MK Fisika Dasar 2_Bab15

Post on 18-Feb-2018

225 views 0 download

Transcript of MK Fisika Dasar 2_Bab15

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 1/44

MK FISIKA DASAR 2ENGE600004

4 SKS

Rachmat Andika

Multiferroic Research Group

Departemen FisikaFMIPA - UI

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 2/44

THE NATURE OF LIGHT AND

THE LAWS OF

GEOMETRIC OPTICS

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 3/44

MATERI

The Nature of Light

Dualism of Light

The Speed of Light

Reflection and Refraction Total Internal Reflection

Dispersion

Huygens’s Principle

Fermat’s Principle

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 4/44

THE NATURE OF LIGHT

The light can propagate in a vacuum media

The light has a wave properties, such as Reflection

Refraction

In seeing something, the light has an important role

for our eyes

 A rainbow is one of the product of light that dispersed

by rain/ water

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 5/44

HISTORICAL OF LIGHT

Newton Light was considered to be a stream of particles that was emitted by

the object

He could explain reflection and refraction

Huygens (1678) Wave theory could also explain reflection and refraction

 Young (1801) Light rays interfere with each other and it couldn’t be explained by a

particle theory

Maxwell Light was a form of high-frequency electromagnetic waves

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 6/44

BUT ….

They could not explain some subsequent experiments,

such as

Where the constant of proportionality h = 6.63 x 10-34 Js

Photoelectric Effect

Max Planck (1900) → Einstein (1905)

The quantization model assumes that the energy of a

light wave is present in particles called photons

Is light a wave or

particle?

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 7/44

THE RAY APPROXIMATION IN

GEOMETRIC OPTICS

In the ray approximation, we assume that a wave moving through a

medium travels in a straight line in the direction of its rays

λ >> d, the rays continue in a straight-line path, and the ray

approximation remains valid

λ ≈ d, the rays spread out after passing through the opening λ << d, the opening behaves as a point source emitting spherical

waves

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 8/44

WAVE FRONT

To simplify light as a wave

Wave front is every point on wave crest

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 9/44

REFLECTION

The direction of a reflected ray is in the plane

perpendicular to the reflecting surface that contains the

incident ray

Specular reflection on a

smooth surface

diffuse reflection on a

rough surface

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 10/44

LAW OF REFLECTION

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 11/44

THE DIFFERENT BETWEEN

REFLECTIONS

For diffuse reflection, the eyes could see the light

reflection on all angles

For specular reflection, the eyes should have to

on the right position with respect to the light

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 12/44

EXAMPLE

Two mirrors make an angle of 120o with each other. A

ray is incident on mirror M1 at an angle 65o to the

normal. Find the direction of the ray after it is

reflected from mirror M2?

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 13/44

REFRACTION

When a ray of light traveling through a transparent

medium encounters a boundary leading into another

transparent medium,part of energy isreflected andpart 

 enters the second medium

The ray that enters the secondmedium is bent at the boundary

 A basic definition of refracted

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 14/44

(a) The light is bent toward the normal

(b)

The light is bent away from the normal

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 15/44

INDEX OF REFRACTION

In general, the speed of light in any material is less than its

speed in vacuum.

In fact, light travels at its maximum speed in vacuum.

Index of refraction is a dimensionless number greater than unity Becausev is always less thanc.

n is equal to unity for vacuum

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 16/44

SNELL’S LAW OF REFRACTION

 As light travels from one medium to

another, its frequency does not change

but its wavelength

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 17/44

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 18/44

EXAMPLE

 A beam of light of wavelength 550 nm traveling in air

is incident on a slab of transparent material. The

incident beam makes an angle of 40.0o with the

normal, and the refracted beam makes an angle of

26.0o

 with the normal. Find the index of refraction of the material

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 19/44

EXAMPLE

 A light ray of wavelength 589 nm traveling through

air is incident on a smooth, flat slab of crown glass at

an angle of 30.0o to the normal Find the angle of refraction

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 20/44

EXAMPLE

 A laser in a compact disc player generates light that

has a wavelength of 780 nm in air. Find the speed of this light once it enters the plastic of a

compact disc (n = 1.55)

What is the wavelength of this light in the plastic

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 21/44

 Angle of deviation

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 22/44

HUYGEN’S

PRINCIPLE

 All points on a given wave front are taken as point sources for theproduction of spherical secondary waves, calledwavelets, which

propagate outward through a medium with speeds characteristics of

waves in that medium.

 After some time interval has passed, the new position of the wave front

is the surface tangent to the wavelets

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 23/44

DISPERSION AND PRISMS

Index of refraction varies with the wavelength of the light passing

through the material. “ Dispersion”

Snell’s law of refraction indicates that light of different wavelength isbent atdifferent angles when incident on a refracting material.

 Angle of deviation is an angle between a ray of single wavelength

incident on the prism from the left emerges refracted from its original

direction of travel

 Angle of

deviation

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 24/44

 Visible spectrum

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 25/44

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 26/44

MEASURING INDEX OF

 REFRACTION USING A PRISM

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 27/44

TOTAL INTERNAL REFLECTION

Total internal reflection can occur when light is

directed from a medium having a given index of

refraction toward one having alower index of

refraction

θc : critical angle

The refracted light ray

moves parallel to the

boundary, θ2 = 90o

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 28/44

EXAMPLE

Find the critical angle for an air-water boundary

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 29/44

FERMAT’S PRINCIPLE

Fermat’s principle states that when a light ray travels

between any two points, its path is the one that requiresthe smallest time interval

PIERRE DE FERMAT(1601-1665)

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 30/44

IMAGE FORMATION

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 31/44

MATERI

Images formed by flat mirrors

Images formed by spherical mirrors

Images formed by refraction

Thin LensesLens Aberrations

Optics Systems

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 32/44

IMAGES FORMED BY FLAT MIRRORS

Images are classified as areal orvirtual

 A real image is formed when light rays pass through and diverge from

the image point

 A virtual image is formed when the light rays do not pass through theimage point but only appear to diverge from that point

the image of an object seen in a

flat mirror isalways virtual

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 33/44

The image is as far behind the mirror as the object isin front

The image is unmagnified, virtual, and upright

The image has front-back reversal

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 34/44

IMAGES FORMED BY SPHERICAL

MIRRORS

Concave mirror Mirror, in which light is reflected from the inner, concave

surface

Concave mirror is sometimes called aconverging mirror,

because the rays from any point on an object converge after

reflection

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 35/44

IMAGES FORMED BY SPHERICAL

MIRRORS

Convex mirror Mirror, in which light is reflected from the outer, convex

surface

Convex mirror is sometimes called adiverging mirror,

because the rays from any point on an object diverge after

reflection

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 36/44

MIRROR EQUATION

fis focal length,

fis usually not the point at which the light rays focus to form an image.the focal point is determined by the curvature of the mirror

It doesn’t depend on the location of the object at all

Or doesn’t depend on the material of mirror

 But it is different for lenses

The light actually passes through the

material and the focal length depends on the

type of material of the lens

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 37/44

RAY DIAGRAMS FOR MIRRORS

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 38/44

RAY DIAGRAM OF CONCAVE

MIRRORS

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 39/44

RAY DIAGRAM OF CONVEX MIRRORS

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 40/44

THIN LENSES

Lens makers’ equation

Lenses are used to form images by refraction

in optical instruments, such as cameras,

telescopes, and microscopes

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 41/44

RAY DIAGRAM FOR THIN LENSES

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 42/44

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 43/44

EXERCISE

Two thin converging lenses of focal lengths f1 = 10 cm

and f2 = 20 cm are separated by 20 cm. an object is

placed 30 cm to the left of lens 1. Find the position

and the magnification of the final image.

7/23/2019 MK Fisika Dasar 2_Bab15

http://slidepdf.com/reader/full/mk-fisika-dasar-2bab15 44/44