Home |
Search |
Today's Posts |
#11
![]() |
|||
|
|||
![]()
"Tdonaly" wrote in message
... Steve's info will get you a beginners understanding of circuit theory That WAS the intent. which is based on a low-frequency, quasi-static simplification of electromagnetic theory. Yikes! Call it what you like. Unfortunately, anything that has any appreciable length, such as a transmission line or an antenna... wave mechanics to get any real idea of what is happening in these situations. I guess you can call it "wave mechanics" if you like, but it IS true that what happens on a transmission line is waves and this is quite different from simple circuit theory. First you need the circuit theory, though. That isn't the end of it, though, since in order to understand what is happening when an object radiates, you have to understand Maxwell's equations....vector calculus. This I'll disagree with. It's been so long since I studied Maxwell's equations, I can't even spell his name, but I can give a workable explanatin of radiation that the beginner can understand and won't cause trouble for any ham's purposes. Will it violate old Maxwell? I don't know and don't care for my purposes and 90% of the people interested. That isn't the end, either, but it's as close as any *normal* human wants to go. Whew! sure glad I'm *abnormal*. Whenever someone who was taught circuit theory tries to apply its vocabulary and concepts to explain all electromagnetic phenomena, that someone is going to run into trouble and come up with a multitude of idiocies for which which he'll find no end of people ready to criticize him. Whoa... Sure glad I'm not trying to do THAT! This is the problem: Cecil and Yuri want to explain the current taper through a long solenoidal coil using the vocabulary and concepts of circuit theory rather than the difficult but more precise language of electromagnetic theory. Sure glad I don't care and that I didn't tack my post onto theirs thus indicating that I was trying to enter that discussion. 73 Steve-- Steve N, K,9;d, c. i My email has no u's. |
#12
![]() |
|||
|
|||
![]()
Well, then there's that too..
-- (:-) Steve N, K,9;d, c. i My email has no u's. "Butch" wrote in message ... Time out!! You people are taking all this far to seriously. Just throw an aerial out the window, feed it to your rig via a tuner, and enjoy Amateur radio. Butch Magee KF5DE Tdonaly wrote: Steve's info will get you a beginners understanding ... ...quasi-static. ...electromagnetic theory. ... ...wave mechanics... ...Maxwell's equations.... ...vector calculus. ...any *normal* human... ...multitude of idiocies ...no end of people ready to criticize him. |
#13
![]() |
|||
|
|||
![]()
Oh yea! that too... I forgot "Maxwell"
-- Steve N, K,9;d, c. i My email has no u's. "Ed Price" wrote in message news:YFmZb.5138$C21.2768@fed1read07... "Butch" wrote in message ... Time out!! You people are taking all this far to seriously. Just throw an aerial out the window, feed it to your rig via a tuner, and enjoy Amateur radio. Butch Magee KF5DE It just not that simple, Butch. I'm sure you have heard that Ham radio is a hobby that has many facets; construction, public service, contesting, field trips, QRP DX, etc. Some of our members get their kicks merging theory with rag chewing. I don't think there's any structure to this sub-category, other than to require at least one mention of Maxwell in every discussion. Ed WB6WSN |
#14
![]() |
|||
|
|||
![]()
Peter, K1PO wrote:
"Oliver heaviside was a poor kid from the London slums who had to go out to work at age 16 and never saw the inside of a college or university." I am aware of Heaviside`s story. He was the idol of one of my professors who frerquently regaled us with heaviside stories, so he became one of my favorites too. Maxwell is not diminished by his advantages. He had the mathematical background he needed to formulate his equations and the moxie to speculate that displacement current generates a magnetic field same as a conduction current does. This is the secret of radiation. Heaviside was able to improve on the calculus, and simplify and reorganize Maxwell`s work. Michael Faraday discovered electromagnetic induction and deserves a lot of credit too. Everybody benefits from the work of others in complicated fields. Faraday lived 1791-1867. Maxwell lived 1831-1879. Heaviside lived 1850-1925. This really was during a golden age for the British. I had the Maxwell`s equations course many decades ago. Strangely enough, it was titled "Ultra High Frequency Techniques". You really had to read the syllabus to know what the course was about. Best regards, Richard Harrison, KB5WZI |
#15
![]() |
|||
|
|||
![]()
Jerry Martes wrote:
"I have never been convinced that "impedance" is the ratio of force to response in any media." Jerry framed the question very nicely. The logic seems simple. More force is required when resistance to change is higher. When current is very small despite high force, it must be due to high resistance. Resistance proportional to force (volts) and inversely proportional to current (amps) seems perfectly logical to me. R=E/I Best regards, Richard Harrison, KB5WZI |
#16
![]() |
|||
|
|||
![]()
Art, KB9MZ wrote:
"The dipole is a very inefficient radiator." Kraus, unfortunately, wasn`t one of my books until recently. I don`t have the words memorized or know where they appear as I do with some of Terman. I seem to remember Kraus saying 95% efficiency was not unusual as a dipole efficiency. As there are so many variations, it`s like a baseball statistic, there must be a statistic that fits somewhere. In any case, "efficient" is only as compared with similar devices. Recall that dBd is the norm as an isotropic antenna is only a theoretical creature. Catalogs are filled with antenna characteristics as compared with a 1/2-wave dipole in free space. It is the standard of comparison. It could hardly be correctly called inefficient. Best regards, Richard Harrison, KB5WZI |
#17
![]() |
|||
|
|||
![]()
Yep!! Very Good Coffee!!!!!!!!!!!
Steve Nosko wrote: Oh yea! that too... I forgot "Maxwell" |
#18
![]() |
|||
|
|||
![]()
I just love it when those born in the slums of London even tho they went to
work when they were 16 they had enough smarts to go head to head with the experts. It must be a result of the morning fog from the river where one learns quickly what is real and what is not. Going to work for a living at 16 is not all that bad since it allows you to make personal decisions that can benefit before the onset of age makes it too late. An East Ender Art "Peter O. Brackett" wrote in message news ![]() Richard: Hmmm.... Impedance... let's give it its' proper due! It was the self taught "electrician", and ultimately Fellow of the Royal Society, Oliver Heaviside, FRS [1850 - 1925] who was born in the London slums to a very poor family and who had never attended any school beyond the age of 16 who was the person who coined, defined and first used the terms "impedance", "admittance", and "reactance". Oliver Heaviside also gave us Maxwell's Equations in the form we now know them. Maxwell wrote his equations in the form of 22 separate equations using the arcane method of "quaternions". Heaviside simplified those 22 equations given by Maxwell down to the four simple equations with two auxilliary constituent relations that we now know and love. James Clerk Maxwell was a Cambridge educated mathematician from an affluent and educated family. Oliver Heaviside was a poor kid from the London slums who had to go out to work at age 16 and never saw the inside of a college or university! Heaviside never appeared to receive the citation at the ceremony to which he was invited when he was inducted as a Fellow of the Royal Society after he was duly elected to that lofty title by the greatest Scientists of the day. "Impedance"... thank you Oliver! -- Peter K1PO Indialantic By-the-Sea, FL "Richard Harrison" wrote in message ... Steve Nosko wrote: "Apparently, because of the way the big bang occurred, when we put a voltage across a resistor current flows in a manner that we discovered follows the equation called Ohm`s law." Big bang? Ohm wasn`t around then. He lived 1787 to 1854. Ohm discovered that current in an electrical resistance is proportional to voltage. Resistance is the type of impedance (opposition to electrical current) in which current is locked in step to the applied voltage. The item called a resistor is the type of resistance that converts electrical energy to heat energy. Not all resistances are resistors. Some resistances don`t convert electrical energy directly into heat. In these non-dissipative resistances, current drop is in-phase with the applied volts, or voltage dropped across the resistance is in-phase with current through the resistance, but it does not cause energy loss. An example of lossless resistance is the Zo or surge impedance of a transmission line. Zo is caused by the distributed inductance and capacitance of the line, but current in the line is in-phase with the voltage across the line. Zo is the voltage to current ratio of the waves traveling in either direction on the transmission line. Zo = volts/amps, yet converts no energy to heat in the lossless line. Another example of lossless resistance is "radiation resistance". This is the desired antenna load, so it is hardly a loss. Loss in the wire, earth, and insulators of the antenna are resistive loads which produce heat but don`t help the signal. An ohm is the unit of resistance. It is defined at 0-degrees C, of a uniform column of mercury 106.300 cm long and weighing 14.451 grams. One ohm is the resistance which drops one voltt when a current of one amp is passed through it. Reactances are also defined by their volts to amps ratios (ohms). The big difference is that reactance does no work and produces no heat. Opposition to electrical current comes from delay required to store ard retrieve energy to and from fields in and around the reactances. Current lags the applied voltage in an inductance. At time = 0, no current flows into an inductance, but rises exponentially from the instant of initial energization. Current leads the applied voltage into a capacitance. At time = 0, full current flows into a capacitance but voltage across the capacitance is zero and rises exponentially from the instant of initial energization. In an a-c circuit, the current through an inductance lags the voltage by 90-degrees. In a a-c circuit, the current through a capacitance leads the voltage by 90-degrees. Phase shifts are produced by energy storage in reactance. There is no phase shift in a resistance. No electrical energy is stored in a resistor, but its matter does have a thermal capacity. Once its atoms are agitated by heat their inertia is evident in the resistance`s temperature. It takes time to cool. Steve wrote: "Things get all messed up." As old Carson Robinson sang: "Life gets tedious, Don`t it?" Steve gave the formulas for capacitive and inductive reactances. They have always seemed convenient to me. Steve says: "---we call this new kind of (corrupted) resistance "Impedance"." No. Impedance is the general name for opposition to electricity. Resistance is the specialized name for the case in which the impedance alone causes no delay and stores no electrical energy. All electrical impedance is defined by its voltage to current ratio, and is the total opposition (resistance and reactance) a circuit offers to the flow of electricity. For d-c, reactance doesn`t count. For a-c, total opposition consists of the vector (phasor) sum of resistance and reactance in a circuit. Impedance is measured in ohms and its reciprocal is called admittance. The symbol for impedance is Z. The symbol for admittance is Y. Steve also writes: "Poof! BUT converts it into radio frequency energy (RF) also called an electromagnetic field or wave." Yes. A radio wave is r-f energy which has escaped the confines of wires and doesn`t come back. Whenever wires in open space carry high-frequency current, some energy gets away as a radiated field, having a strength that varies inversely with the distance. Best regards, Richard Harrison, KB5WZI |
#19
![]() |
|||
|
|||
![]() |
#20
![]() |
|||
|
|||
![]()
Richard Harrison wrote:
Art, KB9MZ wrote: "The dipole is a very inefficient radiator." I seem to remember Kraus saying 95% efficiency was not unusual as a dipole efficiency. I don't think that's the efficiency that Art is talking about. Art's efficiency seems to be defined as the power delivered to the receiver divided by the power sourced by the transmitter. -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
Reply |
Thread Tools | Search this Thread |
Display Modes | |
|
|
![]() |
||||
Thread | Forum | |||
Mobile Ant L match ? | Antenna | |||
A Subtle Detail of Reflection Coefficients (but important to know) | Antenna | |||
Reflection Coefficient Smoke Clears a Bit | Antenna | |||
Length of Coax Affecting Incident Power to Meter? | Antenna | |||
50 Ohms "Real Resistive" impedance a Misnomer? | Antenna |