james clerk maxwell (1831 – 1879). electromagnetic (light) waves

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James Clerk Maxwell (1831 – 1879)

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Page 1: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

James Clerk Maxwell (1831 – 1879)

Page 2: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Electromagnetic (light) Waves

Page 3: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves
Page 4: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Radio…not just AM & FM

Page 5: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

AM vs FM radio

Frequency Modulated

Amplitude Modulated

Page 6: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

• 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). Electromagnetic (light) Waves

Microwaves

Page 8: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Infrared

Page 9: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Thermogram

We radiate infrared light aka “heat”

Page 10: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Visible

Page 11: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Ultraviolet

Page 12: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

X-RAYS

Page 13: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Gamma Ray

Page 14: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Reflection and RefractionReflection and Refraction

of Lightof Light

Page 15: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Rays instead of waves Rays instead of waves approximationapproximation

• 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 16: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Law of ReflectionLaw of Reflection

θi θr

Page 17: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

2 types of reflection:2 types of reflection:

Page 18: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves
Page 19: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

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 20: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Refraction of LightRefraction of LightWhen a ray of light enters a different medium at an angle other than 0o with the normal, it will bend or REFRACT due to a speed change due to material change.

Page 21: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

θiθi

θr

θr

θi>θr θi<θr

Page 22: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

The Index of RefractionThe Index of Refraction

Page 23: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Snell’s Law of Refraction

Page 24: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

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

Page 25: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Frequency Between MediaFrequency Between Media

Page 26: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

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), find

a) its speed in zircona) its speed in zirconb) its frequency inb) its frequency in zirconzirconc) its wavelength in zircon.c) its wavelength in zircon.

Page 27: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Illusions from refractionIllusions from refraction

Page 28: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves
Page 29: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Sunset not really there?Sunset not really there?

Page 30: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

MirageMirage

Page 31: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

DispersionDispersion

Page 32: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Variation of Index of Refraction with Variation of Index of Refraction with WavelengthWavelength

Page 33: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Critical AngleCritical Angle

Page 34: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Total Internal ReflectionTotal Internal Reflection

Page 35: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

TIR and ‘bling bling’

 

Page 36: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Fiber Optics and TIRFiber Optics and TIR

• Plastic or glass rods Plastic or glass rods are used to “pipe” are used to “pipe” light from one place to light from one place to anotheranother

• This ‘light’ can be This ‘light’ can be used to carry used to carry information at light information at light speedspeed

• Fiber Optics, Medical Fiber Optics, Medical EndoscopesEndoscopes

Page 37: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

The RainbowThe Rainbow

Page 38: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Observing the RainbowObserving the Rainbow

• If a raindrop high in the sky is observed, the red ray is seenIf a raindrop high in the sky is observed, the red ray is seen• A drop lower in the sky would direct violet light to the observerA drop lower in the sky would direct violet light to the observer• The other colors of the spectra lie in between the red and the The other colors of the spectra lie in between the red and the

violetviolet

Page 39: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

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

Page 40: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

MIRRORS

Page 41: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Image Types for MirrorsImage Types for Mirrors

Page 42: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Image characteristics:A) TYPE –

B) ORIENTATION

C) MAGNIFICATION (M)

D) Position & height of image and object

Page 43: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Reflection & Image Formation by a Plane Mirror

What you see when you look into a plane (flat) mirror is an image, which appears to be behind the mirror.

Page 44: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Properties of the Image Formed by a Plane/Flat Mirror

Page 45: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Concave Mirror

Converges light rays after reflection

Page 46: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Parallel light rays reflecting off of Parallel light rays reflecting off of concave mirrorconcave mirror

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

Page 47: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Focal Length

Incoming rays are parallel and all reflect through a common point called the FOCAL POINT, F.

Page 49: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Convex MirrorConvex Mirror

Diverges light rays after reflection

Page 50: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

APPLICATIONS:

Page 51: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

RAY DIAGRAMS

Page 52: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Object inside the focal point.

Characteristics of image:

Page 53: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

IMAGE IN CONVEX MIRROR

Page 54: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Mirror equationMirror equation

Page 55: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

MagnificationMagnification

Page 56: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

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 57: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

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 58: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Thin Lenses

Use same formulas as mirrors, except that f ≠ R/2…doesn’t apply

Page 59: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Converging or Convex Lenses The difference

between mirrors and lenses is that mirrors reflect and lenses refract light.

Page 60: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

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

Page 61: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Diverging or Concave Lenses (THICKER AT EDGES)

Page 62: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

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

Page 63: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Ray Diagram

Page 64: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Diverging lens

Page 65: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

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 66: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

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

Page 68: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Lenses and your EYE

Page 69: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

• 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 70: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Farsighted

Page 71: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Nearsighted

Page 72: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

• 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 73: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Combinations of Lenses

Page 74: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

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 75: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

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 100 mm and the second lens, which is 20.0 cm from the first lens, has a focal length of 150.0 mm. What is the magnification of the system?

Page 76: James Clerk Maxwell (1831 – 1879). Electromagnetic (light) Waves

Example 2

An object is placed 20.0 cm to the left of a converging lens of focal length 25.0 cm. A diverging lens of focal length 10.0 cm is 25.0 cm to the right of the converging lens. Find the position and magnification of the final image.