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    Law of Reflection

    Dispersion

    Snells Law

    Brewsters Angle

    Preliminary topics before

    mirrors and lenses

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    Law of ReflectionDispersion

    Snells Law

    Brewsters Angle

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    Geometrical Optics:Study of reflection and refractionof light from surfaces

    The ray approximation states that light travels in straight lines

    until it is reflected or refracted and then travels in straight lines again.

    The wavelength of light must be small compared to the size of

    the objects or else diffractive effects occur.

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    Law of Reflection

    1A

    B

    I = qR

    i

    r

    Mirror

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    Drawing Normals

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    Fermats Principle

    Using Fermats Principle you can prove theReflection law. It states that the path taken

    by light when traveling from one point to

    another is the path that takes the shortest

    time compared to nearby paths.

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    Two light rays 1 and 2 taking different paths

    between points A and B and reflecting off a

    vertical mirror

    1

    2

    A

    B Plane Mirror

    Use calculus - method

    of minimization

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    t= 1

    ( 12 + 2 + 2

    2 + ( )2 )

    =

    2

    12 + 2

    +2( )

    22 + ( )2 )

    = 0

    y

    h12 + 2=

    ( )

    22 + ( )2 )

    =

    I=

    qR

    Write down time as a function of y

    and set the derivative to 0.

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    Law of Refraction: Snells Law

    n1 sinq1 = n2 sinq2

    n1n2

    How do we prove it?

    1

    v1

    sin1=

    1

    2

    2

    Air 1.0

    Glass 1.33

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    t= ( 1112 + 2 + 12

    22 + ( )2 )

    = 0

    11

    =12

    n1 sin

    = 2

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    JAVA APPLET

    Show Fermats principle simulator

    http://www.aug.edu/~chmtmc/ntnujava/Fermat/Fermat.htmlhttp://www.aug.edu/~chmtmc/ntnujava/Fermat/Fermat.html
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    What allows you to see various colors when

    white light passes through a prism

    Dispersion

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    How does a Rainbow work?

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    Why is light totally reflected inside a fiber

    optics cable? Internal reflection

    n1

    sinq1

    = n2

    sinq2

    (1.33) sinq1 = (1.00) sin 90 = 1.00

    When 1 1 1

    1.33 48.75

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    Fiber Cable

    Same here

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    Corner Reflector?

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    Show Total Internal reflection

    simulator

    Halliday, Resnick, Walker: Fundamentals of Physics, 7th Edition -

    http://bcs.wiley.com/he-bcs/Books?action=chapter&bcsId=2037&itemId=0471216437&chapterId=12950http://bcs.wiley.com/he-bcs/Books?action=chapter&bcsId=2037&itemId=0471216437&chapterId=12950
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    What causes a Mirage

    1.06

    1.09

    1.08

    1.07 1.07

    1.08

    1.09

    sky eye

    Hot road causes gradient in the index of refraction that increases

    as you increase the distance from the road

    Index of refraction

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    Inverse Mirage Bend

    Snells Law Example

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    47. In the figure, a 2.00-m-long vertical pole extends from the bottom

    of a swimming pool to a point 50.0 cm above the water. What is the

    length of the shadow of the pole on the level bottom of the pool?

    Consider a ray that grazes the top of the

    pole, as shown in the diagram below. Here

    1 = 35o, l1 = 0.50 m, and l2 = 1.50 m.

    2

    1

    l2

    l1

    L x

    air

    water

    shadow

    x is given by

    x = l1tan 1 = (0.50m)tan35o = 0.35 m.

    The length of the shadow is x + L.

    L is given by

    L=l2tan 2

    Use Snells Law to find 2

    Snells Law Example

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    According to the law of refraction, n2sin 2 =

    n1sin 1. We take n1 = 1 and n2 = 1.33

    oo

    n55.25

    33.1

    35sinsin

    sinsin 1

    2

    11

    2 =

    =

    =

    L is given by

    .72.055.25tan)50.1(tan 22 mmlLo ===

    The length of the shadow is L+x.

    L+x = 0.35m + 0.72 m = 1.07 m.

    2

    1

    l2

    l1

    L x

    air

    water

    shadow

    Calculation of L

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    Polarization by Reflection Brewsters Law

    (1.)sin = + = 90 100% = (90 ) = = 1

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    Plane Mirrors Where is the image formed

    Mirrors and Lenses

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    Plane mirrors

    Normal

    Angle of

    incidence

    Angle of reflection

    i = - p

    Real side Virtual side

    Virtual image

    eye

    Object distance = - image distance

    Image size = Object size

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    Problem: Two plane mirrors make an angle of 90o. How

    many images are there for an object placed between

    them?

    object

    eye

    1

    2

    3

    mirror

    mirror

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    Problem: Two plan mirrors make an angle of 60o. Find all

    images for a point object on the bisector.

    object

    2

    4

    5,6

    3

    1

    mirror

    mirror

    eye

    U i th L f R fl ti t

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    pocket

    Assuming no spinAssuming an elastic collision

    No cushion deformation

    d

    d

    Using the Law of Reflection to

    make a bank shot

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    What happens if we bend the mirror?

    i = - p magnification = 1

    Concave mirror.

    Image gets magnified.

    Field of view is diminished

    Convex mirror.

    Image is reduced.

    Field of view increased.

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    Rules for drawing images for mirrors

    Initial parallel ray reflects through focal point.Ray that passes in initially through focal point reflects parallel

    from mirrorRay reflects from C the radius of curvature of mirror reflects along

    itself. Ray that reflects from mirror at little point c is reflected

    symmetrically

    1

    p +

    1

    =1

    =

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    Concept Simulator/Illustrations

    Halliday, Resnick, Walker: Fundamentals of Physics, 7th Edition -

    S h i l f i f

    http://bcs.wiley.com/he-bcs/Books?action=chapter&bcsId=2037&itemId=0471216437&chapterId=12950http://bcs.wiley.com/he-bcs/Books?action=chapter&bcsId=2037&itemId=0471216437&chapterId=12950
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    Spherical refracting surfaces

    n1

    p+2

    =2 1

    Using Snells Law and assuming small

    Angles between the rays with the central

    axis, we get the following formula:

    A l thi ti t Thi L h th thi k i

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    Apply this equation to Thin Lenses where the thickness is

    small compared to object distance, image distance, and

    radius of curvature. Neglect thickness.

    Converging lens

    Diverging lens

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    Thin Lens Equation

    1

    f=

    1

    p+

    1

    i

    Lensmaker Equation

    1

    f= (n - 1)(

    1

    r1-1

    r2)

    What is the sign convention?

    Lateral Magnification for a Lensm =

    Sign Convention

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    Sign Convention

    p

    Virtual side - V Real side - R

    i

    Light

    Real object - distance p is pos on V side (Incident rays are diverging)

    Radius of curvature is pos on R side.

    Real image - distance is pos on R side.

    Virtual object - distance is neg on R side. Incident rays are converging)

    Radius of curvature is neg on the V side.

    Virtual image- distance is neg on the V side.

    r2r1

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    Rules for drawing rays to locate images from

    a lens

    A ray initially parallel to the central axis will pass through the focal point.

    A ray that initially passes through the focal point will emerge from the lens

    parallel to the central axis.

    A ray that is directed towards the center of the lens will go straight

    through the lens undeflected.

    E l f d i i

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    Example of drawing images

    Example

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    24(b). Given a lens with a focal length f = 5 cm and object distance p

    = +10 cm, find the following: i and m. Is the image real or virtual?

    Upright or inverted? Draw 3 rays.

    pfi

    111=

    m =y

    y= -

    i

    p

    1

    i=1

    5-

    1

    10= +

    1

    10

    Image is real,inverted.

    . .F1 F2p

    Virtual side Real side

    m = -10

    10= - 1

    i = +10 cm

    Example

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    24(e). Given a lens with the properties (lengths in cm) r1 = +30, r2 =

    -30, p = +10, and n = 1.5, find the following: f, i and m. Is the image

    real or virtual? Upright or inverted? Draw 3 rays.

    ( )

    =

    21

    111

    1

    rrn

    f

    ( )30

    1

    30

    1

    30

    115.1

    1=

    ---=

    f

    cmf 30=

    pfi

    111=

    15

    1

    10

    1

    30

    11==

    cmi 15=

    m =y

    y= -

    i

    p

    m = -- 15

    10= +1.5

    Image is virtual,

    upright.

    Virtual sideReal side

    r1. .F1 F2p

    r2

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    27. A converging lens with a focal length of +20 cm is located 10 cm to

    the left of a diverging lens having a focal length of -15 cm. If an object is

    located 40 cm to the left of the converging lens, locate and describe

    completely the final image formed by the diverging lens. Treat each lensSeparately.

    f1

    f1

    Lens 1 Lens 2

    f2

    f2

    10

    40

    +20 -15

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    f1

    f1

    Lens 1 Lens 2

    f2

    f2

    10

    40

    +20 -15

    Ignoring the diverging lens (lens 2), the image formed by the

    converging lens (lens 1) is located at a distance1

    i1

    =1

    f1

    -1

    p1

    =1

    20cm-

    1

    40cm. i1 = 40cm

    40

    This image now serves as a virtual object for lens 2, with p2 = - (40 cm - 10 cm) = - 30 cm.

    30

    Since m = -i1/p1= - 40/40= - 1 , the image is inverted

    L 1 L 2

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    1

    i2

    =1

    f2

    -1

    p2

    =1

    - 15cm

    -1

    - 30cm

    i2=-30cm.

    Thus, the image formed by lens 2 is located 30 cm to the left of lens 2. It is

    virtual (since i2 < 0).

    f1

    f1

    Lens 1 Lens 2

    f2

    f2

    10

    40

    +20 -15

    40

    30

    The magnification is m = (-i1/p1) x (-i2/p2) = (-40/40)x(30/-30) =+1, so the image

    has the same size orientation as the object.

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    Optical Instruments

    Magnifying lens

    Compound microscope

    Refracting telescope