Editing Electrostatic induction

{{Short description|Separation of electric charge due to presence of other charges}}
{{distinguish|Electromagnetic induction}}
{{Electromagnetism|cTopic=Electrostatics}}
'''Electrostatic induction''', also known as "electrostatic influence" or simply "influence" in Europe and Latin America, is a redistribution of [[electric charge]] in an object that is caused by the influence of nearby charges.<ref name="BritannicaOnline">{{cite encyclopedia
  | title = Electrostatic induction
  | encyclopedia = Britannica.com Online
  | publisher = Britannica.com Inc.
  | year = 2008
  | url = http://www.britannica.com/eb/article-9032344/electrostatic-induction
  | access-date = 2008-06-25}}</ref>  In the presence of a charged body, an insulated conductor develops a positive charge on one end and a negative charge on the other end.<ref name="BritannicaOnline" />   Induction was discovered by British scientist [[John Canton]] in 1753 and Swedish professor [[Johan Carl Wilcke]] in 1762.<ref name="Britannica">{{Cite EB1911|wstitle= Electricity |volume= 9 |last= Fleming |first= John Ambrose |author-link= John Ambrose Fleming | pages = 179&ndash;193; see page 181, second para, three lines from end |quote=... the Swede, Johann Karl Wilcke (1732–1796), then resident in Germany, who in 1762 published an account of experiments in which....}}</ref>  [[Electrostatic generator]]s, such as the [[Wimshurst machine]], the [[Van de Graaff generator]] and the [[electrophorus]], use this principle. See also [[Stephen Gray (scientist)|Stephen Gray]] in this context. Due to induction, the [[electrostatic potential]] ([[voltage]]) is constant at any point throughout a conductor.<ref name="Purcell">{{cite book   
  | last = Purcell
  | first = Edward M.  
  |author2=David J. Morin
  | title = Electricity and Magnetism
  | publisher = Cambridge Univ. Press
  | date = 2013
  | pages = 127–128
  | url = https://books.google.com/books?id=A2rS5vlSFq0C&pg=PA127
  | isbn = 978-1107014022}}</ref> Electrostatic induction is also responsible for the attraction of light nonconductive objects, such as balloons, paper or styrofoam scraps, to static electric charges. Electrostatic induction laws apply in dynamic situations as far as the [[quasistatic approximation]] is valid.

== Explanation ==
{{multiple image
| align = right
| direction = horizontal
| header   = 
| image1   = Electrostatic induction experiment.png
| caption1 = Demonstration of induction, in the 1870s. The positive terminal of an [[electrostatic machine]] ''(right)'' is placed near an uncharged brass cylinder ''(left)'', causing the cylinder's near end to acquire a negative charge and the far end to acquire a positive charge. The small [[pith ball electroscope]]s hanging from the bottom show that the charge is concentrated at the ends.
| width1   = 260
| image2   = Cat demonstrating static cling with styrofoam peanuts.jpg
| caption2 = [[Styrofoam peanut]]s clinging to a cat's fur.  A [[static electricity|static electric charge]] builds up on the cat's fur due to [[triboelectricity]] from the cat's movements. The electric field of the charge causes a polarization of the molecules of the styrofoam due to electrostatic induction, resulting in a slight attraction of the styrofoam to the charged fur.
| width2   = 276
}}

A normal uncharged piece of matter has equal numbers of positive and negative [[electric charge]]s in each part of it, located close together, so no part of it has a net electric charge.<ref name="Halliday&Resnick">{{cite book
  | last1  = Halliday
  | first1 = David 
  | last2  = Resnick
  | first2 = Robert 
  | last3  = Walker
  | first3 = Jearl
  | title = Fundamentals of Physics
  | publisher = John Wiley and Sons
  | edition = 9
  | date = 2010
  | pages = 
  | url = https://archive.org/details/halliday-resnick-fundamentals-of-physics-cuuduongthancong.com/page/711/mode/2up
  | archive-url= 
  | archive-date=
  | doi = 
  | id = 
  | isbn = 9780470469118
  | mr = 
  | zbl = 
  | jfm =}}</ref>{{rp|p.711–712}}   The positive charges are the [[atom]]s' [[atomic nuclei|nuclei]] which are bound into the structure of matter and are not free to move.  The negative charges are the atoms' [[electron]]s.  In [[electrical conductor|electrically conductive]] objects such as metals, some of the electrons are able to move freely about in the object.

When a charged object is brought near an uncharged, [[Electrical conductor|electrically conducting]] object, such as a piece of metal, the force of the nearby charge due to [[Coulomb's law]] causes a separation of these internal charges.<ref name="Halliday&Resnick" />{{rp|p.712}}  For example, if a positive charge is brought near the object (see picture of cylindrical electrode near electrostatic machine), the electrons in the metal will be attracted toward it and move to the side of the object facing it.  When the electrons move out of an area, they leave an unbalanced positive charge due to the nuclei.   This results in a region of negative charge on the object nearest to the external charge, and a region of positive charge on the part away from it.  These are called ''induced charges''.  If the external charge is negative, the polarity of the charged regions will be reversed.

Since this process is just a redistribution of the charges that were already in the object, it doesn't change the ''total'' charge on the object; it still has no net charge.  This induction effect is reversible; if the nearby charge is removed, the attraction between the positive and negative internal charges causes them to intermingle again.

== Charging an object by induction ==
[[Image:Electroscope showing induction.png|thumb|upright=1.2|Gold-leaf electroscope, showing induction (labelled polarity of charges), before the terminal is grounded.]]
[[File:13. Електризација на електроскоп со инфлуенца.ogv|thumb|right|222px|Using an electroscope to show electrostatic induction. The device has leaves/needle that become charged when introducing a charged rod to it. The leaves bend the leave/needle, and the stronger the static introduced, the more bending occurs.]]

However, the induction effect can also be used to put a net charge on an object.<ref name="Halliday&Resnick" />{{rp|p.711–713}}  If, while it is close to the positive charge, the above object is momentarily connected through a [[electrical conductor|conductive]] path to [[ground (electricity)|electrical ground]], which is a large reservoir of both positive and negative charges, some of the negative charges in the ground will flow into the object, under the attraction of the nearby positive charge.  When the contact with ground is broken, the object is left with a net negative charge.

This method can be demonstrated using a [[gold-leaf electroscope]], which is an instrument for detecting electric charge.  The electroscope is first discharged, and a charged object is then brought close to the instrument's top terminal.  Induction causes a separation of the charges inside the [[electroscope]]'s metal rod, so that the top terminal gains a net charge of opposite polarity to that of the object, while the gold leaves gain a charge of the same polarity.  Since both leaves have the same charge, they repel each other and spread apart.  The electroscope has not acquired a net charge: the charge within it has merely been redistributed, so if the charged object were to be moved away from the electroscope the leaves will come together again.

But if an electrical contact is now briefly made between the electroscope terminal and [[ground (electricity)|ground]], for example by touching the terminal with a finger,  this causes charge to flow from ground to the terminal, attracted by the charge on the object close to the terminal.  This charge neutralizes the charge in the gold leaves, so the leaves come together again.  The electroscope now contains a net charge opposite in polarity to that of the charged object.  When the electrical contact to earth is broken, e.g. by lifting the finger, the extra charge that has just flowed into the electroscope cannot escape, and the instrument retains a net charge.  The charge is held in the top of the electroscope terminal by the attraction of the inducing charge.  But when the inducing charge is moved away, the charge is released and spreads throughout the electroscope terminal to the leaves, so the gold leaves move apart again.

The sign of the charge left on the electroscope after grounding is always opposite in sign to the external inducing charge.<ref name="Cope">{{cite book   
  | last = Cope
  | first = Thomas A. Darlington 
  | title = Physics
  | publisher = Library of Alexandria
  | url = https://books.google.com/books?id=A0dl7DipTHUC&pg=RA1-PA116
  | isbn = 1465543724}}</ref> The two rules of induction are:<ref name="Cope" /><ref name="Hadley">{{cite book   
  | last = Hadley
  | first = Harry Edwin 
  | title = Magnetism & Electricity for Beginners
  | publisher = Macmillan & Company
  | date = 1899
  | pages = 182
  | url = https://books.google.com/books?id=rygyAQAAMAAJ&pg=PA182
  }}</ref>
*If the object is not grounded, the nearby charge will induce ''equal'' and ''opposite'' charges in the object.
*If ''any part'' of the object is momentarily grounded while the inducing charge is near, a charge opposite in polarity to the inducing charge will be attracted from ground into the object, and it will be left with a charge ''opposite'' to the inducing charge.
{{clear}}

==The electrostatic field inside a conductive object is zero==
[[Image:Electrostatic induction.svg|thumb|upright=1.5|Surface charges induced in metal objects by a nearby charge.  The [[electrostatic field]] ''(lines with arrows)'' of a nearby positive charge ''<span style="color:red;">(+)</span>'' causes the mobile charges in metal objects to separate. Negative charges ''<span style="color:blue;">(blue)</span>'' are attracted and move to the surface of the object facing the external charge.  Positive charges ''<span style="color:red;">(red)</span>'' are repelled and move to the surface facing away.   These induced surface charges create an opposing electric field that exactly cancels the field of the external charge throughout the interior of the metal.  Therefore electrostatic induction ensures that the electric field everywhere inside a conductive object is zero.]]

A remaining question is how large the induced charges are.   The movement of charges is caused by the [[force]] exerted on them by the [[electric field]] of the external charged object, by [[Coulomb's law]].  As the charges in the metal object continue to separate, the resulting positive and negative regions create their own electric field, which opposes the field of the external charge.<ref name="Purcell" />   This process continues until very quickly (within a fraction of a second) an [[Equilibrium state|equilibrium]] is reached in which the induced charges are exactly the right size and shape to cancel the external electric field throughout the interior of the metal object.<ref name="Purcell" /><ref name="Saslow">{{cite book   
  | last = Saslow
  | first = Wayne M. 
  | title = Electricity, magnetism, and light
  | publisher = Academic Press
  | year = 2002
  | location = US
  | pages = 159–161
  | url = https://books.google.com/books?id=4liwlxqt9NIC&q=electrostatic+induction+equilibrium&pg=PA159
  | isbn = 0-12-619455-6}}</ref>  Then the remaining mobile charges (electrons) in the interior of the metal no longer feel a force and the net motion of the charges stops.<ref name="Purcell" />

==Induced charge resides on the surface==
Since the mobile charges (electrons) in the interior of a metal object are free to move in any direction, there can never be a static concentration of charge inside the metal; if there was, it would disperse due to its mutual repulsion.<ref name="Purcell" />  Therefore in induction, the mobile charges move through the metal under the influence of the external charge in such a way that they maintain local electrostatic neutrality; in any interior region the negative charge of the electrons balances the positive charge of the nuclei.  The electrons move until they reach the surface of the metal and collect there, where they are constrained from moving by the boundary.<ref name="Purcell" /> The surface is the only location where a net electric charge can exist.<ref name="Halliday&Resnick" />{{rp|p.754}}

This establishes the principle that electrostatic charges on conductive objects reside on the surface of the object.<ref name="Purcell" /><ref name="Saslow" />  External electric fields induce surface charges on metal objects that exactly cancel the field within.<ref name="Purcell" />

==The voltage throughout a conductive object is constant==
The [[electrostatic potential]] or [[voltage]] between two points is defined as the [[energy]] (work) required to move a small positive charge through an electric field between the two points, divided by the size of the charge. If there is an electric field directed from point <math>\mathbf{b}</math> to point <math>\mathbf{a}</math> then it will exert a force on a charge moving from <math>\mathbf{a}</math>  to <math>\mathbf{b}</math>.  Work will have to be done on the charge by a force to make it move to <math>\mathbf{b}</math> against the opposing force of the electric field.  Thus the electrostatic potential energy of the charge will increase.   So the potential at point  <math>\mathbf{b}</math> is higher than at point <math>\mathbf{a}</math>.  The electric field <math>\mathbf{E}(\mathbf{x})</math> at any point <math>\mathbf{x}</math> is the [[gradient]] (rate of change) of the [[electrostatic potential]] <math>V(\mathbf{x})</math> : 
:<math>\nabla V = \mathbf{E}\,</math>
Since there can be no electric field inside a conductive object to exert force on charges <math>(\mathbf{E} = 0)\,</math>, within a conductive object the gradient of the potential is zero<ref name="Purcell" />  
:<math>\nabla V = \mathbf{0}\,</math>
Another way of saying this is that in electrostatics, electrostatic induction ensures that the potential (voltage) throughout a conductive object is constant.

== Induction in dielectric objects ==
[[Image:Paper shavings attracted by charged cd.jpg|thumb|Paper snippets attracted by a charged CD]]
A similar induction effect occurs in [[nonconductor|nonconductive]] ([[dielectric]]) objects, and is responsible for the attraction of small light nonconductive objects, like balloons, scraps of paper or [[Styrofoam]], to [[static electricity|static electric charges]]<ref name="Sherwood">{{cite book   
  | last = Sherwood
  | first = Bruce A. 
  |author2=Ruth W. Chabay|author2-link= Ruth Chabay
  | title = Matter and Interactions| edition= 3rd
  | publisher = John Wiley and Sons
  | year =  2011
  | location = USA
  | pages = 594–596
  | url = https://books.google.com/books?id=8oyNPd5QbYgC&q=polarization+induced+insulator+attract&pg=PA595
  | isbn = 978-0-470-50347-8}}</ref><ref name="Tippens">[http://www.docstoc.com/docs/76893329/Electric-Force  Paul E. Tippens,  ''Electric Charge and Electric Force'', Powerpoint presentation, p.27-28, 2009, S. Polytechnic State Univ.] {{webarchive |url=https://web.archive.org/web/20120419225338/http://www.docstoc.com/docs/76893329/Electric-Force |date=April 19, 2012 }} on DocStoc.com website</ref><ref name="Henderson">{{cite web
  | last = Henderson
  | first = Tom
  | title = Charge and Charge Interactions
  | work = Static Electricity, Lesson 1
  | publisher = The Physics Classroom
  | year = 2011
  | url = https://www.physicsclassroom.com/class/estatics/u8l1e.cfm
  | access-date = 2012-01-01}}</ref> ''(see picture of cat, above)'', as well as [[static cling]] in clothes.

In nonconductors, the [[electron]]s are bound to [[atom]]s or [[molecule]]s and are not free to move about the object as in conductors; however they can move a little within the molecules.  If a positive charge is brought near a nonconductive object, the electrons in each molecule are attracted toward it, and move to the side of the molecule facing the charge, while the positive [[nucleus (atomic structure)|nuclei]] are repelled and move slightly to the opposite side of the molecule.  Since the negative charges are now closer to the external charge than the positive charges, their attraction is greater than the repulsion of the positive charges, resulting in a small net attraction of the molecule toward the charge.  This effect is microscopic, but since there are so many molecules, it adds up to enough force to move a light object like Styrofoam.

This change in the distribution of charge in a molecule due to an external electric field is called [[dielectric polarization]],<ref name="Sherwood" /> and the polarized molecules are called [[dipole]]s.  This should not be confused with a [[polar molecule]], which has a positive and negative end due to its structure, even in the absence of external charge.  This is the principle of operation of a [[Electroscope#Pith-ball electroscope|pith-ball electroscope]].<ref name="Kaplan">{{cite book
 |title       = Kaplan MCAT Physics 2010-2011
 |publisher   =famous Publishing
 |year        = 2009
 |location    = USA
 |pages       = 329
 |url         = https://books.google.com/books?id=pPleL5NOtb4C&q=%22pith+ball+electroscope%22+induction&pg=PA329
 |isbn        = 978-1-4277-9875-6
 |url-status     = dead
 |archive-url  = https://web.archive.org/web/20140131021101/http://books.google.com/books?id=pPleL5NOtb4C&pg=PA329&dq=%22pith+ball+electroscope%22+induction&hl=en&sa=X&ei=UOL_Tr-0GeeRiQK76aTCCg&ved=0CEcQ6AEwAQ#v=onepage&q=%22pith%20ball%20electroscope%22%20induction&f=false
 |archive-date = 2014-01-31
}}</ref>

== References ==
{{reflist}}

== External links ==
{{EB1911 poster|Electrostatics}}
*{{Commons category-inline}}
*{{cite web
 |title=Charging by electrostatic induction 
 |work=Regents exam prep center 
 |publisher=Oswego City School District 
 |year=1999 
 |url=https://regentsprep.org/Regents/physics/phys03/aeleclab/induct.htm 
 |access-date=2008-06-25 
 |url-status=dead 
 |archive-url=https://web.archive.org/web/20080828082950/http://regentsprep.org/Regents/physics/phys03/aeleclab/induct.htm 
 |archive-date=2008-08-28 
}}

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{{DEFAULTSORT:Electrostatic Induction}}
[[Category:Electrostatics]]
[[Category:Electricity]]