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  • Electricity and Magnetism Capacitance

    Lana Sheridan

    De Anza College

    Jan 29, 2018

  • Last time

    • Potential of charged conductor

    • dipole in a magnetic field

    • Millikan’s experiment - skipping for now

  • Overview

    • Van de Graaf generator

    • Capacitors

    • Potential difference and charged plates

    • Capacitance

    • Capacitance of a parallel plate capacitor

    • Capacitance of a spherical and cylindrical capacitors

  • Van de Graaf generator

    25.8 Applications of Electrostatics 765

    After recording measurements on thousands of droplets, Millikan and his coworkers found that all droplets, to within about 1% precision, had a charge equal to some integer multiple of the elementary charge e :

    q 5 ne n 5 0, 21, 22, 23, . . .

    where e 5 1.60 3 10219 C. Millikan’s experiment yields conclusive evidence that charge is quantized. For this work, he was awarded the Nobel Prize in Physics in 1923.

    25.8 Applications of Electrostatics The practical application of electrostatics is represented by such devices as light- ning rods and electrostatic precipitators and by such processes as xerography and the painting of automobiles. Scientific devices based on the principles of electro- statics include electrostatic generators, the field-ion microscope, and ion-drive rocket engines. Details of two devices are given below.

    The Van de Graaff Generator Experimental results show that when a charged conductor is placed in contact with the inside of a hollow conductor, all the charge on the charged conductor is trans- ferred to the hollow conductor. In principle, the charge on the hollow conductor and its electric potential can be increased without limit by repetition of the process. In 1929, Robert J. Van de Graaff (1901–1967) used this principle to design and build an electrostatic generator, and a schematic representation of it is given in Figure 25.23. This type of generator was once used extensively in nuclear physics research. Charge is delivered continuously to a high-potential electrode by means of a moving belt of insulating material. The high-voltage electrode is a hollow metal dome mounted on an insulating column. The belt is charged at point ! by means of a corona discharge between comb-like metallic needles and a grounded grid. The needles are maintained at a positive electric potential of typically 104 V. The positive charge on the moving belt is transferred to the dome by a second comb of needles at point ". Because the electric field inside the dome is negligible, the positive charge on the belt is easily transferred to the conductor regardless of its potential. In prac- tice, it is possible to increase the electric potential of the dome until electrical dis- charge occurs through the air. Because the “breakdown” electric field in air is about 3 3 106 V/m, a sphere 1.00 m in radius can be raised to a maximum potential of 3 3 106 V. The potential can be increased further by increasing the dome’s radius and placing the entire system in a container filled with high-pressure gas. Van de Graaff generators can produce potential differences as large as 20 mil- lion volts. Protons accelerated through such large potential differences receive enough energy to initiate nuclear reactions between themselves and various target nuclei. Smaller generators are often seen in science classrooms and museums. If a person insulated from the ground touches the sphere of a Van de Graaff genera- tor, his or her body can be brought to a high electric potential. The person’s hair acquires a net positive charge, and each strand is repelled by all the others as in the opening photograph of Chapter 23.

    The Electrostatic Precipitator One important application of electrical discharge in gases is the electrostatic precipi- tator. This device removes particulate matter from combustion gases, thereby reduc- ing air pollution. Precipitators are especially useful in coal-burning power plants and industrial operations that generate large quantities of smoke. Current systems are able to eliminate more than 99% of the ash from smoke. Figure 25.24a (page 766) shows a schematic diagram of an electrostatic precipi- tator. A high potential difference (typically 40 to 100 kV) is maintained between

    The charge is deposited on the belt at point ! and transferred to the hollow conductor at point ".

    "

    !

    Metal dome

    Belt

    Ground

    !

    P

    Insulator

    !

    !

    !

    !

    !

    !

    !

    !

    !

    !

    !

    !

    !

    !

    !

    !

    !

    !

    !

    !

    !

    !

    Figure 25.23 Schematic dia- gram of a Van de Graaff generator. Charge is transferred to the metal dome at the top by means of a moving belt.

    Can (in principle) build up to 3 million Volts when used in air.

  • Capacitance

    capacitor

    Any two isolated conductors separated by some distance that can store different charges.

    (When the capacitor is discharged this stored charge is 0.) 65725-2 CAPACITANCE PART 3

    HALLIDAY REVISED

    shape. No matter what their geometry, flat or not, we call these conductors plates.

    Figure 25-3a shows a less general but more conventional arrangement, called a parallel-plate capacitor, consisting of two parallel conducting plates of area A separated by a distance d. The symbol we use to represent a capacitor (!") is based on the structure of a parallel-plate capacitor but is used for capacitors of all geometries. We assume for the time being that no material medium (such as glass or plastic) is present in the region between the plates. In Section 25-6, we shall remove this restriction.

    When a capacitor is charged, its plates have charges of equal magnitudes but opposite signs: !q and "q. However, we refer to the charge of a capacitor as being q, the absolute value of these charges on the plates. (Note that q is not the net charge on the capacitor, which is zero.)

    Because the plates are conductors, they are equipotential surfaces; all points on a plate are at the same electric potential. Moreover, there is a potential difference be- tween the two plates. For historical reasons, we represent the absolute value of this potential difference with V rather than with the #V we used in previous notation.

    The charge q and the potential difference V for a capacitor are proportional to each other; that is,

    q $ CV. (25-1)

    The proportionality constant C is called the capacitance of the capacitor. Its value depends only on the geometry of the plates and not on their charge or potential difference. The capacitance is a measure of how much charge must be put on the plates to produce a certain potential difference between them: The greater the capacitance, the more charge is required.

    The SI unit of capacitance that follows from Eq. 25-1 is the coulomb per volt. This unit occurs so often that it is given a special name, the farad (F):

    1 farad $ 1 F $ 1 coulomb per volt $ 1 C/V. (25-2)

    As you will see, the farad is a very large unit. Submultiples of the farad, such as the microfarad (1 mF $ 10"6 F) and the picofarad (1 pF $ 10"12 F), are more convenient units in practice.

    Charging a Capacitor One way to charge a capacitor is to place it in an electric circuit with a battery. An electric circuit is a path through which charge can flow. A battery is a device

    Fig. 25-3 (a) A parallel-plate capacitor, made up of two plates of area A separated by a distance d.The charges on the facing plate surfaces have the same magnitude q but opposite signs. (b) As the field lines show, the electric field due to the charged plates is uniform in the central region between the plates.The field is not uniform at the edges of the plates, as indicated by the “fringing” of the field lines there.

    Area A V

    d

    Top side of bottom plate has charge –q

    A

    –q

    +q

    (b)(a)

    Bottom side of top plate has charge +q

    Electric field lines

    halliday_c25_656-681v2.qxd 23-11-2009 14:32 Page 657

    The capacitance of a capacitor relates the potential difference across the capacitor to its stored charge.

  • Capacitors

    Capacitors can be thought of as devices that store charge at some particular potential difference.

    They can also be thought of as storing energy in an electric field.

  • Capacitors

    Usually capacitors are diagrammed and thought of as parallel sheets of equal area, but paired, isolated conductors of any shape can act as capacitors.

    C H A P T E R

    656

    C A P A C I TA N C E25 W H AT I S P H YS I C S ?25-1 One goal of physics is to provide the basic science for practical devices

    designed by engineers. The focus of this chapter is on one extremely common example—the capacitor, a device in which electrical energy can be stored. For ex- ample, the batteries in a camera store energy in the photoflash unit by charging a capacitor. The batteries can supply energy at only a modest rate, too slowly for the photoflash unit to emit a flash of light. However, once the capacitor is charged, it can supply energy at a much greater rate when the photoflash unit is triggered—enough energy to allow the unit to emit a burst of bright light.

    The physics of capacitors can be generalized to other devices and to any situ- ation involving electric fields. For example, Earth’s atmospheric electric field is modeled by meteorologists as being produced