james clerk maxwell (1831 – 1879)

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James Clerk Maxwell (1831 – 1879) In 1865, James Clerk Maxwell showed that light is comprised of both electricity and magnetism.

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James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves. Radio…not just AM & FM. AM vs FM radio. Frequency Modulated. Amplitude Modulated. Both AM & FM radio signals have advantages and disadvantages. - PowerPoint PPT Presentation

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Page 1: James Clerk Maxwell  (1831 – 1879)

James Clerk Maxwell (1831 – 1879)

• In 1865, James Clerk Maxwell showed that light is comprised of both electricity and magnetism.

Page 2: James Clerk Maxwell  (1831 – 1879)

Electromagnetic (light) Waves

c=fλ

Page 3: James Clerk Maxwell  (1831 – 1879)

The speed of the light wave remains constant in a given medium.

Page 4: James Clerk Maxwell  (1831 – 1879)

Radiowaves…not just AM & FM These light waves

are a few cm to several football fields in wavelength

Cordless phones, radios, garage door openers, RC toys.

Page 5: James Clerk Maxwell  (1831 – 1879)

AM vs FM radio

Frequency Modulated

Amplitude Modulated

Page 6: James Clerk Maxwell  (1831 – 1879)

• Both AM & FM radio signals have advantages and disadvantages.

• Generally, AM waves have much longer wavelengths than FM waves and can DIFFRACT better than FM waves and can travel greater distances before the signal fades. FM is more direct line of sight.

• However, because information is coded in the amplitude of an AM wave, power lines and lightning can influence the amplitude and are more likely to interfere with the AM wave.

• FM has a greater range of frequency which is better for music whereas AM is better for talk radio since there isn’t much fluctuation in a person’s voice.

Page 7: James Clerk Maxwell  (1831 – 1879)

Microwaves

Page 9: James Clerk Maxwell  (1831 – 1879)

Pit vipers, pythons, and boas possess special organs that form images in the brain of the thermal environment, much like vision occurs in the human brain. Thus, these snakes "see" heat, and this amazing system is the most sensitive infrared detector on Earth, natural or artificial.

Page 11: James Clerk Maxwell  (1831 – 1879)

Visible

Page 12: James Clerk Maxwell  (1831 – 1879)

Ultraviolet

Page 13: James Clerk Maxwell  (1831 – 1879)

X-RAYS• In 1895, W.C. Röntgen

discovered mysterious rays capable of passing through the human body.

• Mostly used for medical and industry

Page 14: James Clerk Maxwell  (1831 – 1879)

Gamma Ray• High-energy photons are emitted as one of

three types of radiation resulting from natural radioactivity. Differs from X-rays where radiation is emitted by excited nuclei rather than electrons

• Gamma ray sources are used for cancer treatment and for diagnostic purposes

• Highest energy EM wave, highest f, shortest wavelength, most penetrating, most damaging of all EM waves

Page 15: James Clerk Maxwell  (1831 – 1879)

Reflection and Refraction

Page 16: James Clerk Maxwell  (1831 – 1879)

Rays instead of waves A A rayray of light is an imaginary line drawn of light is an imaginary line drawn

along the direction of travel of the light along the direction of travel of the light beams. We use this instead of a wave.beams. We use this instead of a wave.

Page 17: James Clerk Maxwell  (1831 – 1879)

Law of Reflection

θi

The normal is a line perpendicular to the surface

Page 18: James Clerk Maxwell  (1831 – 1879)

Specular Reflection:

Page 19: James Clerk Maxwell  (1831 – 1879)

Diffuse Reflection:

Page 20: James Clerk Maxwell  (1831 – 1879)

With diffuse reflection, your eye sees reflected light at all angles. With specular reflection (from a mirror), your eye must be in the correct position.

Page 21: James Clerk Maxwell  (1831 – 1879)

Which photo demonstratesspecular reflection?

Page 22: James Clerk Maxwell  (1831 – 1879)

If water was smooth you would just see reflection of object as in picture at left. But the surface is rougher where waves act like an array of flat mirrors reflecting is such a way as shown below. The light then appears smeared into a long vertical column.

Sun & moon reflect in a line

Page 23: James Clerk Maxwell  (1831 – 1879)

Refraction of LightSame as waves/sound unit. Bending due to a speed change due to material change entering at an angle.

Identify #1-5

Page 24: James Clerk Maxwell  (1831 – 1879)

θi

θi

θrθr

θi>θr θi<θr

Page 25: James Clerk Maxwell  (1831 – 1879)

The Index of Refraction

Page 26: James Clerk Maxwell  (1831 – 1879)

Some Indices of RefractionSome Indices of Refraction

Page 27: James Clerk Maxwell  (1831 – 1879)

Snell’s Law of Refraction

Page 28: James Clerk Maxwell  (1831 – 1879)

ExampleExample: : A ray of light is incident on the surface of a block of clear ice (1.309) at an angle of 40.0° with the normal. Part of the light is reflected and part is refracted. Find the angle between the reflected and refracted light.

Page 29: James Clerk Maxwell  (1831 – 1879)

Example: The light emitted by a helium–neon laser has a wavelength of 632.8nm in air. As the light travels from air into zircon (1.923), finda) its speed in zircon

b) its frequency in zircon

c) its wavelength in zircon.

Page 30: James Clerk Maxwell  (1831 – 1879)

Illusions from refraction Objects appear ‘bent’ or

disjointed.

Page 31: James Clerk Maxwell  (1831 – 1879)

Objects appear ‘higher’

Our eye-brain system fools us and we conjure up an image since we cannot follow the path of refraction

Page 32: James Clerk Maxwell  (1831 – 1879)

Romantic Sunset not really there!? What will I tell my lover!!

Page 33: James Clerk Maxwell  (1831 – 1879)

Water on the road mirage

Page 35: James Clerk Maxwell  (1831 – 1879)
Page 36: James Clerk Maxwell  (1831 – 1879)

Dispersion

Page 37: James Clerk Maxwell  (1831 – 1879)

Variation of Index of Refraction with Wavelength• Violet light refracts

more than red light when passing from air into a material

Page 38: James Clerk Maxwell  (1831 – 1879)

Critical Angle

θc

Page 39: James Clerk Maxwell  (1831 – 1879)

Total Internal ReflectionWhen you exceed θC

Page 40: James Clerk Maxwell  (1831 – 1879)

Diamonds

 

Page 41: James Clerk Maxwell  (1831 – 1879)

Fiber Optics and T.I.R..

Page 42: James Clerk Maxwell  (1831 – 1879)
Page 43: James Clerk Maxwell  (1831 – 1879)

A bright underwater flood light at the bottom of a 2.75m deep pool is positioned 1.85m from one edge of the pool. At what angle will light emerge from the surface of the water at the edge of the pool with respect to ground. Assume the pool is filled to the brim with water.

light

ground

Page 44: James Clerk Maxwell  (1831 – 1879)

Image Types for Mirrors

Page 45: James Clerk Maxwell  (1831 – 1879)

Image characteristics:

A) TYPE –

B) ORIENTATION -

C) MAGNIFICATION (M) -

D) Position & height of image and object -

Page 46: James Clerk Maxwell  (1831 – 1879)

Reflection & Image Formation by a Plane Mirror

Page 47: James Clerk Maxwell  (1831 – 1879)

Characteristics of the Image Formed by a Plane/Flat Mirror

Page 48: James Clerk Maxwell  (1831 – 1879)

Concave Mirror

Page 49: James Clerk Maxwell  (1831 – 1879)

Parallel light rays reflecting off of concave mirror

Note how all 4 rays reflect and converge at common point. This is called FOCAL POINT.

Page 50: James Clerk Maxwell  (1831 – 1879)

Focal Length Incoming rays are parallel

and all reflect through a common point called the

The distance from the mirror to the focal point is called the

The focal length is ½ the

radius of curvature f= R/2

Page 51: James Clerk Maxwell  (1831 – 1879)

Applications of concave mirror:

SATELLITE DISH -

Behind flashlight bulbs, headlights, searchlights.

Page 52: James Clerk Maxwell  (1831 – 1879)

SOLAR COOKER

Page 53: James Clerk Maxwell  (1831 – 1879)

Convex Mirror

Page 54: James Clerk Maxwell  (1831 – 1879)

APPLICATIONS:

Page 55: James Clerk Maxwell  (1831 – 1879)

RAY DIAGRAMS

Page 56: James Clerk Maxwell  (1831 – 1879)

Object inside the focal point.

Characteristics of image:

Page 57: James Clerk Maxwell  (1831 – 1879)

IMAGE IN CONVEX MIRROR

Page 58: James Clerk Maxwell  (1831 – 1879)

Mirror equationMirror equation

Page 59: James Clerk Maxwell  (1831 – 1879)

MagnificationMagnification

Sign Convention: Reflective side of mirror is positive & back side of mirror is negative

Negative magnification or hi = inverted image

Page 60: James Clerk Maxwell  (1831 – 1879)

Example A concave makeup mirror is designed so that a

person 25cm in front of it sees an upright image magnified by a factor of two. What is the radius of curvature of the mirror?

Page 61: James Clerk Maxwell  (1831 – 1879)

How far from a concave mirror with a focal length of 22.5 cm must an object be placed to produce an image with a magnification of +3.65?

Example2

Page 62: James Clerk Maxwell  (1831 – 1879)

Thin Lenses

Page 63: James Clerk Maxwell  (1831 – 1879)

Converging or Convex Lenses (THICKER AT CENTER)

Page 64: James Clerk Maxwell  (1831 – 1879)

Parallel rays refract through converging lens and then proceed through F on other side.

Page 65: James Clerk Maxwell  (1831 – 1879)

Diverging or Concave Lenses (THICKER AT EDGES)

Page 66: James Clerk Maxwell  (1831 – 1879)

Parallel rays refract through diverging lens and then diverge where rays can be traced backwards through F on incident side.

Page 67: James Clerk Maxwell  (1831 – 1879)

Ray Diagram

Page 68: James Clerk Maxwell  (1831 – 1879)

Diverging lens

Page 69: James Clerk Maxwell  (1831 – 1879)

Sign convention for lenses

Where you expect light to end up is assumed positive (opposite side of lens)

Converging lenses have +f

Diverging lenses have -f

Page 70: James Clerk Maxwell  (1831 – 1879)

Example Based on the picture Based on the picture

shown, describe the shown, describe the type of lens and the type of lens and the type of imagetype of image

If the magnifying glass was immersed in water, If the magnifying glass was immersed in water, what effect (if any) would that have on the what effect (if any) would that have on the rays leaving the lens?rays leaving the lens?

Page 71: James Clerk Maxwell  (1831 – 1879)

APPLICATIONS OF LENSES• Overhead projector (lens + mirror),

eyeglasses, contacts, magnifying glass, telescopes, microscopes, your eye, etc

Page 72: James Clerk Maxwell  (1831 – 1879)

Lenses and your EYE

Page 73: James Clerk Maxwell  (1831 – 1879)

• The ability of the eye to instantly adjust its focal length is known as accommodation.

• Your ciliary muscles flex and manipulate the curvature and shape of your lens which changes the focal length of the lens.

Page 74: James Clerk Maxwell  (1831 – 1879)

Farsighted

Page 75: James Clerk Maxwell  (1831 – 1879)

Nearsighted

Page 76: James Clerk Maxwell  (1831 – 1879)

• Astigmatism means that the cornea is oval like a football instead of spherical like a basketball. This causes light to focus on more than one point in the eye, resulting in blurred vision at a distance or near.

Page 77: James Clerk Maxwell  (1831 – 1879)

Combinations of Lenses

Page 78: James Clerk Maxwell  (1831 – 1879)

Combination of Thin Lenses• The image produced by the first lens is calculated

as though the second lens were not present• The light then approaches the second lens as if it

had come from the image of the first lens• The image of the first lens is treated as the object

of the second lens• The image formed by the second lens is the final

image of the system

Page 79: James Clerk Maxwell  (1831 – 1879)

• If the image formed by the first lens lies on the back side of the second lens, then the image is treated at a virtual object for the second lensdo will be negative – virtual objects CAN form real

images

• The overall magnification is the product of the magnification of the separate lenses

Page 80: James Clerk Maxwell  (1831 – 1879)

ExampleAn object is located 4.75m from a simple optical system consisting of two converging lenses. The first lens of this system has a focal length of 100mm and the second lens, which is 20.0cm from the first lens, has a focal length of 150.0mm. What is the magnification of the system?

Page 81: James Clerk Maxwell  (1831 – 1879)

Example 2 An object is placed 20.0cm to the left of a

converging lens of focal length 25.0cm. A diverging lens of focal length 10.0cm is 25.0cm to the right of the converging lens. Find the position and magnification of the final image.