An induction coil or "spark coil" (archaically known as an inductorium or Ruhmkorff coil after Heinrich Ruhmkorff) is a type of electrical transformer used to produce high-voltage pulses from a low-voltage direct current (DC) supply. To create the flux changes necessary to induce voltage in the secondary coil, the direct current in the primary coil is repeatedly interrupted by a vibrating mechanical contact called an interrupter. Invented in 1836 by Nicholas Callan, with additional research by Charles Grafton Page and others, the induction coil was the first type of transformer. It was widely used in x-ray machines, spark-gap radio transmitters, arc lighting and quack medical electrotherapy devices from the 1880s to the 1920s. Today its only common use is as the ignition coils in internal combustion engines and in physics education to demonstrate induction.
Construction and function
See schematic diagram. An induction coil consists of two coils of insulated copper wire wound around a common iron core (M). One coil, called the primary winding (P), is made from relatively few (tens or hundreds) turns of coarse wire. The other coil, the secondary winding, (S) typically consists of many (thousands) turns of fine wire.
An electric current is passed through the primary, creating a magnetic field. Because of the common core, most of the primary's magnetic field couples with the secondary winding. The primary behaves as an inductor, storing energy in the associated magnetic field. When the primary current is suddenly interrupted, the magnetic field rapidly collapses. This causes a high voltage pulse to be developed across the secondary terminals through electromagnetic induction. Because of the large number of turns in the secondary coil, the secondary voltage pulse is typically many thousands of volts. This voltage is often sufficient to cause an electric spark, to jump across an air gap (G) separating the secondary's output terminals. For this reason, induction coils were called spark coils.
The size of induction coils is usually specified by the length of spark it can produce; a '4 inch' (10 cm) induction coil is one that could produce a 4 inch spark. This form of specification was, though imprecise, until the advent of the cathode ray oscilloscope the most reliable measure of peak voltage of such asymmetric waveforms. The relationship between spark length and voltage is linear:
- 4 inches (10 cm) = 110kV ; 8 inches (20 cm) = 150kV ; 12 inches (30 cm) = 190kV ; 16 inches (41 cm) = 230kV
To operate the coil continually, the DC supply current must be repeatedly connected and disconnected to create the magnetic field changes needed for induction. To do that, induction coils use a magnetically activated vibrating arm called an interrupter or break (A) to rapidly connect and break the current flowing into the primary coil. 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 voltage v2 (red, left), is roughly proportional to the rate of change of primary current i1 (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.
An arc forms at the interrupter contacts at 'break' which consumes energy stored in the coil, slowing the rate of change of primary current, reducing the output voltage. To prevent this a capacitor (C) of 0.5 to 15 μF is connected across the contacts to increase the speed of switching on 'break', producing much higher voltages.[dubious ] It also prevents damage to the contacts by the arc. The capacitor and primary winding together form a tuned circuit, so on break an oscillating decaying sinusoidal current flows in the primary.[dubious ] This induces a sinusoidal voltage in the secondary. As a result: the high voltage output pulse at each break actually consists of a rapidly alternating series of positive and negative pulses (left) which decay rapidly to zero.
To prevent the high voltages generated in the coil from breaking down the thin insulation and arcing between 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 in series. The primary coil is first wound on the iron core and insulated from the secondary with a thick paper or rubber coating. 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. 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 melted paraffin wax or rosin; 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 prevent eddy currents, which cause energy losses, the iron core is made of a bundle of parallel iron wires, individually coated with shellac to insulate them electrically. 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
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 in spark-gap radio transmitters and x-ray machines around the turn of the 20th century. In powerful coils the high primary current created arcs at the interrupter contacts which quickly destroyed the contacts. 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. Léon Foucault and others developed interrupters consisting of an oscillating needle dipping into and out of a container of mercury. 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, 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. The electrolytic or Wehnelt interrupter, invented by Arthur Wehnelt in 1899, consisted of a short platinum needle anode immersed in an electrolyte of dilute sulfuric acid, with the other side of the circuit connected to a lead plate cathode. 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 the hydrogen could explode. Mercury turbine interrupters had a centrifugal pump which sprayed a stream of liquid mercury onto rotating metal contacts. 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.
The induction coil was the first type of electrical transformer. 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 reduce eddy current losses.
Michael Faraday discovered the principle of induction, Faraday's induction law, in 1831 and did the first experiments with induction between coils of wire. The induction coil was invented by the American physician Charles Grafton Page in 1836 and independently by Irish scientist and Catholic priest Nicholas Callan in the same year at the St. Patrick's College, Maynooth and improved by William Sturgeon. George Henry Bachhoffner and Sturgeon (1837) independently discovered that a "divided" iron core of iron wires reduced power losses. The early coils had hand cranked interrupters, invented by Callan and Antoine Philibert Masson (1837). The automatic 'hammer' interrupter was invented by Rev. Prof. James William MacGauley (1838) of Dublin, Ireland, Johann Philipp Wagner (1839), and Christian Ernst Neeff (1847). Hippolyte Fizeau (1853) introduced the use of the quenching capacitor. Heinrich Ruhmkorff generated higher voltages by greatly increasing the length of the secondary, in some coils using 5 or 6 miles (10 km) of wire and produced sparks up to 16 inches. In the early 1850s, American inventor Edward Samuel Ritchie introduced the divided secondary construction to improve insulation. Jonathan Nash Hearder worked on induction coils. Callan's induction coil was named an IEEE Milestone in 2006.
Induction coils were used to provide high voltage for early gas discharge and Crookes tubes and other high voltage research. They were also used to provide entertainment (lighting Geissler tubes, for example) and to drive small "shocking coils", Tesla coils and violet ray devices used in quack medicine. They were used by Hertz to demonstrate the existence of electromagnetic waves, as predicted by James Clerk Maxwell and by Lodge and Marconi in the first research into radio waves. Their largest industrial use was probably in early wireless telegraphy spark-gap radio transmitters and to power early cold cathode x-ray tubes from the 1890s to the 1920s, after which they were supplanted in both these applications by AC transformers and vacuum tubes. However their largest use was as the ignition coil or spark coil in the ignition system of internal combustion engines, where they are still used, although the interrupter contacts are now replaced by solid state switches. A smaller version is used to trigger the flash tubes used in cameras and strobe lights.
- Ignition coil
- Trembler coil
- Spark gap transmitter
- Tesla coil
- Faraday's law of induction
- Ignition system
- Magnetic field
- Nicholas Callan
- John Archibald Fleming "Induction Coil". Encyclopædia Britannica, 11th Ed. 13. The Encyclopædia Britannica Co. 1911. pp. 502–505. Retrieved October 13, 2014.
- Collins, Archie F. (1908). The Design and Construction of Induction Coils. New York: Munn & Co. p.98
- Collins, 1908, p. iii
- Collins, 1908, p. 16-19
- Schall & Son Electro-medical Instruments and their Management London 1914
- Collins, 1908, p. 98
- Moore, Arthur (1911). How to make a wireless set. Chicago: The Popular Mechanics Co. ISBN 978-1440048746.
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.
- Faraday, Michael (1834). "Experimental Researches in Electricity. Seventh Series". Philosophical Transactions of the Royal Society of London. 124: 77–122. doi:10.1098/rstl.1834.0008.
- Page, 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.
- Czarnik, Stanley A. (March 1993). "The Classic Induction Coil" (PDF). Popular Electronics. 9 (3): 35–40. ISSN 1042-170X. Retrieved September 3, 2015., archived Archived 2016-10-30 at the Wayback Machine.
- Callan, N. J. (December 1836). "On a new galvanic battery". Philosophical Magazine. 9 (3): 472–478. doi:10.1080/14786443608649044. Retrieved February 14, 2013.
- Callan, N. J. A Description of an Electromagnetic Repeater in Sturgeon, 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
- Fleming, John Ambrose (1896). The Alternate Current Transformer in Theory and Practice, Vol. 2. London: The Electrician Publishing Co. pp. 16–18.
- McKeith, Niall. "Reverend Professor Nicholas Callan". National Science Museum. St. Patrick's College, Maynooth. Archived from the original on February 25, 2013. Retrieved February 14, 2013.
- Fleming (1896) The Alternate Current Transformer in Theory and Practice, Vol. 2, p. 10-11
- 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. Retrieved February 14, 2013. On page 458, an interrupter consisting of a toothed wheel is described.
- 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. Retrieved February 14, 2013.
- Masson, Antoine Philibert; Louis Breguet (1841). "Mémoire sur l'induction". Annales de Chimie et de Physique. 4 (3): 129–152. Retrieved February 14, 2013. On page 134, Masson describes the toothed wheels that functioned as an interrupter.
- 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
- Neeff, Christian Ernst (1839). "Ueber einen neuen Magnetelektromotor (On a new electromagnetic motor)". Annalen der Physik und Chemie. 46: 104–127. Retrieved February 14, 2013.
- 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. Retrieved February 14, 2013. Description of Neeff and Wagner's earlier toothed wheel interrupter
- 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. Retrieved February 14, 2013.
- Severns, Rudy. "History of soft switching, Part 2" (PDF). Design Resource Center. Switching Power Magazine. Archived from the original (PDF) on 2011-07-16. Retrieved 2008-05-16.
- 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
- 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
- Fleming, J. A. (1891). "The Historical Development of the Induction Coil and Transformer". The Electrician. 26–27: V26:–&ndash, 417, V27: 211&ndash, 213, 246&ndash, 248, 300&ndash, 302, 359&ndash, 361, 433&ndash, 435. at page 360.
- "Hearder's induction coil". Journal of the Franklin Institute. 63 (3): 179–81. 1857. doi:10.1016/0016-0032(57)90712-3.
- "The improved induction coil". Philosophical Magazine. Series 4. 13 (88): 471. 1857. doi:10.1080/14786445708642330.
- "The improved induction coil". Philosophical Magazine. Series 4. 14 (93): 319–20. 1857. doi:10.1080/14786445708642396.
- Hearder, Ian G. (September 2004). "Hearder, Jonathan Nash (1809–1876)". Oxford Dictionary of National Biography. Oxford University Press. Retrieved 7 April 2010.
- "Milestones:Callan's Pioneering Contributions to Electrical Science and Technology, 1836". IEEE Global History Network. IEEE. Retrieved 26 July 2011.
- Norrie, H. S., "Induction Coils: How to Make, Use, and Repair Them". Norman H. Schneider, 1907, New York. 4th edition.
- Collins, Archie F. (1908). The Design and Construction of Induction Coils. New York: Munn & Co.
- Fleming, John Ambrose (1896). The Alternate Current Transformer in Theory and Practice, Vol.2. The Electrician Publishing Co. Has detailed history of invention of induction coil
- Battery powered Driver circuit for Induction Coils
- The Cathode Ray Tube site
- Newman, F. H. (1921). "A New Form of Wehnelt Interrupter". Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences. 99 (699): 324–30. Bibcode:1921RSPSA..99..324N. doi:10.1098/rspa.1921.0045. JSTOR 93959.
- http://media.digikey.com/pdf/other%20related%20documents/panasonic%20other%20doc/small%20signal%20relay%20techincal%20info.pdf See section "Contact Protection – Counter EMF".
- https://web.archive.org/web/20161009151329/http://www.worldphaco.net/uploads/CAPACITIVE_DISCHARGE_IGNITION_vs_MAGNETIC_DISCHARGE_IGNITION..pdf See figure 9 for actual discharge.