Chapter 20: Static electricity


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Nature provides few more awesome displays than lightning. Benjamin Franklin was colonial America’s foremost scientist. Starting in 1740, Franklin studied electricity produced by friction, charges that result from rubbing two surfaces together. Franklin proposed his famous kite experiment in 1750, and two years later showed that “electrical fire” could be drawn from a cloud. Franklin became famous as s scientist throughout Europe. This fame probably helped assure his diplomatic successes in France during the American Revolution. You may have rubbed your shoes on the carpet hard enough to create a lightning-like spark when you touched someone. Franklin’s kite experiment showed that lightning is similar to frictional electricity. Electrostatics is the study of electrical charges that can be collected and held in lone place. Running a comb through your hair transfers electrons to the comb, giving it a negative charge. If the comb, for example, is brought close to bits of paper, a charge separation is induced on the paper bits. The attractive electric force accelerates the paper bits upward against the force of gravity.

Microscopic View of Charge

  • Electric charges exist in the atom itself. In 1890, J.J. Thompson discovered that all materials contain light, negatively–charged particles he called electrons. Also, between 1909 and 1911, Ernest Rutherford, a New Zealander, discovered that atoms have a massive, positively-charged nucleus, or center. The electrons surround the nucleus. The positive charge of the nucleus is exactly balanced by the negative charge of the electron. That is, the atom is uncharged; it is neutral.
  • Conductors and Insulators
  • Materials through which charges will not move easily are called insulators. Charges removed from one area on an insulator are not replaced by charges from another area. Glass, dry wood, most plastics, cloth, and dry air are good insulators.
  • Materials such as metals that allow charges to move about easily are called electrical conductors. Electrons carry, or conduct, electric charge through the metal. Metals are good conductors because at least one electron on each atom can be removed easily. These electrons are free to move about the metal in the same way atoms in a gas move about a container. They are said to form an electron gas. Copper and aluminum are both excellent conductors and are used commercially to carry electricity. Graphite, the form of carbon used in pencils, also is a good conductor.
  • Electrical forces must be strong, as they can easily produce acceleration larger than the acceleration caused by gravity. We have also seen that they can be either repulsive or attractive, while gravitational forces are always attractive. Many scientists made attempts to measure the electrical force. Daniel Bernoulli, otherwise known for his work on fluids, made some crude measurements in 1760. In 1770, Henry Cavendish showed electric forces must obey an inverse square force law, but, being extremely shy, he did not publish his work. His manuscripts were discovered over a century later, after all his work had been duplicated by others.
  • An electroscope consists of a metal knob connected by a metal stem to two thin, lightweight pieces of metal foil called leaves.
  • Coulomb’s Law

    Coulomb found how the force between two charged spheres, A and B, depended on the distance. First he carefully measured the amount of force needed to twist the suspending wire through a given angle. He then placed equal charges on spheres A and B and varied the distance, d, between them. The electric force moved A from its rest position, twisting the suspending wire. By measuring the deflection of A, Coulomb could calculate the force of repulsion. He made many measurements with spheres charged with both positively and negatively. He showed that the force, F, varied inversely with the square of the distance between the centers of the spheres.

    F u Kqq’o d2

    Summary

    Electrical Charges

  • There are two kinds of electrical charges, positive and negative. Electrons are negative.
  • Electrical charge is conserved; it cannot be created or destroyed.
  • Bodies can be charged negatively or positively by transferring electrons to it. An object is charged positively by removing electrons from it.
  • Charges added to one part of an insulator remain on the part.
  • Charges added to a conductor very quickly spread over the surface of the body. This is called electrical conduction.
  • Charges exert forces on other charges. Like charges repel; unlike charges attract.
  • Electrical Fields

  • An electroscope indicates electrical charge. In an electroscope, forces on charges cause thin metal leaves to spread.
  • A charged rod can charge an electroscope by induction by causing a separation of charges.
  • Coulomb’s law states that the force between two charged point objects varies directly with the product of the two charges and inversely with the square of the distance between them.
  • The unit of charge is the coulomb. One coulomb, C, is the magnitude of the charge of 6.25x10 18 electrons or protons. The elementary charge, the charge of the proton or electron, is 1.60x 10–19 C.
  • A charged body of either sign can produce separation of charge in a neutral body. Thus a charged body attracts a neutral body.
  • Chapter 21: Electric fields

    The electric force, like the gravitational force varies inversely as the square of the distance between two objects. Both forces can act at a great distance. How can a force be exerted across what seems to be empty space? In trying to understand the electric force, Michael Faraday (1791-1867) developed the concept of an electric field. According to Faraday, a charge creates an electric field about it in all directions. If a second charge is placed at some point in the field, the second charge interacts with the field at that point. The force it feels is the result of a local interaction. Interaction between particles separated by some distance is no longer required.

    The electric Field

    An electric field is the property of space around a charged object that causes forces on other charge objects.

    The direction of the electric field is the direction of the force on the positive test charge. The magnitude of the electric field intensity is measured in newtons per coulomb, N/C.

    E= F muK q’ q’

    Notice that just as the electric field is the force per unit charge, the gravitational field is the force per unit mass, g=F/m.

    The collection of all the force vectors on the test charge is called an electric field. Any charge placed in an electric field experiences a force on it due to the electric field at that location. The strength of the force depends on the magnitude of the field, E, and the size of the charge, q. Thus F=Eq. The direction of the force depends on the direction of the field and the sign of the charge.

    A picture of an electric field can be made by using arrows to represent the field vectors at various locations. The length of the arrow shows its direction. To find the field from two charges, the fields from the individual charges can be added vertically.

    Picturing the Electric Field

    An alternative picture of an electric field is shown below. The lines are called electric field lines. The direction of the field at any point is the tangent drawn to the field line at that point. The strength of the electric field is indicated by the spacing between the lines. The field is strong where the lines are close together. It is weaker where the lines are spaced farther apart. Remember that electric fields exist in three dimensions.

    When there are two or more charges, the field is the vector sum of the fields due to the individual charges. Note that field lines always leave a positive charge and enter a negative charge. The Van de Graaff machine is a device that transfers large amounts of charge from one part of the machine to the top metal terminal. Field lines do not really exist. They are just a means of providing a model of an electric field. Electric fields, on the other hand, do exist. An electric field is produced by one or more charges and is independent of the existence of the test charge that is used to measure it. The field provides a method of calculating the force on a charged body. It does not explain, however, why charged bodies exert forces on each other. That question is still unanswered.

    How does the potential difference depend on the electric field? In the case of the gravitational field, near the surface of Earth the gravitational force and field are relatively constant. A constant electric force and field can be made by placing two large flat conductors plates parallel to each other. One is charged positively and the other negatively. The electric field between the plates is constant except at the edges of the plate. Its direction is from the positive to the negative plate.

    Millikan’s Oil Drop Experiment

    One important application of the uniform electric field between two parallel plates was the measurement of the charge of an electron. This was made by American physicist Robert A. Millikan (1868-1953) in 1909.

    The presently accepted theory of matter says that protons are made up of fundamental particles called quarks. The charge on a quark is either +1/3 or -2/3 the charge on an electron. A theory of quarks that agrees with other experiments states that quarks can never be isolated. Many experiments have used an updated Millikan apparatus to look for fractional charges on drops or tiny metal spheres. There have been no reproducible discoveries of fractional charges. Thus, no isolated quark has been discovered, the quark theory remains consistent with experiments.

    Summary

    Creating and Measuring Electric Fields

  • An electric field exists around any charged object. The field produces forces on other charged bodies.
  • The electric field intensity is the force per unit charge. The direction of the electric field is the direction of the force on a tiny, positive test charge.
  • Electric field lines provide a picture of the electric field. They are directed away from positive charges and toward negative charges.
  • Aplications of Electric Fields

  • Electric potential difference is the change in potential energy per unit charge in an electric field. Potential differences are measured in volts.
  • The electric field between two parallel plates is uniform between the plates except near the edges.
  • Robert Millikan’s experiments showed that electric charge is quantized and that the charge carried by an electron is -1.6x 10-10 C.
  • Charges will move in conductors until the electric potential is the same everywhere on the conductor.
  • A charged object can have its excess charge removed by touching it to Earth or to an object touching Earth. This is called grounding.
  • Electric fields are strongest near sharply-pointed conductors.
  • Capacitance is the ratio of the charge on a body to its potential. The capacitance of a body is independent of the charge on the body and the potential difference across it.
  • Links

    Static Electricity1
    Static Electricity2
    Static Electricity3
    Static Electricity4
    Static Electricity5
    Electic Fields1
    Elecric Fields2
    Electric Fields3

    Sources:

    Merill Physics:(Priniples by Paul W.Zitzewitz & Robert F. Neff.Chapters 20-20

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