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    UMass Amherst Biochemistry Teaching Initiative

    Electricity and Magnetism

    Lecture Notes

    Chapter 27: The Electric Field

    2/24/2012 1Warwick Bowen PHYS1002 Lectures, CH. 27

    We gratefully acknowledge the University of Colorado forproviding many of the concept questions utilised in this

    course

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    UMass Amherst Biochemistry Teaching Initiative

    Lecture 2

    Sections 26.5 & 27.1-2: Basics of

    electric fields, principle ofsuperposition

    2/24/2012 Warwick Bowen PHYS1002 Lectures, CH. 26 2

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    UMass Amherst Biochemistry Teaching Initiative

    1 Demonstration: Electric Field

    Van de Graaff Generator

    2/24/2012 3Warwick Bowen PHYS1002 Lectures, CH. 27

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    7

    A.

    B.

    C. 0

    D.

    E. None of these

    Charges -Q and +Q are located on the x-axis as shown.

    What is the magnitudeof the electric field at point A?

    2 Question 3

    2/24/2012 Warwick Bowen PHYS1002 Lectures, CH. 27 7

    kQ

    R2

    11

    9

    kQ

    R2

    11

    4

    kQ

    R2

    1

    91

    x

    -Q +Q

    R R R

    A

    A. B. C. D. E.

    20% 20% 20%20%20%

    A. A

    B. B

    C. C

    D. DE. E

    10

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    Electric field of a dipoleWe can represent an electric dipole by two opposite charges q separated by

    the small distance s.

    The dipole moment determines the electric field strength and is defined as

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    Electric field of a dipole

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    A. A

    B. B

    C. C

    D. D

    E. E

    Three charges (equal magnitude) are arranged as shown.

    I) What is the direction of the E-field at point A?

    2 Question 4A

    2/24/2012 Warwick Bowen PHYS1002 Lectures, CH. 27 10

    _

    + +A

    A. B. C. D. E.

    20% 20% 20%20%20%

    Yellow

    Purple: zero

    Pink

    Blue

    Green

    A.

    D.

    B.

    C.

    E. zero 10

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    A. A

    B. B

    C. C

    D. D

    E. E

    2 Question 4B

    2/24/2012 Warwick Bowen PHYS1002 Lectures, CH. 27 11

    Yellow

    : some other direction

    Bluen

    A.

    B.

    D.C.

    E. some other direction

    A. B. C. D. E.

    0% 0% 0%0%0%

    Three charges (equal magnitude) are arranged as shown.

    II) An electron is fired into the region of the three

    charges from the lower right as shown. What is the

    direction of the acceleration of the electron when

    it is at point A?

    _

    + +

    A

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    A. A

    B. B

    C. CD. D

    E. E

    A. B.

    C. D.

    E: none of these/dont know

    Two IDENTICAL positive charges (protons) are fixed in place on the x-

    axis. Which of the following sketches best represents the electric field

    lines around these protons?

    2 Question 5

    2/24/2012 Warwick Bowen PHYS1002 Lectures, CH. 27 12

    A. B. C. D. E.

    0% 0% 0%0%0%

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    There are no charges in the regions shown. Which of the following are

    physically possible electrostatic field line configurations?

    2 Question 6

    2/24/2012 Warwick Bowen PHYS1002 Lectures, CH. 27 13

    A. AB. B

    C. C

    D. D

    E. More than one of the above is O.K.

    A. B. C. D. E.

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    There are no charges in the regions shown.

    Which of the following electrostatic field configurations are physically

    possible?

    2 Question 7

    2/24/2012 Warwick Bowen PHYS1002 Lectures, CH. 27 14

    (a) (b)

    (c)A. B. C. D. E.

    0% 0% 0%0%0%

    A. None are possible

    B. (a) only

    C. (b) only

    D. (c) only

    E. More than one of the above is o.k. 10

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    Pictorial representation of

    electric field

    2/24/2012 Warwick Bowen PHYS1002 Lectures, CH. 27 15

    Field-vector diagram Field-line diagram

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    Tactics: drawing and using

    electric field lines

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    Summary of E-field model

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    18UMass Amherst Biochemistry Teaching Initiative

    Vector Algebra

    If youre not confident with vector

    algebra, download the vectors worksheetfrom blackboard and go through it in your

    PASS session this week.

    Rm 7-209 (same room as prac labs)

    2/24/2012 18Warwick Bowen PHYS1002 Lectures, CH. 29 ... ...

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    19UMass Amherst Biochemistry Teaching Initiative

    Lecture 3

    Sections 27.3-5: Electric fields of

    continuous charge distributions andof basic objects

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    20Warwick Bowen PHYS1002 Lectures, CH. 27

    Aims

    To understand and be able to calculate surface chargedensity.

    To understand the method of determining the electric field

    of continuous charge distributions.

    To know and be able to calculate the electric fields of

    basic objects (lines, rings, disks, planes, capacitors, and

    spheres).

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    3 Question 1

    2/24/2012 Warwick Bowen PHYS1002 Lectures, CH. 27 21

    A piece of plastic is uniformly charged with surface charge density 1.

    The plastic is then broken into a large piece with surface charge

    density 2 and a small piece with surface charge density 3.

    Rank in order, from largest to smallest, the

    surface charge densities 1 to 3.

    A. B. C. D. E.

    20% 20% 20%20%20%

    A. 1

    > 2

    > 3

    B. 1 > 2 = 3

    C. 1 = 2 = 3

    D. 2 = 3 > 1

    E. 3 > 2 > 110

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    Surface charge density

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    24UMass Amherst Biochemistry Teaching Initiative

    Demonstration: Electric field

    shapes

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    4 Sample exam question

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    4 Sample exam question

    2/24/2012 Warwick Bowen PHYS1002 Lectures, CH. 27 32

    z

    x

    y

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    4 Sample exam question

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    4 Sample exam question

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    4 Sample exam question

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    4 Sample exam question

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    Rank in order, from largest to smallest, the electric field strengths Ea to

    Ee at these five points near an infinite plane of charge.

    4 Question 2

    2/24/2012 Warwick Bowen PHYS1002 Lectures, CH. 27 37A. B. C. D. E.

    20% 20% 20%20%20%

    10

    A. E a

    = Eb

    = Ec

    = Ed

    = Ee

    B. Ea > Ec > Eb > Ee > Ed

    C. Eb = Ec = Ed = Ee > Ea

    D. Ea > Eb = Ec > Ed = Ee

    E. Ee > Ed > Ec > Eb > Ea

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    38

    Getting to an infinite plane

    1) Sum field of point charges around a ring

    2) Sum field of concentric rings on a plane

    3) Let radius of plane go to infinity

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    Electric field strengths

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    The equation for the electric field outside an object with a net charge Q

    can be expressed using E= kQ/r2

    4 Question 3

    2/24/2012 Warwick Bowen PHYS1002 Lectures, CH. 27 40

    A. B. C. D. E.

    20% 20% 20%20%20%

    10

    A. if an only if the object is a point charge

    (like an electron or proton).

    B. if the object is stationary.

    C. if the object is a point charge or a

    uniformly charged sphere.

    D. if the object is a sphere, a disk, or a ring.

    E. regardless of the shape of the object.

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    The electric charge per unit area is +for plate 1 and for plate 2.

    The magnitude of the electric field associated with plate 1 is

    /2o, andthe electric field lines for this plate are as shown.

    When the two are placed

    parallel to one another,

    the magnitude of theelectric field is:

    5 Question 2

    2/24/2012 Warwick Bowen PHYS1002 Lectures, CH. 27 43

    A. B. C. D. E.

    0% 0% 0%0%0%

    A. /o between, 0 outside.

    B. /o between, /2o outside.

    C. zero both between and outside.

    D. /2o both between and

    outside.

    E. none of the above. 10

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    44UMass Amherst Biochemistry Teaching Initiative

    5 Demonstration:

    Electroplating

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    45UMass Amherst Biochemistry Teaching Initiative

    Vector Algebra

    If youre not confident with vector

    algebra, download the vectors worksheetfrom blackboard and go through it in your

    PASS session this week.

    Rm 7-209 (same room as prac labs)

    2/24/2012 45Warwick Bowen PHYS1002 Lectures, CH. 29 ... ...

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    46UMass Amherst Biochemistry Teaching Initiative

    Lecture 4

    Sections 27.6-7, 28.1-3: Motion of

    charged particles in electric fields,

    electric dipoles, symmetry, electric

    flux

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    47Warwick Bowen PHYS1002 Lectures, CH. 28

    Aims

    To understand and be able to predict the motion of

    charged objects and dipoles in the presence of electric

    fields.

    To understand the three fundamental symmetries

    (translation, rotation, and reflection).

    To understand that symmetries which apply to charged

    objects also apply to the shape of their electric field.

    To understand the concept of electric flux, and be able

    to calculate the flux through a surface.

    To know the definition of the direction of positive flux

    through a closed surface.

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    A. A

    B. B

    C. C

    D. D

    E. E

    Which electric field is responsible for the trajectory of

    the proton?

    6 Question 2

    2/24/2012 Warwick Bowen PHYS1002 Lectures, CH. 27 49

    A. B. C. D. E.

    0% 0% 0%0%0%

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    Motion of charged particles

    in an E-fieldThe electric field exerts a force:

    on a charged particle. If this was the only force acting on q, it causes the

    charged particle to accelerate with:

    In a uniform field, the acceleration is constant:

    2/24/2012 Warwick Bowen PHYS1002 Lectures, CH. 27 51

    analogous to constantacceleration due togravity g near theEarths surface

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    (1) (2)

    (3) (4)

    A dipole is placed in an external field as shown. In which situation(s)

    is the net force on the dipole zero?

    7 Question 1

    2/24/2012 Warwick Bowen PHYS1002 Lectures, CH. 27 55

    A. B. C. D. E.

    20% 20% 20%20%20%

    A. (1)

    B. (3)

    C. (1) and (2)

    D. (3) and (4)

    E. (2) and (4)

    10

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    57

    Dipoles in an electric field

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    Dipoles in an electric fieldTorque rotates dipole to align to electric field. The net force on

    the dipole is then always in the direction of increasing field

    magnitude.

    Dipoles experience a net force towards any charged object.

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    The dipole force allows trapping of neutral particles in regions of high

    electric field strength, such as at the focus of an intense laser beam.

    E.g. optical tweezers: important technique in biology for investigating the

    properties of DNA and understanding the properties of cells.

    Optical dipole traps

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    Optical dipole traps have also become an important tool for research in the

    areas of ultra-cold atoms and quantum computing.

    2/24/2012 60Warwick Bowen PHYS1002 Lectures, CH. 27

    Optical dipole traps

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    Optical dipole traps

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    7 Sample exam question

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    64UMass Amherst Biochemistry Teaching Initiative

    Chapter 27. Summary Slides

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    General Principles

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    General Principles

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    Applications

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    Applications