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Induction coil

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This article is about the type oftransformerthat produces high-voltage pulses. For the more general electrical component, seeInductor.For the high-frequency heating coil, seeinduction heating.For the device in telephone sets, seehybrid coil.
Induction coil
Antique induction coil used in schools, from around 1900, Bremerhaven, Germany
TypeTransformer
Working principle‍Electromagnetic induction
InventedNicholas Callan
Charles G. Page(independently, 1836)
Induction coil showing construction, from 1920.

Aninduction coilor "spark coil" (archaicallyknown as aninductoriumorRuhmkorff coil[1]afterHeinrich Rühmkorff) is a type of electricaltransformer[2][3][4]used to produce high-voltage pulses from a low-voltagedirect current(DC) supply.[1][5]To create thefluxchanges necessary to induce voltage in the secondary coil, the direct current in the primary coil is repeatedly interrupted by a vibrating mechanicalcontactcalled aninterrupter.[1]Invented in 1836 by the Irish-Catholic priestNicholas Callan,also independently by American inventorCharles Grafton Page,[1]the induction coil was the first type of transformer. It was widely used inx-ray machines,[1][6]spark-gap radio transmitters,[1][6]arc lightingand quack medicalelectrotherapydevices from the 1880s to the 1920s. Today its only common use is as theignition coilsininternal combustion enginesand in physics education to demonstrateinduction.

Construction and function

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Schematic diagram

An induction coil consists of two coils of insulated wire wound around a commoniron core(M).[1][7]One coil, called theprimary winding(P),is made from relatively few (tens or hundreds) turns of coarse wire.[7]The other coil, thesecondary winding,(S)typically consists of up to a million turns of fine wire (up to 40 gauge).[8][1][7]

Anelectric currentis passed through the primary, creating amagnetic field.[1][7]Because of the common core, most of the primary's magnetic field couples with the secondary winding.[citation needed]The primary behaves as aninductor,storing energy in the associated magnetic field. When the primary current is suddenly interrupted, the magnetic field rapidly collapses. This causes ahigh voltagepulse to be developed across the secondary terminals throughelectromagnetic induction.Because of the large number of turns in the secondary coil, the secondary voltage pulse is typically many thousands ofvolts.This voltage is often sufficient to cause anelectric spark,to jump across an air gap(G)separating the secondary's output terminals. For this reason, induction coils were called spark coils.

An induction coil is traditionally characterised by the length of spark it can produce; a '4 inch' (10 cm) induction coil could produce a 4 inch spark. Until the development of thecathode ray oscilloscope,this was the most reliable measurement of peak voltage of such asymmetric waveforms. The relationship between spark length and voltage is linear within a wide range:

4 inches (10 cm) = 110kV; 8 inches (20 cm) = 150kV; 12 inches (30 cm) = 190kV; 16 inches (41 cm) = 230kV[9]

Curves supplied by a 1984 reference agree closely with those values.[10]

Interrupter

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Without capacitor
With capacitor
Waveforms in an induction coil with output open (no spark).i1(blue)is the current in the coil's primary winding,v2(red)is the voltage across the secondary. Not to common scale;v2is much larger in bottom drawing.[dubious–discuss]

To operate the coil continually, the DC supply current must be repeatedly connected and disconnected to create the magnetic field changes needed for induction.[1]To do that, induction coils use a magnetically activated vibrating arm called aninterrupterorbreak(A) to rapidly connect and break the current flowing into the primary coil.[1]The interrupter is mounted on the end of the coil next to the iron core. When the power is turned on, the increasing current in the primary coil produces an increasing magnetic field, the magnetic field attracts the interrupter's iron armature (A). After a time, the magnetic attraction overcomes the armature's spring force, and the armature begins to move. When the armature has moved far enough, the pair of contacts (K) in the primary circuit open and disconnect the primary current. Disconnecting the current causes the magnetic field to collapse and create the spark. Also, the collapsed field no longer attracts the armature, so the spring force accelerates the armature toward its initial position. A short time later the contacts reconnect, and the current starts building the magnetic field again. The whole process starts over and repeats many times per second. The secondary voltagev2(red,left), is roughly proportional to the rate of change of primary currenti1(blue).

Opposite potentials are induced in the secondary when the interrupter 'breaks' the circuit and 'closes' the circuit. However, the current change in the primary is much more abrupt when the interrupter 'breaks'. When the contacts close, the current builds up slowly in the primary because the supply voltage has a limited ability to force current through the coil's inductance. In contrast, when the interrupter contacts open, the current falls to zero suddenly. So the pulse of voltage induced in the secondary at 'break' is much larger than the pulse induced at 'close', it is the 'break' that generates the coil's high voltage output.

Capacitor

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An arc forms at the interrupter contacts on break which has undesirable effects: the arc consumes energy stored in the magnetic field, reduces the output voltage, and damages the contacts.[11]To prevent this, a quenchingcapacitor(C)of 0.5 to 15μFis connected across the primary coil to slow the rise in the voltage after a break. The capacitor and primary winding together form atuned circuit,so on break, adamped sinusoidal waveof current flows in the primary and likewise induces a damped wave in the secondary. As a result, the high voltage output consists of a series of damped waves(left).[citation needed]

Construction details

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To prevent the high voltages generated in the coil from breaking down the thininsulationandarcingbetween the secondary wires, the secondary coil uses special construction so as to avoid having wires carrying large voltage differences lying next to each other. In one widely used technique, the secondary coil is wound in many thin flat pancake-shaped sections (called "pies" ), connected inseries.[12][1]

The primary coil is first wound on the iron core and insulated from the secondary with a thick paper or rubber coating.[1]Then each secondary subcoil is connected to the coil next to it and slid onto the iron core, insulated from adjoining coils with waxed cardboard disks. The voltage developed in each subcoil isn't large enough to jump between the wires in the subcoil.[1]Large voltages are only developed across many subcoils in series, which are too widely separated to arc over. To give the entire coil a final insulating coating, it is immersed in meltedparaffin waxorrosin;the air evacuated to ensure there are no air bubbles left inside and the paraffin allowed to solidify, so the entire coil is encased in wax.

To preventeddy currents,which cause energy losses, the iron core is made of a bundle of parallel iron wires, individually coated withshellacto insulate them electrically.[1]The eddy currents, which flow in loops in the core perpendicular to the magnetic axis, are blocked by the layers of insulation. The ends of the insulated primary coil often protruded several inches from either end of the secondary coil, to prevent arcs from the secondary to the primary or the core.

Mercury and electrolytic interrupters

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(left)3-electrode Wehnelt interrupter used in high power coils.(right)Mercury turbine interrupter. The motor turns the toothed wheel while a stream of mercury is sprayed on the teeth. By adjusting the wheel up and down the duty cycle of the primary current can be changed.

Although modern induction coils used for educational purposes all use the vibrating arm 'hammer' type interrupter described above, these were inadequate for powering the large induction coils used inspark-gap radio transmittersandx-ray machinesaround the turn of the 20th century. In powerful coils the high primary current created arcs at the interrupter contacts which quickly destroyed the contacts.[1]Also, since each "break" produces a pulse of voltage from the coil, the more breaks per second the greater the power output. Hammer interrupters were not capable of interruption rates over 200 breaks per second and the ones used on powerful coils were limited to 20 – 40 breaks per second.

Therefore much research went into improving interrupters and improved designs were used in high power coils, with the hammer interrupters only used on small coils under 8 "sparks.[13]Léon Foucaultand others developed interrupters consisting of an oscillating needle dipping into and out of a container ofmercury.[1]The mercury was covered with a layer of spirits which extinguished the arc quickly, causing faster switching. These were often driven by a separate electromagnet or motor,[1]which allowed the interruption rate and "dwell" time to be adjusted separately from the primary current.

The largest coils used either electrolytic or mercury turbine interrupters.[1]The electrolytic or Wehnelt interrupter, invented byArthur Wehneltin 1899, consisted of a shortplatinumneedleanodeimmersed in anelectrolyteof dilutesulfuric acid,with the other side of the circuit connected to a lead platecathode.[1][14]When the primary current passed through it, hydrogen gas bubbles formed on the needle which repeatedly broke the circuit. This resulted in a primary current broken randomly at rates up to 2000 breaks per second. They were preferred for powering X-ray tubes. They produced a lot of heat and due to this the hydrogen could explode. Mercury turbine interrupters had acentrifugalpump which sprayed a stream of liquidmercuryonto rotating metal contacts.[1]They could achieve interruption rates up to 10,000 breaks per second and were the most widely used type of interrupter in commercial wireless stations.[1][14]

History

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Early coil byWilliam Sturgeon,1837. The sawtooth zinc interrupter wheel(D)was turned by hand. The first coil to use a divided core of iron wires(F)to prevent eddy currents.
Early coil by Charles G. Page, 1838, had one of the first automatic interrupters. The cup was filled with mercury. The magnetic field attracted the iron piece on the arm(left),lifting the wire out of the cup, breaking the primary circuit.
Induction coil byHeinrich Ruhmkorff,1850s. In addition to the hammer interrupter(right),it had a mercury interrupter by Fizeau(left)that could be adjusted to change the dwell time.
One of the largest coils ever constructed, built in 1877 by Alfred Apps for William Spottiswoode. Wound with 280 miles of wire, could produce a 42 in. (106 cm) spark, corresponding to roughly one million volts. Powered by 30 quart size liquid batteries and a separate interrupter(not shown).
The first induction coil, built by Nicholas Callan, 1836.

The induction coil was the first type of electricaltransformer.During its development between 1836 and the 1860s, mostly by trial and error, researchers discovered many of the principles that governed all transformers, such as the proportionality between turns and output voltage and the use of a "divided" iron core to reduceeddy currentlosses.

Michael Faradaydiscovered the principle of induction,Faraday's induction law,in 1831 and did the first experiments with induction between coils of wire.[15]The induction coil was invented by the American physicianCharles Grafton Pagein 1836[16][17]and independently by Irish scientist and Catholic priestNicholas Callanin the same year at theSt. Patrick's College, Maynooth[1][18][19][20][21]and improved byWilliam Sturgeon.[1]George Henry Bachhoffner[1]and Sturgeon (1837) independently discovered that a "divided" iron core of iron wires reduced power losses.[22]The early coils had hand cranked interrupters, invented by Callan and Antoine Philibert Masson (1837).[23][24][25]The automatic 'hammer' interrupter was invented by Rev. Prof.James William MacGauley(1838) of Dublin, Ireland,[16][26]Johann Philipp Wagner (1839), and Christian Ernst Neeff (1847).[1][27][28]Hippolyte Fizeau(1853) introduced the use of the quenching capacitor.[1][29][30]Heinrich Ruhmkorffgenerated higher voltages by greatly increasing the length of the secondary,[1]in some coils using 5 or 6 miles (10 km) of wire and produced sparks up to 16 inches. In the early 1850s, American inventorEdward Samuel Ritchieintroduced the divided secondary construction to improve insulation.[31][32]Jonathan Nash Hearderworked on induction coils.[33][34][35][36][37]Callan's induction coil was named anIEEE Milestonein 2006.[38]

Induction coils were used to provide high voltage for earlygas dischargeandCrookes tubesand other high voltage research. They were also used to provide entertainment (lightingGeissler tubes,for example) and to drive small "shocking coils",Tesla coilsandviolet raydevices used inquack medicine.They were used byHertzto demonstrate the existence of electromagnetic waves, as predicted byJames Clerk Maxwelland byLodgeandMarconiin the first research into radio waves. Their largest industrial use was probably in earlywireless telegraphyspark-gap radio transmittersand to power earlycold cathodex-ray tubesfrom the 1890s to the 1920s, after which they were supplanted in both these applications by ACtransformersandvacuum tubes.However their largest use was as theignition coilor spark coil in theignition systemofinternal combustion engines,where they are still used, although the interrupter contacts are now replaced bysolid stateswitches. A smaller version is used to trigger theflash tubesused in cameras andstrobelights.

Induction coil(top)powering 1915 wall mounted x-ray unit, with electrolytic interrupter(bottom).
Vibrator ignition coilused in early automobiles such as the Ford Model T around 1910
Modern automobileignition coil,the largest remaining use for induction coils

See also

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Footnotes

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  1. ^abcdefghijklmnopqrstuvwxyzaaabFleming, John Ambrose(1911)."Induction Coil".InChisholm, Hugh(ed.).Encyclopædia Britannica.Vol. 14 (11th ed.). Cambridge University Press. pp. 502–505.
  2. ^"Annus Mirabilis".The New Scientist.5(19). London: Reed Business Information: 445. February 1959.Retrieved20 November2018.[permanent dead link]
  3. ^Strickland, Jeffrey (2011).Weird Scientists: the Creators of Quantum Physics.Lulu. p. 98.ISBN978-1-257-97624-9.
  4. ^Waygood, Adrian (2016).Electrical Science for Technicians.Routledge. p. 162.ISBN978-1-317-53491-4.
  5. ^Collins, Archie F. (1908).The Design and Construction of Induction Coils.New York: Munn & Co. p.98.p.98
  6. ^abCollins, 1908, p. iii
  7. ^abcdCollins, 1908, p. 16-19
  8. ^Cyclopedia of Applied Electricity,American School of Correspondence, Chicago (1908), Electricity and Magnetism, 74. Induction coils.
  9. ^Schall, K. (1914).Electro-medical Instruments and their Management.Schall & Son London.
  10. ^E. Kuffel; W. S. Zaengl (1984).High Voltage Engineering.Pergamon Press. p. 374.ISBN0-08-024212-X.
  11. ^Schall, K. (1905).Electro-medical Instruments and their Management.Bemrose & Sons Ltd. Printers. pp.78.
  12. ^Schneider, Norman H. (1896).Ruhmkorff induction coils, their construction, operation and application.Spon & Chamberlain. pp.10-14, 16.
  13. ^Collins, 1908, p. 98
  14. ^abMoore, Arthur (1911).How to make a wireless set.Chicago: The Popular Mechanics Co.ISBN978-1-4400-4874-6.The electrolytic interrupter consists of a vessel containing a solution of dilute sulphuric acid with two terminals immersed in this solution. The positive terminal or anode is made of platinum and should have a surface of about 3/16 in.[sic] The negative terminal or cathode is made of lead and should have an area of something like 1 sq. ft. When this interrupter is connected in series with the primary of an induction coil and a source of electromotive force of about 40 volts, the circuit will be interrupted, due to the formation and collapse of bubbles on the platinum electrode.Page 31 describes electrolytic interrupter, but does not identify as Wehnelt interrupter.
  15. ^Faraday, Michael (1834). "Experimental Researches in Electricity. Seventh Series".Philosophical Transactions of the Royal Society of London.124:77–122.Bibcode:1834RSPT..124...77F.doi:10.1098/rstl.1834.0008.S2CID116224057.
  16. ^abPage, Charles Grafton (1867).History of Induction: The American Claim to the Induction Coil and Its Electrostatic Developments.Washington, D.C.: Intelligencer Printing House. pp.26–27, 57.
  17. ^Czarnik, Stanley A. (March 1993)."The Classic Induction Coil"(PDF).Popular Electronics.9(3): 35–40.ISSN1042-170X.RetrievedSeptember 3,2015.,archivedArchived2016-10-30 at theWayback Machine
  18. ^Callan, N. J. (December 1836)."On a new galvanic battery".Philosophical Magazine.9(3): 472–478.doi:10.1080/14786443608649044.RetrievedFebruary 14,2013.
  19. ^Callan, N. J.A Description of an Electromagnetic RepeaterinSturgeon, Ed., William (1837).The Annals of Electricity, Magnetism, and Chemistry, Vol. 1.London: Sherwood, Gilbert, and Piper. pp. 229–230.and p.522 fig. 52
  20. ^Fleming, John Ambrose (1896).The Alternate Current Transformer in Theory and Practice, Vol. 2.London: The Electrician Publishing Co. pp. 16–18.
  21. ^McKeith, Niall."Reverend Professor Nicholas Callan".National Science Museum.St. Patrick's College, Maynooth. Archived fromthe originalon February 25, 2013.RetrievedFebruary 14,2013.
  22. ^Fleming (1896)The Alternate Current Transformer in Theory and Practice, Vol. 2,p. 10-11
  23. ^Masson, Antoine Philibert (1837)."Rapport sur plusieurs mémoires, relatifs à un mode particulier d'action des courants électriques (Report on several memoirs regarding a particular mode of action of electric currents)".Comptes Rendus.4:456–460.RetrievedFebruary 14,2013.On page 458, an interrupter consisting of a toothed wheel is described.
  24. ^Masson, A. (1837)."De l'induction d'un courant sur lui-même (On the induction of a current in itself)".Annales de Chimie et de Physique.66:5–36.RetrievedFebruary 14,2013.
  25. ^Masson, Antoine Philibert; Louis Breguet (1841)."Mémoire sur l'induction".Annales de Chimie et de Physique.4(3): 129–152.RetrievedFebruary 14,2013.On page 134, Masson describes the toothed wheels that functioned as an interrupter.
  26. ^McGauley, J. W. (1838). "Electro-magnetic apparatus for the production of electricity of high intensity".Proceedings of the British Association for the Advancement of Science.7:25.presented at meeting of September 1837 in Liverpool, England
  27. ^Neeff, Christian Ernst (1839)."Ueber einen neuen Magnetelektromotor (On a new electromagnetic motor)".Annalen der Physik und Chemie.46:104–127.RetrievedFebruary 14,2013.
  28. ^Neeff, C. (1835)."Das Blitzrad, ein Apparat zu rasch abwechselnden galvanischen Schliessungen und Trennungen (The spark wheel, an apparatus for rapidly alternating closings and openings of galvanic circuits)".Annalen der Physik und Chemie.36:352–366.RetrievedFebruary 14,2013.Description of Neeff and Wagner's earlier toothed wheel interrupter
  29. ^Fizeau, H.(1853)."Note sur les machines électriques inductives et sur un moyen facile d'accroître leurs effets"[Note on electric induction machines and on an easy way to increase their effects].Comptes Rendus(in French).36:418–421.RetrievedFebruary 14,2013.
  30. ^Severns, Rudy."History of soft switching, Part 2"(PDF).Design Resource Center.Switching Power Magazine. Archived fromthe original(PDF)on 2011-07-16.Retrieved2008-05-16.
  31. ^American Academy of Arts and Sciences,Proceedings of the American Academy of Arts and Sciences,Vol. XXIII, May 1895 - May 1896, Boston: University Press, John Wilson and Son (1896), pp. 359-360
  32. ^Page, Charles G.,History of Induction: The American Claim to the Induction Coil and Its Electrostatic Developments,Washington, D.C.: Intelligencer Printing House (1867),pp. 104-106
  33. ^Fleming, J. A.(1891)."The Historical Development of the Induction Coil and Transformer".The Electrician.26–27: V26:––417, V27: 211–213, 246–248, 300–302, 359–361, 433–435.at page 360.
  34. ^"Hearder's induction coil".Journal of the Franklin Institute.63(3): 179–81. 1857.doi:10.1016/0016-0032(57)90712-3.
  35. ^"The improved induction coil".Philosophical Magazine.Series 4.13(88): 471. 1857.doi:10.1080/14786445708642330.
  36. ^"The improved induction coil".Philosophical Magazine.Series 4.14(93): 319–20. 1857.doi:10.1080/14786445708642396.
  37. ^Hearder, Ian G. (September 2004)."Hearder, Jonathan Nash (1809–1876)".Oxford Dictionary of National Biography.Oxford University Press.Retrieved7 April2010.
  38. ^"Milestones:Callan's Pioneering Contributions to Electrical Science and Technology, 1836".IEEE Global History Network.IEEE.Retrieved26 July2011.

Further reading

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