روعه exellent p p reflection of light 2

25
Lecture 2: Reflection of Light: Mirrors (Ch 25) & Refraction of Light: Lenses (Ch 26)

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Page 1: روعه  Exellent P P  Reflection Of Light 2

Lecture 2:

Reflection of Light: Mirrors (Ch 25)&

Refraction of Light: Lenses (Ch 26)

Page 2: روعه  Exellent P P  Reflection Of Light 2

Light - Electromagnetic Wave

• Wavefronts• Rays• Plane waves

Page 3: روعه  Exellent P P  Reflection Of Light 2

Reflection of Light

The incident ray, the reflected ray, and the normal to the surface all lie in the same plane, and the angle of reflection equals the angle of incidence :

      

Page 4: روعه  Exellent P P  Reflection Of Light 2

Formation of images by a plane mirror

The image is upright. The image is the same size as you are. The image is located as far behind the mirror as you are in front of it.

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Spherical Mirror

CONCAVE Mirror

Focal length of concave mirror = ½ R

Spherical Aberration

Page 6: روعه  Exellent P P  Reflection Of Light 2

Spherical Mirror

Focal length of convex mirror = - ½ R

CONVEX mirror

Concave Solar Concentrators

Page 7: روعه  Exellent P P  Reflection Of Light 2

Formation of image by CONCAVE mirror

Ray 1, This ray is initially parallel to the principal axis and, therefore, passes through the focal point F after reflection from the mirror.

Ray 2.This ray initially passes through the focal point F and is reflected parallel to the principal axis. Ray 2 is analogous to ray 1 except that the reflected, rather than the incident, ray is parallel to the principal axis.

Ray 3.This ray travels along a line that passes through the center of curvature C and follows a radius of the spherical mirror; as a result, the ray strikes the mirror perpendicularly and reflects back on itself.

Page 8: روعه  Exellent P P  Reflection Of Light 2

Formation of image by CONCAVE mirror

Page 9: روعه  Exellent P P  Reflection Of Light 2

Formation of image by CONVEX mirror

An object placed in front of a convex mirror always produces a virtual image behind the mirror. The virtual image is reduced in size and upright.

Ray 1,This ray is initially parallel to the principal axis and, therefore, appears to originate from the focal point F after reflection from the mirror.Ray 2.This ray heads toward F, emerging parallel to the principal axis after reflection. Ray 2 is analogous to ray 1, except that the reflected, rather than the incident, ray is parallel to the principal axis.Ray 3.This ray travels toward the center of curvature C; as a result, the ray strikes the mirror perpendicularly and reflects back on itself.

Page 10: روعه  Exellent P P  Reflection Of Light 2

The Mirror Equation and MagnificationF = Focal lengthdo = Object distancedi = Image distancem = Magnification

                                                  

Concave mirror: The image distance is a positive quantity, as are the object distance and the focal length. If the Image is formed behind the mirror, the image distance is negative.

                                                                                                 

Page 11: روعه  Exellent P P  Reflection Of Light 2

Summary of Sign Conventions for Spherical Mirrors

Focal length f is + for a concave mirror. f is − for a convex mirror.

Object distance do is + if the object is in front of the mirror (real object). do is − if the object is behind the mirror (virtual object).

Image distance di is + if the image is in front of the mirror (real image). di is − if the image is behind the mirror (virtual image).

Magnification m is + for an image that is upright with respect to the object. m is − for an image that is inverted with respect to the object.

Page 12: روعه  Exellent P P  Reflection Of Light 2

Refraction and Snell’s Law

Index of Refraction: nv = c/n, where c = speed of light in vacuum

When light travels from a material with refractive index n1 into a material with refractive index n2, the refracted ray, the incident ray, and the normal to the interface between the materials all lie in the same plane. The angle of refraction is related to the angle of incidence by :

Page 13: روعه  Exellent P P  Reflection Of Light 2

More on refraction and its effects

Apparent depth: d’ = d (n2/n1)

Page 14: روعه  Exellent P P  Reflection Of Light 2

Snell’s Law Derivation

http://www.physics.northwestern.edu/vpl/optics/snell.html

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Total Internal Reflection                                                                            

Sparkle of Diamond Optical Fiber

Page 16: روعه  Exellent P P  Reflection Of Light 2

Dispersion                                                                            

Page 17: روعه  Exellent P P  Reflection Of Light 2

Lenses

Page 18: روعه  Exellent P P  Reflection Of Light 2

Formation of Image by Lenses

Page 19: روعه  Exellent P P  Reflection Of Light 2

Thin Lens Equation and Magnification

Page 20: روعه  Exellent P P  Reflection Of Light 2

Summary of Sign Conventions for Lenses

Focal length

f is + for a converging lens.f is − for a diverging lens.

Object distancedo is + if the object is to the left of the lens (real object), as is usual.do is − if the object is to the right of the lens (virtual object).

Image distancedi is + for an image (real) formed to the right of the lens by a real object.di is − for an image (virtual) formed to the left of the lens by a real object.

Magnificationm is + for an image that is upright with respect to the object.m is − for an image that is inverted with respect to the object.

Page 21: روعه  Exellent P P  Reflection Of Light 2

Lenses in Combination

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The Human Eye

Light travels through five different refractive index mediums before reaching the retina!

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Near and Farsightedness

Lasik: How does it work?

http://www.sankaranethralaya.org/lasik_work.htm

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The Compound Microscope

                                                                                                                                          

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The Telescope