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  • Welcome to Physics

    2112

    Hit “E” on your clicker

    Electricity & Magnetism Lecture 22, Slide 1

  • Physics 2112

    Unit 22

    Outline

    ➢ Displacement Current

    ➢ Maxwell’s Equations (Final Form)

    ➢ E&M Waves

    Electricity & Magnetism Lecture 22, Slide 2

  • Your Comments

    Electricity & Magnetism Lecture 22, Slide 3

    AmazingThis pre-lecture was a lot more fun then a lot of the stuff we have learned over the last week of schoolI really liked how the checkpoint questions were not well explained by the prelecture. In seriousness, the derivation of the DE for the wave solution was done at breakneck speeds and was impossible for me to follow.Pretty fascinating prelecture... if you just make yourself believe everything that's going on and accept the last conclusion. Couldn't really understand much in the middle after the displacement current section.I think that the after doing a few problems it will become clearer but the relationship between magnetic fields and electric fields is hard to visualize.Can you explain the graph for electromagnetic waves.why are integrals everywhere in this course ?!

  • Where we are now

    =•surface

    AdB 0

    ENCLo

    loop

    IldB =•

    •−=• AdBdtd

    ldEloop

    o

    enc

    surface

    QAdE

    =•

    Our equations so far…..

    Unit 22, Slide 4

    Gauss’ Law

    Gauss’ Law for B fieldAmpere’s Law

    Faraday’s Law

    dt

    d B−=

  • 3 Points, all a distance r from axis of a current c

    carrying wire connected to capacitor

    Displacement Current

    Electricity & Magnetism Lecture 22, Slide 5

    r●

    I1

    1 3●

    2

    rIBB o 2/|||| 31 ==

    ??0|| 2 =B

    )( disENCLoloop

    IIldB +=• Define

    “displacement current”

    such that:

  • Modify Ampere’s Law

    Electricity & Magnetism Lecture 22, Slide 6

    A

    QE

    00

    ==

    0

    QEAE ==

    EQ = 0

    dt

    d

    td

    dQ E= 0

    DItd

    dQDefine:

  • Real Current: Charge Q passes through area A in time t:

    Displacement Current: Electric flux through area A changes in time

    Displacement Current

    Electricity & Magnetism Lecture 22, Slide 7

    dt

    dI ED

    = 0

    td

    dQI =

    )(dt

    dIldB EoENCLo

    loop

    +=•

  • A parallel plate capacitor has plates that are 2cm in diameter and 1mm apart. If the current into the capacitor is 0.5A, what is the magnetic field between the plates 0.5cm from the axis of the center of the plates?

    R

    r●

    I1

    Q1

    d

    Conceptual PlanUse modified Ampere’s Law

    Strategic PlanFind electric flux contained within circle with radius of 0.5cmFind time rate of change of that flux

    Example 22.1

    Electricity & Magnetism Lecture 22, Slide 8

    1cm

    0.5cm

  • R

    r●

    I1

    Q1

    d

    To calculate the magnetic field using the displacement current, I’m going to have the find the E flux over a certain area and the circumference of a particular circle. To find the B field at r = 0.5cm case, what is the area and what is that circle?

    a) area of a circle with r=0.5cm, circumference of a circle with r = 0.5cm

    b) area of a circle with r=1.0cm, circumference of a circle with r = 0.5cm

    c) area of a circle with r=0.5cm, circumference of a circle with r = 1.0cm

    Question

    Electricity & Magnetism Lecture 22, Slide 9

    1cm

    0.5cm

  • A parallel plate capacitor has plates that are 2cm in diameter and 1mm apart. If the current into the capacitor is 0.5A, what is the magnetic field between the plates 3.0 cm from the axis of the center of the plates?

    R

    r

    I1

    Q1

    Conceptual PlanUse modified Ampere’s Law

    Strategic PlanFind electric flux contained within circle with radius of 0.5cmFind time rate of change of that flux

    Example 22.1(b)

    Electricity & Magnetism Lecture 22, Slide 11

    1cm

    3cm

  • To calculate the magnetic field using the displacement current, I’m going to have the find the E flux over a certain area and the circumference of a particular circle. To find the B field at r = 3.0cm case, what is the area and what is that circle?

    a) area of a circle with r=3cm, circumference of a circle with r = 3cm

    b) area of a circle with r=1.0cm, circumference of a circle with r = 3cm

    c) area of a circle with r=3.0cm, circumference of a circle with r = 1.0cm

    Question

    Electricity & Magnetism Lecture 22, Slide 12

  • CheckPoint 1(A)

    Electricity & Magnetism Lecture 22, Slide 14

    At time t = 0 the switch in the circuit shown below is closed.

    Points A and B lie inside the capacitor; A is at the center and

    B is at the outer edge..

    A

    After the switch is closed, there will

    be a magnetic field at point A which

    is proportional to the current in the

    circuit.

    A. True

    B. False

  • CheckPoint 1(A)

    Electricity & Magnetism Lecture 22, Slide 15

    B is proportional to Ibut

    At A, B = 0 !!

    2

    10

    2 R

    rIB

    =

    At time t = 0 the switch in the circuit shown below is closed.

    Points A and B lie inside the capacitor; A is at the center and

    B is at the outer edge..

    A

    After the switch is closed, there will

    be a magnetic field at point A which

    is proportional to the current in the

    circuit.

    A. True

    B. False

  • Switch S has been open a long time when at t =0, it is closed. Capacitor C has circular plates of radius R. At time t = t1, a current I1 flows in the circuit and the capacitor carries charge Q1.

    What is the time dependence of the magnetic field B at a radius r between the plates of the capacitor?

    0 11 22

    I rB

    R

    =

    (A) (B) (C)

    Follow-Up

    Electricity & Magnetism Lecture 22, Slide 17

    S

    Ra

    V C

    A B C

  • Final form

    =•surface

    AdB 0

    •+=• AdEdtd

    IldB oENCLoloop

    •−=• AdBdtd

    ldEloop

    o

    enc

    surface

    QAdE

    =•

    Ta da!..... Maxwell’s Equations

    Unit 22, Slide 19

    Gauss’ Law

    Gauss’ Law for B fieldAmpere’s Law

    Faraday’s Law

  • Wave Equation

    Electricity & Magnetism Lecture 22, Slide 20

    Remember this guy? Not the spring constant!

    Remember from 2111??

  • Electricity & Magnetism Lecture 22, Slide 22

    ++

    --

    •−=• AdBdtd

    ldEloop

    Bhdxdt

    dhEd )*(* −=

    dx

    Bd

    dt

    d

    dx

    Ed

    −=2

    2

    •=• AdEdtd

    ldB ooloop

    o o

    dB dE

    dx dt = −

    Some Calculations

    dt

    dB

    dx

    Ed−=

    2 2

    2 2o o

    d E d E

    dx dt =

  • Welcome to Physics

    2112

    Hit “E” on your clicker

    Electricity & Magnetism Lecture 22, Slide 23

  • see PHYS 2115

    Electricity & Magnetism Lecture 22, Slide 24

    2 2

    2 2o o

    d E d E

    dx dt =

    A wave equation????

    oo

    v

    1=

    With a velocity of …?

    Some Calculations

  • Electricity & Magnetism Lecture 22, Slide 25

  • Electricity & Magnetism Lecture 22, Slide 26

  • Electricity & Magnetism Lecture 22, Slide 27

    The Sun

    Keep us warm Keep us safe

  • High Energy, Low Wavelength Low Energy, Long Wavelength

    What makes it through the atmosphere?

    Unit 15 Climate Science - Slide 28

  • Electricity & Magnetism Lecture 22, Slide 30

    Example 22.2

    An electromagnetic plane wave has a wavelength of

    0.100nm.

    a) What is its wave number, k?

    b) What is its frequency?

    c) What portion of the electro-magnetic spectrum

    does it fall in?

  • Electricity & Magnetism Lecture 22, Slide 32

    Past Confusion

    Nothing is moving here.

    Arrows only represent strength of field.

    Actually a plane wave.

  • CheckPoint 2(A)

    Electricity & Magnetism Lecture 22, Slide 33

    Ex = E0sin(kz − wt)

    E = E0 sin (kz − wt):E depends only on z coordinate for constant t. z coordinate is same for A, B, C.

    An electromagnetic plane wave is traveling in the +z direction. The

    illustration below shows this wave an some instant in time. Points A, B, and

    C have the same z coordinate.

    Compare the magnitudes of the electric field at points A and B.

    A. Ea < EbB. Ea = EbC. Ea > Eb

  • CheckPoint 2(A)

    Electricity & Magnetism Lecture 22, Slide 34

    Ex = E0sin(kz − wt)

    E = E0 sin (kz − wt):E depends only on z coordinate for constant t. z coordinate is same for A, B, C.

    An electromagnetic plane wave is traveling in the +z direction. The

    illustration below shows this wave an some instant in time. Points A, B, and

    C have the same z coordinate.

    Compare the magnitudes of the electric field at points A and B.

    A. Ea < EbB. Ea = EbC. Ea > Eb

  • CheckPoint 2(B)

    Electricity & Magnetism Lecture 22, Slide 35

    Ex = E0sin(kz − wt)

    E = E0 sin (kz − wt):E depends only on z coordinate for constant t. z coordinate is same for A, B, C.

    An electromagnetic plane wave is traveling in the +z direction. The

    illustration below shows this wave an some instant in time. Points A, B, and

    C have the same z coordinate.

    Compare the magnitudes of the electric field at points A and C.

    A. Ea < EcB. Ea = EcC. Ea > Ec

  • CheckPoint 2(B)

    Electricity & Magnetism Lecture 22, Slide 36

    Ex = E0sin(kz − wt)

    E = E0 sin (kz − wt):E depends only on z coordinate for constant t. z coordinate is same for A, B, C.

    An electromagnetic plane wave is traveling in the +z direction. The

    illustration below shows this wave an some instant in time. Points A, B, and

    C have the same z coordinate.

    Compare the magnitudes of the electric field at points A and C.

    A. Ea < EcB. Ea = EcC. Ea > Ec

  • Question

    Electricity & Magnetism Lecture 22, Slide 37

    Consider a point (x,y,z) at time t when Ex is negative and has its maximum value.

    At (x,y,z) at time t, what is By?

    A) By is positive and has its maximum valueB) By is negative and has its maximum valueC) By is zeroD) We do not have enough information

    Ex = E0sin(kz − wt)

  • Question

    Electricity & Magnetism Lecture 22, Slide 38

    Consider a point (x,y,z) at time t when Ex is negative and has its maximum value.

    At (x,y,z) at time t, what is By?

    A) By is positive and has its maximum valueB) By is negative and has its maximum valueC) By is zeroD) We do not have enough information

    Ex = E0sin(kz − wt)