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Guest
Posted: Tue Oct 09, 2007 9:40 am
Good day to everyone!

Please, I am in search of a book that describe how derive Kirchhoff's
Current Law (KCL), Kirchhoff's Voltage Law (KVL), Ohm's law from
Maxwell's equations.

I have seen something using the Perturbation theory (quantum
mechanics) and I know that something has been written in
Electromagnetic Fields, Energy, and Forces by Robert M. With Lan Jen
Chu and Richard B. Adler Fano.

have you other suggestion?

thank you and sorry for my "school of broken english"

G.M.S.
Italy
Frank Deicke
Posted: Tue Oct 09, 2007 11:33 am
Guest
gianmaria.sandigliano@gmail.com wrote:
Quote:
Good day to everyone!

Please, I am in search of a book that describe how derive Kirchhoff's
Current Law (KCL), Kirchhoff's Voltage Law (KVL), Ohm's law from
Maxwell's equations.

I have seen something using the Perturbation theory (quantum
mechanics) and I know that something has been written in
Electromagnetic Fields, Energy, and Forces by Robert M. With Lan Jen
Chu and Richard B. Adler Fano.

have you other suggestion?

thank you and sorry for my "school of broken english"

G.M.S.
Italy


Try that one:
Ramo, Simon: "Fields and waves in communication theory".
There are some good explanations to Maxwell's equations, KCL, KVL and
Ohm's law.

Frank
Timo A. Nieminen
Posted: Tue Oct 09, 2007 2:59 pm
Guest
On Tue, 9 Oct 2007, gianmaria.sandigliano@gmail.com wrote:

Quote:
Good day to everyone!

Please, I am in search of a book that describe how derive Kirchhoff's
Current Law (KCL), Kirchhoff's Voltage Law (KVL), Ohm's law from
Maxwell's equations.

I have seen something using the Perturbation theory (quantum
mechanics) and I know that something has been written in
Electromagnetic Fields, Energy, and Forces by Robert M. With Lan Jen
Chu and Richard B. Adler Fano.

You're not going to get Ohm's law from the Maxwell equations. The
minimal set would be the Lorentz force law, and diffusion subject to an
external force. This will give you Ohm's law qualitatively, but isn't
going to tell you the conductivity of any real material (you might get
this in a heavy-duty solid state physics book). Easy enough - in the
diffusive regime, the electron drift velocity is proportional to the
electric field, this velocity and the electron density tell you the
current. The voltage drop is just V=E*L, where L is the length of the
conductor.

For the voltage law, you just need the fact that you can express the
electrostatic field as the gradient of a scalar potential (which you can
show from the Maxwell equations if you wish). Integrate E.dl about a
closed loop and what answer do you get?

For the current law, just use conservation of charge, which, again, you
can show from the Maxwell equations.

Of the three laws you're asking about, Ohm's law is the only difficult
one, and it's very difficult, especially if you want to deal with real
materials, for which the conductivity is not a constant. Ohm's law is a
convenient approximation, very useful since it's simple, but it isn't
correct in a strict sense. It's usually just assumed as one of the three
constitutive relations in classical electromagnetism (J=conductivity*E,
along with D=epsilon*E, B=mu*H).

--
Timo Nieminen - Home page: http://www.physics.uq.edu.au/people/nieminen/
E-prints: http://eprint.uq.edu.au/view/person/Nieminen,_Timo_A..html
Shrine to Spirits: http://www.users.bigpond.com/timo_nieminen/spirits.html
Guest
Posted: Wed Oct 10, 2007 4:57 am
Thanks Timo, but i know what you are saying.
I need the complete bound between Maxwell's low and KVL and KCL for a
formal demostration in Electromagnetic Compatibility course at
University (Politecnico Tourin - Electronic engineering).
With the perturbation theory (http://en.wikipedia.org/wiki/
Perturbation_theory), working on parameter i can made a bound with
dimensional and "tipical" timing of a circuit, defining a break point
where classic kvl and kcl don't give exact solvutions.
A0 order give us classic kvl and kcl
The "higher orders" rapresent for ex. (depends on witch maxwell's
equation you are working on) external magnetic influence.

We have done a "first" demostration of this in classroom, and
something about it is written in
Electromagnetic Fields, Energy, and Forces by Robert M. With Lan Jen
Chu and Richard B. Adler Fano (year 1960, little problem to found
it!).

Not a lot about it has been written, some scientific articles... so i
was in search of some news on this specific application for write a
little "thesis" (not the final one of my study Razz)

Thanks a lot!

G.M.S.


On 9 Ott, 21:59, "Timo A. Nieminen" <t...@physics.uq.edu.au> wrote:
Quote:
You're not going to get Ohm's law from the Maxwell equations. The
minimal set would be the Lorentz force law, and diffusion subject to an
external force. This will give you Ohm's law qualitatively, but isn't
going to tell you the conductivity of any real material (you might get
this in a heavy-duty solid state physics book). Easy enough - in the
diffusive regime, the electron drift velocity is proportional to the
electric field, this velocity and the electron density tell you the
current. The voltage drop is just V=E*L, where L is the length of the
conductor.

For the voltage law, you just need the fact that you can express the
electrostatic field as the gradient of a scalar potential (which you can
show from the Maxwell equations if you wish). Integrate E.dl about a
closed loop and what answer do you get?

For the current law, just use conservation of charge, which, again, you
can show from the Maxwell equations.

Of the three laws you're asking about, Ohm's law is the only difficult
one, and it's very difficult, especially if you want to deal with real
materials, for which the conductivity is not a constant. Ohm's law is a
convenient approximation, very useful since it's simple, but it isn't
correct in a strict sense. It's usually just assumed as one of the three
constitutive relations in classical electromagnetism (J=conductivity*E,
along with D=epsilon*E, B=mu*H).
Timo A. Nieminen
Posted: Wed Oct 10, 2007 6:27 am
Guest
On Wed, 10 Oct 2007, gianmaria.sandigliano@gmail.com wrote:

Quote:
Thanks Timo, but i know what you are saying.
I need the complete bound between Maxwell's low and KVL and KCL for a
formal demostration in Electromagnetic Compatibility course at
University (Politecnico Tourin - Electronic engineering).
With the perturbation theory (http://en.wikipedia.org/wiki/
Perturbation_theory), working on parameter i can made a bound with
dimensional and "tipical" timing of a circuit, defining a break point
where classic kvl and kcl don't give exact solvutions.
A0 order give us classic kvl and kcl
The "higher orders" rapresent for ex. (depends on witch maxwell's
equation you are working on) external magnetic influence.

We have done a "first" demostration of this in classroom, and
something about it is written in
Electromagnetic Fields, Energy, and Forces by Robert M. With Lan Jen
Chu and Richard B. Adler Fano (year 1960, little problem to found
it!).

Not a lot about it has been written, some scientific articles... so i
was in search of some news on this specific application for write a
little "thesis" (not the final one of my study Razz)

Well then, you need to consider when the static/quasi-static assumptions
fail. When does radiation become important? Is there any other
electromagnetic effect other than radiation that can make circuit theory
fail? Why or why not? There was a paper addressing some of this in the
last few months on this in Am. J. Phys., iirc, and there have been other
related papers in the past in the same journal.

As it's for assessment, the point is to show what you know and
_understand_, rather than what other people know (at least, it should be
the point!). For example, why do you choose a particular break point where
the circuit laws fail? What does this break point mean physically, beyond
being a usual engineering rule-of-thumb?

KVL is about how well a voltage (does this depend on gauge?) behaves as
you become non-electrostatic. KCL depends on how well you can talk about
"current in a wire", with non-static fields. How do you decide where to
choose a break-point?

--
Timo Nieminen - Home page: http://www.physics.uq.edu.au/people/nieminen/
E-prints: http://eprint.uq.edu.au/view/person/Nieminen,_Timo_A..html
Shrine to Spirits: http://www.users.bigpond.com/timo_nieminen/spirits.html
Guest
Posted: Thu Oct 11, 2007 4:44 am
Hi Timo,

My gratitude debt with you is every-day greater! :-D

You are right in all exept one thing. The assessment :-D

I'am 30, i can not study when it was time and i am studying now with
huge effort Razz
1- because i have lost a lot of physics grounds
2- because i have to share my time with family and work
So, now, assessment in not the real target of my study, i study
because i WANT

My need of know what other people know is because the objective of my
essay is a
comparison of the ways used to define a break point that i tnink is
allready well know:
- the circuit laws start to fail when circuit's size are of same order
of magnitude of wavelength of signals we are using
Far from this condition we use circuits low. Under this condition we
have Microwave Engineering.

In classroom we have proved it using perturbation theory.
But my professor says that there are other ways, not well documented
(or may be right say not well documented for student use)
for reach the same target and, if some students want to try to find
them, they can do it and write a little essay...

so it is what i am trying to do Very Happy
1- find
2- understand what i find and compare Razz
3- write ;-)

Thank you again, also for bear with me :-)

G.M.S.




Quote:
Well then, you need to consider when the static/quasi-static assumptions
fail. When does radiation become important? Is there any other
electromagnetic effect other than radiation that can make circuit theory
fail? Why or why not? There was a paper addressing some of this in the
last few months on this in Am. J. Phys., iirc, and there have been other
related papers in the past in the same journal.

As it's for assessment, the point is to show what you know and
_understand_, rather than what other people know (at least, it should be
the point!). For example, why do you choose a particular break point where
the circuit laws fail? What does this break point mean physically, beyond
being a usual engineering rule-of-thumb?

KVL is about how well a voltage (does this depend on gauge?) behaves as
you become non-electrostatic. KCL depends on how well you can talk about
"current in a wire", with non-static fields. How do you decide where to
choose a break-point?

--
Timo Nieminen - Home page:http://www.physics.uq.edu.au/people/nieminen/
E-prints:http://eprint.uq.edu.au/view/person/Nieminen,_Timo_A..html
Shrine to Spirits:http://www.users.bigpond.com/timo_nieminen/spirits.html
Benj
Posted: Thu Oct 11, 2007 1:27 pm
Guest
gianmaria.sandigli...@gmail.com wrote:
Quote:
Hi Timo,

My gratitude debt with you is every-day greater! :-D

You are right in all exept one thing. The assessment :-D

I'am 30, i can not study when it was time and i am studying now with
huge effort Razz
1- because i have lost a lot of physics grounds
2- because i have to share my time with family and work
So, now, assessment in not the real target of my study, i study
because i WANT

Doing things because they interest you is ALWAYS the best!

Quote:
My need of know what other people know is because the objective of my
essay is a
comparison of the ways used to define a break point that i tnink is
allready well know:
- the circuit laws start to fail when circuit's size are of same order
of magnitude of wavelength of signals we are using
Far from this condition we use circuits low. Under this condition we
have Microwave Engineering.

Sure, circuit theory and it's limitations ARE well known! But hey, do
understanding FIRST and math later. You sound to me like the guys who
ask for a bunch of references to scientific papers to tell them how to
put a new cord on a lamp! Go get some basic text books FIRST and read
them! You don't even know that Ohms law is just an experimental fact
which only holds approximately even in the best of conditions!

You have to understand what a circuit approximation is all about. KVC
is basically simple. It is nothing more than a statement of the fact
that integration about a loop in a CONSERVATIVE field gives zero. Note
that the field inside a battery is NOT conservative. Hence that part
does not work. You have to be able to derive the field from the
gradient of a scalar potential. Furthermore, the difference between
circuit and field theory goes WELL beyond radiation. For one thing in
circuit theory voltages and currents must be defined. In other words
circuits have terminals with defined voltages and currents. You
therefore have to have practical situations where at least
approximately voltages can be defined in this manner. When voltages
and currents are distributed throughout materials and vary they do NOT
define circuits and cannot be approximated by circuit theory.

The answer here is not "perturbation theory" or "quantum mechanics"
but good old understanding FIRST! OK? As Timo notes, to define the
borders of circuit theory is to define your ability to define
"terminals" with exact voltages and currents. The rest of the device
can be distributed (but not non-conservative) PROVIDED you can define
voltage and current at it's terminals. Note that radiation is not
necessarily a reason for circuit theory to fail. Antennas with
terminals are often modeled as circuit elements. Any circuit is filled
with electric and magnetic fields. The potentials and currents create
them. However, it is the goal of circuit theory to provide a quick and
dirty solution to some of the answers one seeks about the device
WITHOUT actually using those fields in a calculation. Clearly this is
NOT always possible. Your interest is in the borderland between where
it is and is not possible.

The problem is that everyday many people use circuit theory and field
theory but have pretty much forgotten how one is an approximation of
the other and the conditions necessary for that approximation to hold.
Guest
Posted: Fri Oct 12, 2007 4:51 am
I am really sorry Benj, but i think i have problems to explain my
point :-(

There is a brackpoint, you have defined circuit's low, but htere is
more...
Perturbation theory IS my point because give approximate solution to
maxwell's equation and at the
0 order i can find the "classical" explanation about integration about
a loop in a CONSERVATIVE field gives zero, ecc..
but at the highest order i find important solution in EMC study....
that is what i am searching...

sorry, i do not know the right way to explain myself Sad
it sound me like i ask you about pinapple and you asware me about
apple Sad((

I think that FIRST, before UNDERSTAND, is better impruve english :-P

GMS

On 11 Ott, 20:27, Benj <bjac...@iwaynet.net> wrote:

Quote:
Sure, circuit theory and it's limitations ARE well known!
[...]
The problem is that everyday many people use circuit theory and field
theory but have pretty much forgotten how one is an approximation of
the other and the conditions necessary for that approximation to hold.
Don Kelly
Posted: Sat Oct 13, 2007 1:16 am
Guest
----------------------------
<gianmaria.sandigliano@gmail.com> wrote in message
news:1192182679.245627.155860@i38g2000prf.googlegroups.com...
Quote:
I am really sorry Benj, but i think i have problems to explain my
point :-(

There is a brackpoint, you have defined circuit's low, but htere is
more...
Perturbation theory IS my point because give approximate solution to
maxwell's equation and at the
0 order i can find the "classical" explanation about integration about
a loop in a CONSERVATIVE field gives zero, ecc..
but at the highest order i find important solution in EMC study....
that is what i am searching...

sorry, i do not know the right way to explain myself Sad
it sound me like i ask you about pinapple and you asware me about
apple Sad((

I think that FIRST, before UNDERSTAND, is better impruve english :-P

GMS

On 11 Ott, 20:27, Benj <bjac...@iwaynet.net> wrote:

Sure, circuit theory and it's limitations ARE well known!
[...]
The problem is that everyday many people use circuit theory and field
theory but have pretty much forgotten how one is an approximation of
the other and the conditions necessary for that approximation to hold.
-----------

KVL simply means that if you go around the block and return to where you
start- you haven't gone anywhere. One of Maxwell's equations says the same
thing.
KCL: states that what goes in, comes out which is also stated by one of
Maxwell's equations.
The difference is that KVL and KCL are typically applied to specific paths
and junctions while Maxwell's equations are more general .
Because of the limitations of KVL and KCL to these specific paths as well as
ignoring factors other than induced voltages (actually KVL doesn't specify
(or care) why a voltage exists between two points in a circuit) , circuit
theory is considered a quasi-static approximation to Maxwell's equations
(i.e throw out the awkward terms)

Where does circuit theory fail and field theory is required?
a) where definite paths and nodes do not exist- i.e in RF transmission
b)where the circuit models necessarily become so complex that it is easier
to go directly to field models- eg wave guides.
c) and this is apparently what is wanted, where a given circuit model is
not accurate enough according to some subjective standard.
This is rather amorphous so that the determination of a once and for all
criterion is unlikely.

just my two bits worth
Don Kelly dhky@shawcross.ca
remove the X to answer

Quote:

 
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