If you need assistance, please send an email to forum at 4hv dot org. To ensure your email is not marked as spam, please include the phrase "4hv help" in the subject line. You can also find assistance via IRC, at irc.shadowworld.net, room #hvcomm.
Support 4hv.org!
Donate:
4hv.org is hosted on a dedicated server. Unfortunately, this server costs and we rely on the help of site members to keep 4hv.org running. Please consider donating. We will place your name on the thanks list and you'll be helping to keep 4hv.org alive and free for everyone. Members whose names appear in red bold have donated recently. Green bold denotes those who have recently donated to keep the server carbon neutral.
Special Thanks To:
Aaron Holmes
Aaron Wheeler
Adam Horden
Alan Scrimgeour
Andre
Andrew Haynes
Anonymous000
asabase
Austin Weil
barney
Barry
Bert Hickman
Bill Kukowski
Blitzorn
Brandon Paradelas
Bruce Bowling
BubeeMike
Byong Park
Cesiumsponge
Chris F.
Chris Hooper
Corey Worthington
Derek Woodroffe
Dalus
Dan Strother
Daniel Davis
Daniel Uhrenholt
datasheetarchive
Dave Billington
Dave Marshall
David F.
Dennis Rogers
drelectrix
Dr. John Gudenas
Dr. Spark
E.TexasTesla
eastvoltresearch
Eirik Taylor
Erik Dyakov
Erlend^SE
Finn Hammer
Firebug24k
GalliumMan
Gary Peterson
George Slade
GhostNull
Gordon Mcknight
Graham Armitage
Grant
GreySoul
Henry H
IamSmooth
In memory of Leo Powning
Jacob Cash
James Howells
James Pawson
Jeff Greenfield
Jeff Thomas
Jesse Frost
Jim Mitchell
jlr134
Joe Mastroianni
John Forcina
John Oberg
John Willcutt
Jon Newcomb
klugesmith
Leslie Wright
Lutz Hoffman
Mads Barnkob
Martin King
Mats Karlsson
Matt Gibson
Matthew Guidry
mbd
Michael D'Angelo
Mikkel
mileswaldron
mister_rf
Neil Foster
Nick de Smith
Nick Soroka
nicklenorp
Nik
Norman Stanley
Patrick Coleman
Paul Brodie
Paul Jordan
Paul Montgomery
Ped
Peter Krogen
Peter Terren
PhilGood
Richard Feldman
Robert Bush
Royce Bailey
Scott Fusare
Scott Newman
smiffy
Stella
Steven Busic
Steve Conner
Steve Jones
Steve Ward
Sulaiman
Thomas Coyle
Thomas A. Wallace
Thomas W
Timo
Torch
Ulf Jonsson
vasil
Vaxian
vladi mazzilli
wastehl
Weston
William Kim
William N.
William Stehl
Wesley Venis
The aforementioned have contributed financially to the continuing triumph of 4hv.org. They are deserving of my most heartfelt thanks.
Registered Member #54278
Joined: Sat Jan 17 2015, 04:42AM
Location: Amite, La.
Posts: 367
This thread shares valuable knowledge (to me...) as it progresses: I pay close attention to all replys and learn from them--I also look forward to more...
Here are two short segments of (I think, the same) MIT lecture that appeared to illustrate (with an actual demonstration circuit (at the end of part 2) this Faraday vs Kirchhoff 'phenomenon'.
part 1:
part 2:
I am still searching for that 'detailed supplement' but can't seem to find it on the MIT page. I will post it when I find it. I saw it a couple year's ago, so I know it is out there--it is convincing--certainly to the students!
BTW: at the start of part 2, when he mentions 100 and 900 "VOLT" components, he actually means "OHMS".
Registered Member #834
Joined: Tue Jun 12 2007, 10:57PM
Location: Brazil
Posts: 644
Complex impedances are just an algebraic representation of what happens when the voltages and currents are all in sinusoidal steady state. Of course Kirchhoff's laws apply there, but that analysis can't be applied directly in transient waveforms, where Kirchhoff's laws also apply, as long as the assumption of a lumped circuit is valid.
In the MIT lecture the circuit is made with a loop of wire around the central solenloid interrupted by the two resistors, and the oscilloscope reads the voltages over the resistors with the ground connection between both. The outcome is perfectly correct, since the loop of wire forms a transformer with the solenoid. The "missing" voltage source is over the loop, induced by the solenoid switching. Care must be taken to route properly the connections to the oscilloscope, otherwise the coupling to the leads may be significant too.
Registered Member #3414
Joined: Sun Nov 14 2010, 05:05PM
Location: UK
Posts: 4245
Signification wrote ...
Here are two short segments of (I think, the same) MIT lecture that appeared to illustrate (with an actual demonstration circuit (at the end of part 2) this Faraday vs Kirchhoff 'phenomenon'.
The results obtained are exactly what you'd expect from this circuit:
(I forgot to add the resistor values, 100 Ohm on the left, and 900 Ohm on the right, the same as in the demo.)
In the previous demonstration (the first video) the 1 volt source was across the meter as well as the 100 Ohm resistor. In the second demonstration, it's obviously not measured by either meter, as it's an induced voltage that is induced around the whole loop.
***** Emf = closed path integral of E•dl = - L di/dt (NOT 0) ***** THIS IS THE GENERAL LAW OF FARADAY:
EDIT: Not quite. Faradays law relates the E*dl path integral to the flux change dphi/dt.
Why not just use this whenever an inductor is (or is not) in the loop and settle for the right answer obtained every time and in a valid way. AND, unlike several applications in other fields, where such an argument leads to non-classical techniques to get the "exact / precise / perfect" answer is impractical, here it is no more difficult.
Actually it is more difficult to do it this way. Consider an inductor and other components wired in a loop. Applying Faradays law to all of this would require to calculate the flux inside the inductor and also inside the circuit loop. The field inside the inductor will be affected by its core and you also will need a specification of its geometry, i.e. turns, diameter etc. Also some of the inductors field will spill into the circuit loop contributing to the emf. This involves solving Maxwells equations for the whole circuit and in practice, nobody goes into the pain of doing this.
You can get a nearly accurate result by simply reading off the inductance value printed on the inductor, neglect the inductance of the circuit loop and apply Kirchhoffs law.
Registered Member #54278
Joined: Sat Jan 17 2015, 04:42AM
Location: Amite, La.
Posts: 367
Uspring wrote ...
Signification wrote:
***** Emf = closed path integral of E•dl = - L di/dt (NOT 0) ***** THIS IS THE GENERAL LAW OF FARADAY:
EDIT: Not quite. Faradays law relates the E*dl path integral to the flux change dphi/dt.
The relation which I think is the most important (which maybe I should have written) is the one that relates the "CLOSED PATH" circuit integral with the connecting "OPEN SURFACE" B-field integral, namely:
closed loop integral of E•dl = d/dt of the open surface integral B•dA ( I think I got that right--end of a rough day / night )
Things seem to start with Oersted's: Φ proportional to i
The remainder of your msg is sort of what I have been waiting to see, an illustrating example...I intend to 'work it out' in some detail...
Registered Member #2529
Joined: Thu Dec 10 2009, 02:43AM
Location:
Posts: 600
Antonio wrote ...
Complex impedances are just an algebraic representation of what happens when the voltages and currents are all in sinusoidal steady state. Of course Kirchhoff's laws apply there, but that analysis can't be applied directly in transient waveforms, where Kirchhoff's laws also apply, as long as the assumption of a lumped circuit is valid.
Transients are no problem. You just do Fourier analysis; and it all falls out, (at least, provided it's linear.)
If it's not linear, Kirchoff's laws still apply, as a limit case, but you have to use an iterative process, which may not necessarily entirely follow Kirchoff, but any deviations are errors in the process; variations from what the real circuit will do (provided there's no unmodelled strays).
It's only really the strays that mess up Kirchoff, it's not an incorrect model of reality per se.
This site is powered by e107, which is released under the GNU GPL License. All work on this site, except where otherwise noted, is licensed under a Creative Commons Attribution-ShareAlike 2.5 License. By submitting any information to this site, you agree that anything submitted will be so licensed. Please read our Disclaimer and Policies page for information on your rights and responsibilities regarding this site.