Electrostatic induction

From Wikipedia, the free encyclopedia
Jump to: navigation, search

Electrostatic induction is a redistribution of electrical charge in an object, caused by the influence of nearby charges.[1] Induction was discovered by British scientist John Canton in 1753 and Swedish professor Johan Carl Wilcke in 1762.[2] Electrostatic generators, such as the Wimshurst machine, the Van de Graaff generator and the electrophorus, use this principle. Due to induction, the electrostatic potential (voltage) is constant at any point throughout a conductor.[3] Induction is also responsible for the attraction of light nonconductive objects, such as balloons, paper or styrofoam scraps, to static electric charges. Electrostatic induction should not be confused with electromagnetic induction.

Explanation[edit]

Demonstration of induction, in the 1870s. The positive terminal of an electrostatic machine is placed near an uncharged brass cylinder, causing the left end to acquire a positive charge and the right to acquire a negative charge. The small pith ball electroscopes hanging from the bottom show that the charge is concentrated at the ends.

A normal uncharged piece of matter has equal numbers of positive and negative electric charges in each part of it, located close together, so no part of it has a net electric charge. The positive charges are the atoms' nuclei which are bound into the structure of matter and are not free to move. The negative charges are the atoms' electrons. In 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, electrically conducting object, such as a piece of metal, the force of the nearby charge causes a separation of these internal charges. For example, if a positive charge is brought near the object (see picture at right), 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 cause them to intermingle again.

Charging an object by induction[edit]

Gold-leaf electroscope, showing induction, before the terminal is grounded.

However, the induction effect can also be used to put a net charge on an object. If, while it is close to the positive charge, the above object is momentarily connected through a conductive path to 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, 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.[4] The two rules of induction are:[4][5]

  • 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.

The electrostatic field inside a conductive object is zero[edit]

Surface charges induced in metal objects by a nearby charge. The electrostatic field (lines with arrows) of a nearby positive charge (+) causes the mobile charges in metal objects to separate. Negative charges (blue) are attracted and move to the surface of the object facing the external charge. Positive charges (red) 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.

[6] A remaining question is how large the induced charges are. In the absence of gravity, the movement of charge is caused by the force exerted by the electric field of the external charged object. 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.[3] This process continues until very quickly (within a fraction of a second) an equilibrium is reached in which the induced charges are exactly the right size to cancel the external electric field throughout the interior of the metal object.[3][7] 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.[3] If the conductor is immersed in a gravitational field then the potential energy of this additional field must be included. As an example, at the Earth's surface there is about 55 picoVolts/meter of vertical electric field in conductors, as required to counter the force of gravity upon the mobile electrons.(mg=qE).[citation needed]

Induced charge resides on the surface[edit]

Since the mobile charges 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 attract opposite polarity charge to neutralize it.[3] Therefore in induction, the mobile charges move under the influence of the external charge until they reach the surface of the metal and collect there, where they are constrained from moving by the boundary.[3]

This establishes the important principle that electrostatic charges on conductive objects reside on the surface of the object.[3][7] External electric fields induce surface charges on metal objects that exactly cancel the field within.[3] Since the field is the gradient of the electrostatic potential, another way of saying this is that in electrostatics, the potential (voltage) throughout a conductive object is constant.[3]

Induction in dielectric objects[edit]

Paper shavings attracted by charged cd.jpg

A similar induction effect occurs in nonconductive (dielectric) objects, and is responsible for the attraction of small light nonconductive objects, like balloons, scraps of paper or Styrofoam, to static electric charges.[8][9][10][11] In nonconductors, the electrons are bound to atoms or molecules 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 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 is called polarization, and the polarized molecules are called dipoles. 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 is the principle of operation of a pith-ball electroscope.[12]

Notes[edit]

  1. ^ "Electrostatic induction". Encyclopaedia Britannica. Encyclopaedia Britannica, Inc. 2008. Retrieved 2008-06-25. 
  2. ^ "Electricity". Encyclopaedia Britannica, 11th Ed. 9. The Encyclopaedia Britannica Co. 1910. p. 181. Retrieved 2008-06-23. 
  3. ^ a b c d e f g h i Purcell, Edward M.; David J. Morin (2013). Electricity and Magnetism. Cambridge Univ. Press. pp. 127–128. ISBN 1107014026. 
  4. ^ a b Cope, Thomas A. Darlington. Physics. Library of Alexandria. ISBN 1465543724. 
  5. ^ Hadley, Harry Edwin (1899). Magnetism & Electricity for Beginners. Macmillan & Company. p. 182. 
  6. ^ The electric field inside a conductor is zero
  7. ^ a b Saslow, Wayne M. (2002). Electricity, magnetism, and light. US: Academic Press. pp. 159–161. ISBN 0-12-619455-6. 
  8. ^ Sherwood, Bruce A.; Ruth W. Chabay (2011). Matter and Interactions, 3rd Ed.. USA: John Wiley and Sons. pp. 594–596. ISBN 0-470-50347-5. 
  9. ^ Paul E. Tippens, Electric Charge and Electric Force, Powerpoint presentation, p.27-28, 2009, S. Polytechnic State Univ. on DocStoc.com website
  10. ^ Henderson, Tom (2011). "Charge and Charge Interactions". Static Electricity, Lesson 1. The Physics Classroom. Retrieved 2012-01-01. 
  11. ^ Winn, Will (2010). Introduction to Understandable Physics Vol. 3: Electricity, Magnetism and Ligh. USA: Author House. p. 20.4. ISBN 1-4520-1590-2. 
  12. ^ Kaplan MCAT Physics 2010-2011. USA: Kaplan Publishing. 2009. p. 329. ISBN 1-4277-9875-3. 

External links[edit]