Jump to content
Main menu
Main menu
move to sidebar
hide
Navigation
Main page
Recent changes
Random page
Help about MediaWiki
Special pages
Niidae Wiki
Search
Search
Appearance
Create account
Log in
Personal tools
Create account
Log in
Pages for logged out editors
learn more
Contributions
Talk
Editing
Electrical impedance
(section)
Page
Discussion
English
Read
Edit
View history
Tools
Tools
move to sidebar
hide
Actions
Read
Edit
View history
General
What links here
Related changes
Page information
Appearance
move to sidebar
hide
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
==History== Perhaps the earliest use of complex numbers in circuit analysis was by Johann Victor Wietlisbach in 1879 in analysing the [[Maxwell bridge]]. Wietlisbach avoided using differential equations by expressing AC currents and voltages as [[exponential function]]s with [[imaginary number|imaginary]] exponents (see {{section link|#Validity of complex representation}}). Wietlisbach found the required voltage was given by multiplying the current by a complex number (impedance), although he did not identify this as a general parameter in its own right.<ref>Kline, Ronald R., ''Steinmetz: Engineer and Socialist'', Johns Hopkins University Press, 1992 {{isbn|9780801842986}}, p. 78.</ref> The term ''impedance'' was coined by [[Oliver Heaviside]] in July 1886.<ref>''Science'', p. 18, 1888{{Full citation needed|date=March 2023}}{{failed verification|date = January 2024}}</ref><ref>Oliver Heaviside, ''The Electrician'', p. 212, 23 July 1886, reprinted as ''Electrical Papers, Volume II'', p 64, AMS Bookstore, {{ISBN |0-8218-3465-7}}</ref> Heaviside recognised that the "resistance operator" (impedance) in his [[operational calculus]] was a complex number. In 1887 he showed that there was an AC equivalent to [[Ohm's law]].<ref>Kline, p. 79.</ref> [[Arthur Kennelly]] published an influential paper on impedance in 1893. Kennelly arrived at a complex number representation in a rather more direct way than using imaginary exponential functions. Kennelly followed the graphical representation of impedance (showing resistance, reactance, and impedance as the lengths of the sides of a right angle triangle) developed by [[John Ambrose Fleming]] in 1889. Impedances could thus be added [[Vector (mathematics and physics)|vectorially]]. Kennelly realised that this graphical representation of impedance was directly analogous to graphical representation of complex numbers ([[Argand diagram]]). Problems in impedance calculation could thus be approached algebraically with a complex number representation.<ref>Kline, p. 81-2.</ref><ref>Kennelly, Arthur,[https://archive.org/details/transactionsame31engigoog/page/175/mode/1up "Impedance"], ''Transactions of the American Institute of Electrical Engineers'', vol. 10, pp. 175β232, 18 April 1893.</ref> Later that same year, Kennelly's work was generalised to all AC circuits by [[Charles Proteus Steinmetz]]. Steinmetz not only represented impedances by complex numbers but also voltages and currents. Unlike Kennelly, Steinmetz was thus able to express AC equivalents of DC laws such as Ohm's and Kirchhoff's laws.<ref>Kline, p. 85.</ref> Steinmetz's work was highly influential in spreading the technique amongst engineers.<ref>Kline, p. 90-1.</ref>
Summary:
Please note that all contributions to Niidae Wiki may be edited, altered, or removed by other contributors. If you do not want your writing to be edited mercilessly, then do not submit it here.
You are also promising us that you wrote this yourself, or copied it from a public domain or similar free resource (see
Encyclopedia:Copyrights
for details).
Do not submit copyrighted work without permission!
Cancel
Editing help
(opens in new window)
Search
Search
Editing
Electrical impedance
(section)
Add topic