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Fermat’s principle:
Fermat’s principle:
“light travel b/w two points along the path that required the
least time as compared to other nearby path is called Fermat's
principle”
From Fermat's we determine:
 Law of reflection [i = r ]
 Law of refraction [
sin 𝜃1
sin 𝜃2
=n]
When light travel in the certain medium fall on the surface of other medium the part
of it turn back in the certain medium this is called reflection of light
Law of reflection:
 The incident ray, the
normal and the reflected
ray at the point of
incident all lie in the same
plane
 The angle of incident is
equal to the angle of
reflection
Normal
Plane mirror
i = r
𝜃1
𝜃2
The process of bending of light when it passes from one medium to other is called
refraction of light.
Law of refraction:
 The incident ray, the
normal and the reflected
ray at the point of
incident all lie in the same
plane
 The ratio of sin of angle
incident and sin of angle
of refraction are always
equal to constant.
Normal
Mirror slab
Normal
sin 𝜃1
sin 𝜃2
=n
𝜃1
𝜃2
Law of reflection:
x d-x
𝜃1
𝜃2
p
A
B
a b
d
N
sin𝜃1=
𝑎
𝑎2+𝑥2
sin𝜃2=
𝑑−𝑥
𝑏2+(𝑑−𝑥)2
sin𝜃1=
𝑝𝑒𝑝𝑒𝑛𝑑𝑖𝑐𝑢𝑙𝑎𝑟
ℎ𝑦𝑝𝑜𝑡𝑒𝑛𝑜𝑢𝑠
L= 𝑎2 + 𝑥2 + 𝑏2 + (𝑑 − 𝑥)2
AP= 𝑎2 + 𝑥2
PB= 𝑏2 + (𝑑 − 𝑥)2
L=AP+PB
𝑑𝐿
𝑑𝑥
=
2𝑥
2 𝑎2+𝑥2
+
2(𝑑−𝑥)(−1)
2 𝑏2+(𝑑−𝑥)2
𝑑𝐿
𝑑𝑥
=0
0=
2𝑥
2 𝑎2+𝑥2
+
2(𝑑−𝑥)(−1)
2 𝑏2+(𝑑−𝑥)2
0=
𝑥
𝑎2+𝑥2
-
(𝑑−𝑥)
𝑏2+(𝑑−𝑥)2
𝑥
𝑎2+𝑥2
=
(𝑑−𝑥)
𝑏2+(𝑑−𝑥)2
See from finger the equation
become
sin𝜃1= sin𝜃2
i = r
So it is proved
Law of refraction:
x
d-x
𝜃1
𝜃2
p
A
B
a
b
d
Nsin𝜃1=
𝑎
𝑎2+𝑥2
sin𝜃2=
𝑑−𝑥
𝑏2+(𝑑−𝑥)2
Ttotal=tAP+tPB
𝑑𝑡
𝑑𝑥
=0
0=
2𝑥
2𝑣1 𝑎2+𝑥2
+
2(𝑑−𝑥)(−1)
2𝑣2 𝑏2+(𝑑−𝑥)2
0=
𝑥
𝑣1 𝑎2+𝑥2
-
(𝑑−𝑥)
𝑣2 𝑏2+(𝑑−𝑥)2
𝑥
𝑣1 𝑎2+𝑥2
=
(𝑑−𝑥)
𝑣2 𝑏2+(𝑑−𝑥)2
See from finger the equation
become
sin𝜃1 𝑣1= sin𝜃2 𝑣2
So it is proved
t=
𝑠
𝑣
t=
𝐴𝑃
𝑣1
+
𝑃𝐵
𝑣2
t=
𝑎2+𝑥2
𝑣1
+
𝑏2+(𝑑−𝑥)2
𝑣2
𝑑𝑡
𝑑𝑥
=
2𝑥
2𝑣1 𝑎2+𝑥2
+
2(𝑑−𝑥)(−1)
2𝑣2 𝑏2+(𝑑−𝑥)2
sin 𝜃1
sin 𝜃2
=
𝑣1
𝑣2
sin 𝜃1
sin 𝜃2
=n
sin𝜃1=
𝑝𝑒𝑝𝑒𝑛𝑑𝑖𝑐𝑢𝑙𝑎𝑟
ℎ𝑦𝑝𝑜𝑡𝑒𝑛𝑜𝑢𝑠
Reflection through spherical mirror :
Spherical mirror:
A mirror whose polished reflecting surface is a part of hollow sphere is called
spherical mirror
There are two types of
spherical mirrors:
 Concave mirror
 Convex mirror
Concave mirror:
A spherical mirror whose inner side is reflecting is called concave mirror
 Size of image depend upon the
position of object.
 Both real and virtual image form by
concave mirror.
 Focus form in the front of mirror f
c
Convex mirror:
A spherical mirror whose outer side is reflecting is called convex mirror
 Size of image of object always smaller
then object.
 Only virtual image are formed
 Focus lie behind the mirror
f
c

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Reflection refraction

  • 1.
  • 3. Fermat’s principle: “light travel b/w two points along the path that required the least time as compared to other nearby path is called Fermat's principle” From Fermat's we determine:  Law of reflection [i = r ]  Law of refraction [ sin 𝜃1 sin 𝜃2 =n]
  • 4. When light travel in the certain medium fall on the surface of other medium the part of it turn back in the certain medium this is called reflection of light Law of reflection:  The incident ray, the normal and the reflected ray at the point of incident all lie in the same plane  The angle of incident is equal to the angle of reflection Normal Plane mirror i = r 𝜃1 𝜃2
  • 5. The process of bending of light when it passes from one medium to other is called refraction of light. Law of refraction:  The incident ray, the normal and the reflected ray at the point of incident all lie in the same plane  The ratio of sin of angle incident and sin of angle of refraction are always equal to constant. Normal Mirror slab Normal sin 𝜃1 sin 𝜃2 =n 𝜃1 𝜃2
  • 6. Law of reflection: x d-x 𝜃1 𝜃2 p A B a b d N sin𝜃1= 𝑎 𝑎2+𝑥2 sin𝜃2= 𝑑−𝑥 𝑏2+(𝑑−𝑥)2 sin𝜃1= 𝑝𝑒𝑝𝑒𝑛𝑑𝑖𝑐𝑢𝑙𝑎𝑟 ℎ𝑦𝑝𝑜𝑡𝑒𝑛𝑜𝑢𝑠 L= 𝑎2 + 𝑥2 + 𝑏2 + (𝑑 − 𝑥)2 AP= 𝑎2 + 𝑥2 PB= 𝑏2 + (𝑑 − 𝑥)2 L=AP+PB 𝑑𝐿 𝑑𝑥 = 2𝑥 2 𝑎2+𝑥2 + 2(𝑑−𝑥)(−1) 2 𝑏2+(𝑑−𝑥)2 𝑑𝐿 𝑑𝑥 =0 0= 2𝑥 2 𝑎2+𝑥2 + 2(𝑑−𝑥)(−1) 2 𝑏2+(𝑑−𝑥)2 0= 𝑥 𝑎2+𝑥2 - (𝑑−𝑥) 𝑏2+(𝑑−𝑥)2 𝑥 𝑎2+𝑥2 = (𝑑−𝑥) 𝑏2+(𝑑−𝑥)2 See from finger the equation become sin𝜃1= sin𝜃2 i = r So it is proved
  • 7. Law of refraction: x d-x 𝜃1 𝜃2 p A B a b d Nsin𝜃1= 𝑎 𝑎2+𝑥2 sin𝜃2= 𝑑−𝑥 𝑏2+(𝑑−𝑥)2 Ttotal=tAP+tPB 𝑑𝑡 𝑑𝑥 =0 0= 2𝑥 2𝑣1 𝑎2+𝑥2 + 2(𝑑−𝑥)(−1) 2𝑣2 𝑏2+(𝑑−𝑥)2 0= 𝑥 𝑣1 𝑎2+𝑥2 - (𝑑−𝑥) 𝑣2 𝑏2+(𝑑−𝑥)2 𝑥 𝑣1 𝑎2+𝑥2 = (𝑑−𝑥) 𝑣2 𝑏2+(𝑑−𝑥)2 See from finger the equation become sin𝜃1 𝑣1= sin𝜃2 𝑣2 So it is proved t= 𝑠 𝑣 t= 𝐴𝑃 𝑣1 + 𝑃𝐵 𝑣2 t= 𝑎2+𝑥2 𝑣1 + 𝑏2+(𝑑−𝑥)2 𝑣2 𝑑𝑡 𝑑𝑥 = 2𝑥 2𝑣1 𝑎2+𝑥2 + 2(𝑑−𝑥)(−1) 2𝑣2 𝑏2+(𝑑−𝑥)2 sin 𝜃1 sin 𝜃2 = 𝑣1 𝑣2 sin 𝜃1 sin 𝜃2 =n sin𝜃1= 𝑝𝑒𝑝𝑒𝑛𝑑𝑖𝑐𝑢𝑙𝑎𝑟 ℎ𝑦𝑝𝑜𝑡𝑒𝑛𝑜𝑢𝑠
  • 8. Reflection through spherical mirror : Spherical mirror: A mirror whose polished reflecting surface is a part of hollow sphere is called spherical mirror There are two types of spherical mirrors:  Concave mirror  Convex mirror Concave mirror: A spherical mirror whose inner side is reflecting is called concave mirror  Size of image depend upon the position of object.  Both real and virtual image form by concave mirror.  Focus form in the front of mirror f c
  • 9. Convex mirror: A spherical mirror whose outer side is reflecting is called convex mirror  Size of image of object always smaller then object.  Only virtual image are formed  Focus lie behind the mirror f c