the middle is high.  Eventually these voltages
and currents get so high that a significant fraction of the energy gets
radiated into space each wave.  The transmitter has to put that energy back
each wave to keep the sloshing, and therefore the transmitting, going.

Antennas can be designed so that the transmitter input can be at one end
instead of the middle, but the principle is still the same.  A little input
makes a lot of sloshing, which eventually gets so strong that it causes
enough of a disturbance in the local E and B fields such that they start
carrying energy away each cycle.  That's the energy the transmitter has to
add back each cycle to keep things going.  The energy that is carried away
eventually (within a wavelength or so) organizes itself into a
self-propagating wave.  It becomes a continuous dance between the E and B
fields which propagates at the speed of light.  It is this propagating E/B
field dance we call electromagnetic radiation.  For simplicity we call the
lower frequencies of it (a few 10s of KHz to a few GHz) radio waves.  At a
little higher frequencies we call them microwaves or radar waves, then
terahertz radiation, then infrared, then visible light from red to green to
blue, then ultraviolet radiation, then X rays, then gamma rays.  Despite the
different names for different frequency ranges, they are all exactly the
same propagating dance between the E and B fields, differing only in how
fast they dance back and forth (the frequency).

Since the propagation always happens at the speed of light (in a vacuum
anyway), frequency and wavelength are just reciprocals of each other.  Often
you will hear the higher frequency waves identified by wavelength instead of
frequency, but keep in mind that either is specifying the same thing.  Since
the speed of light in vacuum is about 300Mm/s, a 300MHz radio wave and a 1
meter radio wave are the same thing.  It's humbling to ponder the vast
dynamic range of electromagnetic field frequencies (or wavelengths).  WWVB
transmits the NIST atomic clock time signal from Boulder at only 60KHz.
That's a wavelength of 5Km, or 3.1 miles.  1MHz is in the middle of the AM
band, with a wavelength of 300 meters or about .2 miles.  Visible light
covers roughly a 2:1 range from about 350 to 700 nm, and X rays and gamma
rays are still many times smaller than that.

********************************************************************
Embed Inc, Littleton Massachusetts, http://www.embedinc.com/products
(978) 742-9014.  Gold level PIC consultants since 2000.
> How does it "move" charges up and down the antenna if there isn't a
> closed circuit?

If you insist on thinking about it in terms of circuits, free space
constitutes  ~  75 Ohm path to "ground", in the "RF" spectrum.

Experts, feel free to substitute your favored impedance.

best regards,

Jack
Free space Z is ~377 ohms, based on Helmhotz equations.
We had to derive it from first principles in EM class.

http://en.wikipedia.org/wiki/Impedance_of_free_space

John Gardner wrote:

{Quote hidden}

Thanks.

Jack

2010\04\01@005745 by
I think I found another helpful explanation here:

Here are the two explanations:

"the antenna is connected to a transmitter which is designed to output
a voltage as a function of time. this voltage is an e.m.f. that forces
free charge in the conductive element of the transmitting antenna to
slosh back and forth along the element. in the receiving antenna,
there is free charge in the conductive element that are affected
(because like-signed charges repel and unlike-signed charges attrack)
by the movement of charge that is happening in the transmitting
antenna. because of the usual large distance between the transmitting
antenna and the receiving antenna, that movement of charge in the
receiving antenna is minute, much smaller than the quantity of charge
and movement in the transmitting antenna. but that is what receivers
and RF amplifiers are for; making that small movement of charge
control a much larger movement of charge (that eventually finds its

so you have the motion of charge at one location affecting the
movement of charge at another location. since the reaction of charge
in the receiving antenna is not an instantaneous reaction (from the
POV of an observer that is equal distant between the two antennae),
what is it that is in between the two antennae that, after a finite
period of time, forces the charge in the receiving antenna to move?"

Is this correct? So is he saying that simply oscillating the voltage
from, let's say, +5 to -5 volts like a sine wave at the end of the
antenna, causes the free electrons on the antenna to slosh back and
forth on the antenna, thereby creating an electromagnetic wave?

If so, is the only way to govern the "output power" of the transmitter
to change the voltage applied to the antenna? Or is there another way?

Also, is the voltage output terminal that the antenna is connected to
usually high impedance or low impedance?

"The transmitter voltage does not create the electric field. The
transmitter outputs current and voltage simultaneously, as well as an
E and H field simulataneously. E, H, I, & V are all in unison for a
resistive t-line (Z0 = real). There is a finite impedance value for
the transmission line, Z0. The current and voltage are simultaneously
present and Ohm's law is always upheld. For a 300 ohm Z0, the
transmitter connected at the input outputs a V and an I, say 600 mV
and 2.0 mA. The I and V waveforms travel along the t-line and when the
end is reached the E and H fields radiate power into space.

The reason is that an antenna only works for high enough frequencies.
The current here is displacement current. No closed path is reuired
for such. The t-line ends abruptly in mid-air, yet current exists. The
E and H fields are present in between the conductors of the t-line.
Then at the end where it ends, the fields continue to propogate into
space.

Have I helped or made matters worse?"

Ok, I have no idea what this person is saying here.
John Gardner wrote:
> If you insist on thinking about it in terms of circuits, free space
> constitutes  ~  75 Ohm path to "ground", in the "RF" spectrum.

Wrong.  The impendance of free space 370 something ohms.  This also has very
little to do with what the OP was asking, and will likely only confuse.
It's bad enough he's getting flooded with distracting and confusing
information, but outright wrong information is even worse.  Please refrain
if you can't even get the facts right.

********************************************************************
Embed Inc, Littleton Massachusetts, http://www.embedinc.com/products
(978) 742-9014.  Gold level PIC consultants since 2000.
solarwind wrote:
> Is this correct? So is he saying that simply oscillating the voltage
> from, let's say, +5 to -5 volts like a sine wave at the end of the
> antenna, causes the free electrons on the antenna to slosh back and
> forth on the antenna, thereby creating an electromagnetic wave?

Yes.

> If so, is the only way to govern the "output power" of the transmitter
> to change the voltage applied to the antenna? Or is there another way?

That's the simplest way and the way AM radio works because the output power
has to be modulated by the same signal you ultimately hear coming out of a

However, there are other ways to change the power seen by a distant
receiver.  You could change the orientation of the antenna, since most
antennas do not radiate the same power in all directions.  You could change
the antenna length and geometry to de-tune it, for example.

In practise, the usual way to modulate output power is to modulate the
voltage of the carrier fed into the antenna.

> Also, is the voltage output terminal that the antenna is connected to
> usually high impedance or low impedance?

It's usually low or specifically designed to drive the impedence presented
by the particular antenna in use.  75 and 50 ohms are common transmitter
output impedences.

********************************************************************
Embed Inc, Littleton Massachusetts, http://www.embedinc.com/products
(978) 742-9014.  Gold level PIC consultants since 2000.
>> Also, is the voltage output terminal that the antenna is connected to
usually high impedance or low impedance?

1. An antenna, as seen by a transmitter or receiver, is a complex
impedance (R+jX). R is the radiation resistance plus loss resistance. X is
the reactance. Antenna current squared times radiation resistance is the
power actually radiated. Antenna current squared times the loss resistance
is power lost to heat. Reactance is due to a non-resonant antenna
configuration and can be tuned out with a series inductor or capacitor,
though these also add losses (and for high reactances, the resistive
losses in the compensating reactance can be significant).

2. Amplitude modulation is multiplication of the carrier sine wave by the
modulating signal plus an offset. For example,
V(t)=(sin(wc*t)*(1+sin(wm*t) where wc is the carrier frequency in radians
per second and wm is the modulating frequency in radians per second. If
you remove the "1+", the signal changes from normal AM (double sideband
with carrier) to DSBSC (double sideband supressed carrier). A common
method of generating AM (called high level modulation) is to just put the
audio in series with the DC to the RF amplifier. This is often done with a
"modulation transformer". Broadcast transmitters would use a modulation
reactor in addition to a modulation transformer so the DC current of the
RF amplifier does not go through the modulation transformer, thereby
reducing distortion due to core saturation. You can see schematics of

3. There are all sorts of modulation tricks that can be simplified down to
two DSPSC signals added together where the carriers are shifted by 90
degrees. You can generate analog or digital QAM, phase modulation, etc.
using this technique.

4. Antenna geometry determines the driving point impedance, the radiation
pattern, and the gain. Gain is usually expressed as dBi or dB over
directional antenna radiates less in some directions and more in others.
An example of calculating the field strength from an isotropic radiator as
shown at the end of the article at
http://louise.hallikainen.org/rw/insite/insite73.html . It comes down to
putting a sphere around the radiatior. The sphere absorbs all the power
that was radiated by the antenna. As the sphere is enlarged, its surface
area becomes larger, so the power density (watts per square meter)
decreases, but the total power remains the same. Electromagnetic
transmission through a vacuum is lossless. Through other media there may
be absorbtion where some  of the power is converted to heat. Watts per
square meter can be converted to a field strength of volts per meter or
amperes per meter using Ohm's law where R is  the impedance of free space
(about 377 ohms). 377 ohms = (V/m)/(A/m) in the "far field". Other media
have different impedances. The impedance may be though of as the
characteristic impedance of a transmission line. At a media boundary,
where the characteristic impedance changes, some of the signal is
transmitted in to the new medium and some is reflected. The ratio depends
on the ratios of the characteristic impedances. A shielded enclosure works
by reflecting most of the signal back in to the enclosure and transmitting
a little into the wall of the enclosure. At the outer surface of the
enclosure, the wave is again reflected back into the enclosure wall by the
impedance change at the outer wall while some is transmitted  out of the
enclosure.

It's all interesting stuff....

Harold

Good luck!

Harold

--
FCC Rules Updated Daily at http://www.hallikainen.com - Advertising
opportunities available!

Antennas are an especially fascinating aspect of "Radio". A resonant
Demo copy of EZNEC and model most antennas for a quick study. The ARRL Radio
Amateur's Handbook is the best and most available source for such
information. The antenna information is relevant at least back into the
1930's. The ARRL Antenna Handbook is a bit deeper and of course more
specialized. You might make the jump from there to one of John Krause's
books. If you understand John Krause's work you are ready to teach the
subject. Terman's Radio Engineering is also tough to beat. The 1938 edition

Don't be turned off by anything labeled "Radio Amateur". It is NOT "Radio
for Dummies"!

BTW, I discovered a new (1990's) mode of operation in February known as
BPSK-31. From North Carolina I have since worked stations all over the world
(including Melbourne Australia, Europe and Siberia with about 30 watts.

Also, check out your University for a "Ham Radio Club". If they have one it
is likely populated by fellow Nerds with an Electronics Obsession. You will
feel at home there!

John Ferrell  W8CCW

"A nation of sheep will beget a government of wolves."
-Edward R. Murrow
{Original Message removed}
On Thu, Apr 1, 2010 at 9:46 AM, Olin Lathrop <olin_piclist@embed
>> If so, is the only way to govern the "output power" of the transmitter
>> to change the voltage applied to the antenna? Or is there another way?
>
> That's the simplest way and the way AM radio works because the output power
> has to be modulated by the same signal you ultimately hear coming out of a
>
> However, there are other ways to change the power seen by a distant
> receiver.  You could change the orientation of the antenna, since most
> antennas do not radiate the same power in all directions.  You could change
> the antenna length and geometry to de-tune it, for example.
>
> In practise, the usual way to modulate output power is to modulate the
> voltage of the carrier fed into the antenna.

Now I'm trying to sort out the connection between amplitude of the
radio wave and the power of the transmitter.

So can it be said that by varying the voltage of the antenna, we are
varying the amplitude of the wave as well as fluctuating the output
power proportional to the varied voltage? Is it the amplitude that
governs the output power of the antenna or is it the number of photons
created? What is the relationship between the amplitude, power, and
number of photons?

>
> Don't be turned off by anything labeled "Radio Amateur". It is NOT "Radio
> for Dummies"!

I've heard this about Marconi "I myself am only an amateur". Attributed to
Marconi at the 1933 Chicago World's Fair Amateur Radio special event
station. I only find a couple references on Google, but I had also heard
it many years ago. Don't know if it's true...

Harold
WA6FDN

--
FCC Rules Updated Daily at http://www.hallikainen.com - Advertising
opportunities available!
This has been a great thread.  Many Thanks to Olin, Harold, and John.
Another good reference on all this is "Electromagnetics Explained"  By Ron
Schmitt.  ISBN 0-7506-7403-2.
It's light on the math and heavy on the intuitive explanations (if you can
consider anything RF "intuitive").

Cheers,
Dave Challis
KA6DRC

> {Original Message removed}
On Thu, Apr 1, 2010 at 10:50 AM, solarwind <x.solarwind.xgmail.com> wrote:
{Quote hidden}

Whoops, I just realized that I tried to merge the wave theory and
particle theory of electromagnetic radiation. There appears to be a
relationship, in that amplitude ~~ sqrt(# of photons), amplitude is
proportional to the square root of the number of photons.
Harold Hallikainen ha scritto:
> I've heard this about Marconi "I myself am only an amateur". Attributed to
> Marconi at the 1933 Chicago World's Fair Amateur Radio special event

:)

great Marconi!
one of the latest good italians...
Harold Hallikainen wrote:
>> Don't be turned off by anything labeled "Radio Amateur". It is NOT "Radio
>> for Dummies"!
>>
>
> I've heard this about Marconi "I myself am only an amateur". Attributed to
> Marconi at the 1933 Chicago World's Fair Amateur Radio special event
> station. I only find a couple references on Google, but I had also heard
> it many years ago. Don't know if it's true...
>
> Harold
> WA6FDN
>
>
>
At a tangent...

meaning   (unpaid)  rather than  modern  meaning (incompetent) .  Of
course thre are idiot Amateurs, just as there are idiot "Paid
to run box and aerial to people that actually design and build stuff.
The only group of people allowed to legally build and use uncertified
Wireless Transmission equipment.

I & Q based schemes to generate modulation may need very linear
amplifiers for (C)OFDM or  higher QAM modulations of digital base band
remote control are the only common modes that use on/off keying of
signal, like 0V and 5V in Digital circuits.

A promising field of research is Polar drive  (Amplitude and Phase ),
the Amplitude part of the signal modulates a SMPSU that powers  a Class
C (or even D)  RF  amp  fed  with  carrier   modulated by  phase.

Before DSP it was nearly impossible to work this as the AM part lags in
time the PM part and the AM part is very non-linear. A DSP system can
measure a test signal (alternate sawtooth on Amplitude and Phase drives
with the other signal at a nominal 50%). Then the system uses a feed
forward lookup table of pre-distortion and a suitable digital delay on
the Baseband Phase component. Like I & Q system, a polar amp can
generate any modulation, but I & Q on DSP needs two matched DACs (or one
twice as fast and a switch). A Polar amp can use a DSP NCO to generate
the phase varying carrier direct and generate the PWM direct drive for
the SMPSU output FETS (removing the normal SMPSU anlogue feedback and
PWM circuits. Thus the  receiver   ADCs   can be used to  calibrate the
transmitter  via  a sample line.

I don't think NEC is useful for all types of aerials and all frequencies
(10kHz to 100GHz, say) as there may be ground effects at low frequencies
and very inefficient aerial  and at high frequencies there are better
tools to work with striplines , waveguides, patch antennna arrays and
dishes.

As with any modelling tool you need to know what model to put in. Try
model of a 1MHz to 60MHz transformer in spice. Without knowing a lot of
hard to measure parameters, your model results are meaningless.

solarwind wrote:
> Now I'm trying to sort out the connection between amplitude of the
> radio wave and the power of the transmitter.
>
> So can it be said that by varying the voltage of the antenna, we are
> varying the amplitude of the wave as well as fluctuating the output
> power proportional to the varied voltage? Is it the amplitude that
> governs the output power of the antenna or is it the number of photons
> created? What is the relationship between the amplitude, power, and
> number of photons?

The power out the antenna is proportional to the square of the voltage in,

Let's say the antenna is a ordinary dipole tuned to the carrier frequency.
That means it has a characteristic impedence of 75 ohms at the carrier
frequency.  If the transmitter feeds 10V carrier into the antenna, then the
radiated power (ignoring the little loss in the antenna) is (10V)**2 /
75ohms = 1.3 Watts.  If the voltage were doubled to 20V, then the radiated
power would quadruple, and so would the power the transmitter has to put out
to maintain that voltage.

********************************************************************
Embed Inc, Littleton Massachusetts, http://www.embedinc.com/products
(978) 742-9014.  Gold level PIC consultants since 2000.
Dario Greggio wrote:
> Harold Hallikainen ha scritto:
>
>> I've heard this about Marconi "I myself am only an amateur". Attributed to
>> Marconi at the 1933 Chicago World's Fair Amateur Radio special event
>>
>
> :)
>
> great Marconi!
> one of the latest good italians...
>
part Irish.
Michael Watterson ha scritto:
>> great Marconi!
>> one of the latest good italians...
>>
> part Irish.

wow, really he was, Michael?
going to wikipedia now, I never heard that!

(indeed we study only a "little" of modern history in here...)

--

Ciao, Dario
--
Cyberdyne

The greatest book of all time on the subject is "La Radio ? mais c'est
très simple!" by Eugène Aisberg.
(in my opinion)
On Thu, Apr 1, 2010 at 12:16 PM, Marechiare <marechiaregmail.com> wrote:
>
> The greatest book of all time on the subject is "La Radio ? mais c'est
> très simple!" by Eugène Aisberg.
> (in my opinion)

Is there an English version? I'm not that fluent in French, not enough
for science anyway.
>>
>> The greatest book of all time on the subject is "La Radio ?
>> mais c'est très simple!" by Eugène Aisberg.
>> (in my opinion)
>
> Is there an English version? I'm not that fluent in French, not
> enough for science anyway.

I don't know English version, but in French the book (ISBN:
210004107X) reached 29 édition in 1998:
catalog-retail.amazon.fr/abis/syh/DisplayCondition?_encoding=UTF8&coliid=&qid=&asin=210004107X&sr=&colid=&ld=AMZDP
What other languages do you know? The book was published in about
dozen languages.
My favorite explanation on how radio works is that apparently given by Einstein:

http://monster-island.org/tinashumor/humor/eincat.html

-- Peter

On Thursday, April 1, 2010, Marechiare <marechiaregmail.com> wrote:
> I don't know English version, but in French the book (ISBN:
> 210004107X) reached 29 édition in 1998:
> catalog-retail.amazon.fr/abis/syh/DisplayCondition?_encoding=UTF8&coliid=&qid=&asin=210004107X&sr=&colid=&ld=AMZDP
> What other languages do you know? The book was published in about
> dozen languages.

Well French, English, and another one which I'm pretty sure the book
is not published in.
On Fri, Apr 2, 2010 at 12:53 AM, solarwind <x.solarwind.xgmail.com> wrote:

> Well French, English, and another one which I'm pretty sure the book
> is not published in.
>

Just curious, what is the "another" language?

Thanks
Tamas

>
> -
> My favorite explanation on how radio works is that apparently given by Einstein:
>
> http://monster-island.org/tinashumor/humor/eincat.html

It's dead certain that Heisenberg probably may or may not have been
happy with that explanation, if he were still alive, or not.

Russell
>> My favorite explanation on how radio works is that apparently given by
>> Einstein:
>>
>> http://monster-island.org/tinashumor/humor/eincat.html
>
> It's dead certain that Heisenberg probably may or may not have been
> happy with that explanation, if he were still alive, or not.
>
>
>             Russell

You probably mean Schrodinger (sp?), not Heisenberg.

-- Bob Ammerman
RAm Systems

>>> http://monster-island.org/tinashumor/humor/eincat.html

>> It's dead certain that Heisenberg probably may or may not have been
>> happy with that explanation, if he were still alive, or not.

> You probably mean Schrodinger (sp?), not Heisenberg.

Should really be Schroedinberg or Heisendinger - probably the latter,
as we need concepts of cats and uncertainty.

R

Here is a collection of free ebooks:

http://www.pmillett.com/tecnical_books_online.htm

MJ

On 31-Mar-10 04:54, Russell McMahon wrote:
{Quote hidden}

Wow, thanks!

On Sat, Apr 3, 2010 at 10:44 AM,  <enkitecgmail.com> wrote:
>
>     Here is a collection of free ebooks:
>
>     http://www.pmillett.com/tecnical_books_online.htm
>
>     MJ
>
>

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