LIGHT, CBSE CLASS X, PHYSICS NOTES PART III
CBSE CLASS 10, LIGHT, PHYSICS NOTES-(PART III)
LIGHT
According to the CBSE Syllabus 2025-26
CBSE Class 10 Science Chapter 10 Light Notes
Remaining Topics of this Chapter
8. Uses of a concave mirror.
9. Ray diagram of the image formed by the convex mirror.
-When an object is placed at infinity.
-When an object is placed between the pole and infinity.
10. Uses of a convex mirror.
11. Sign convention for reflection by a spherical mirror.
12. Mirror formulas.
-Magnification of a spherical mirror.
USES OF CONCAVE MIRROR
Concave and Convex
mirrors are used for many daily purposes.
(i)
Used in torches, search lights and vehicles headlights to get powerful parallel
beam of light.
(ii)
Concave mirrors are used by dentists to see large image of teeth of patients.
(Teeth have to be placed between pole and focus).
(iii)
Concave mirror is used as shaving mirror to see a larger image of the face.
(iv)
Large concave mirrors are used to concentrate sunlight to produce heat in solar
furnace.
Ray diagrams of images formed by convex mirror
(i) When object is placed at infinity
Image
Position − At ‘F’
Nature
of image – Virtual, erect
Size
– Point sized
(ii) When object is placed between pole and infinity
Image
Position – Between ‘P’ and ‘F’
Nature
of image– Virtual, erect
Size
– Diminished
A
full length image of a tall building/tree can be seen in a small convex mirror.
USES OF CONVEX MIRROR
(i) Convex mirrors are used as rear view mirrors in vehicles because
a. they always give an erect though diminished
image.
b. they have a wider field of view as they are
curved outwards.
(ii) Convex mirrors are used at blind turns and
on points of merging traffic to facilitate vision of both side traffic.
(iii) Used in shops as security mirror.
SIGN CONVENTION FOR REFLECTION BY SPHERICAL
MIRROR
(i) The object is placed to the left of the mirror.
(ii) All distances parallel to the principal
axis are measured from the pole of the mirror.
(iii) All distances measured in the direction of
incident ray (along + X-axis) are taken as positive and those measured against
the direction of incident ray (along – X-axis) are taken as negative.
(iv) Distance measured perpendicular to and
above the principal axis are taken as positive.
(v) Distances measured perpendicular to and
below the principal axis are taken as negative.
• Object distance = ‘u’ is always negative.
• Focal length of concave mirror = Negative
• Focal length of convex mirror = Positive
Mirror Formula
1/v +
1/u = 1/f
where,
v = Image distance
u
= Object distance
f
= Focal length
MAGNIFICATION OF SPHERICAL MIRRORS
It
is the ratio of the height of image to the height of object.
m
= Height of image/Height of object
m = hi/ho
Also,
m = -v/u
If ‘m’ is negative, image is real.
If ‘m’ is positive, image is virtual.
If hi = ho then
m = 1, i.e., image is equal to object.
If hi > ho then
m > 1 i.e., image is enlarged.
If hi < ho then
m < 1 i.e., image is diminished.
•
Magnification of plane mirror is always + 1.
‘+’
sign indicates virtual image.
‘1’
indicates that image is equal to object’s size.
•
If ‘m’ is ‘+ve’ and less than 1, it is a convex mirror.
•
If ‘m’ is ‘+ve’ and more than 1, it is a concave mirror.
•
If ‘m’ is ‘-ve’, it is a concave mirror.
MIRROR FORMULA AND MAGNIFICATION
1/v + 1/u = 1/f
Where ‘u’ is object
distance, ‘v’ is the image distance and ‘f’ is the focal length of the
spherical mirror, which is found by the similarity of triangles.
a.
The magnification produced by a spherical mirror is the ratio of the height of
the image to the height of the object. It is usually represented as ‘m’.
SIGN CONVENTION FOR RAY DIAGRAM
Distances
measured towards positive x and y axes (coordinate system) are positive, and
towards negative, x and y-axes are negative. Keep in mind the origin is the
pole (P). Usually, the height of the object is taken as positive as it is above
the principal axis, and the height of the image is taken as negative as it is
below the principal axis.
POSITION AND SIZE OF IMAGE FORMED
The size of the image
can be found using the magnification formula m = h’/h = – (v/u). If m is -ve it
is a real image and if it is +ve it is a virtual image.
REFRACTION THROUGH A GLASS SLAB AND REFRACTIVE
INDEX
REFRACTION
The shortest path need
not be the quickest path. Since light is always in a hurry, it bends when it
enters a different medium as it is still following the quickest path. This
phenomenon of light bending in a different medium is called refraction.
LAWS OF REFRACTION
a.
The incident ray, the refracted ray and the normal to the interface of two
transparent media at the point of incidence all lie in the same plane.
b.
The ratio of the sine of the angle of incidence to the sine of the angle of
refraction is a constant for the light of a given colour and for the given pair
of media. This law is also known as Snell’s law of refraction.
Absolute and Relative Refractive Index
The refractive index
of one medium with respect to another medium is called the relative refractive
index. When taken with respect to a vacuum, it’s known as an absolute refractive
index.
REFRACTION THROUGH A RECTANGULAR GLASS SLAB
When the light is
incident on a rectangular glass slab, it emerges out parallel to the incident
ray and is laterally displaced. It moves from rarer to a denser medium and then
again to a rarer medium.
REFRACTION AT A PLANAR SURFACE
Following Snell’s Law:
a.
Light bends towards the normal when moving from rarer to denser medium at the
surface of the two media.
b.
Light bends away from the normal when moving from denser to rarer medium at the
surface of contact of the two media.
REFRACTIVE INDEX
The extent to which
light bends when moving from one medium to another is called the refractive
index. This depends on the ratio of the speeds in the two media. The greater
the ratio, the more the bending. It is also the ratio of the sine of the angle
of incidence and the sine of the angle of refraction, which is a constant for
any given pair of media. It is denoted by:
n = sin∠i/sin∠r = speed of light in medium 1/speed of light
in medium2
The ratio of the speed
of light in a vacuum to the speed of monochromatic light in the substance of
interest is known as the relative refractive index. Mathematically, it is
represented as:
n = c/v
Where n is the
refractive index of a medium, c is the velocity of light in a vacuum and v is
the velocity of light in that particular medium.
TOTAL INTERNAL REFLECTION
a.
When the light goes from a denser to a rarer medium, it bends away from the
normal. The angle at which the incident ray causes the refracted ray to go
along the surface of the two media parallelly is called the critical angle.
b.
When the incident angle is greater than the critical angle, it reflects inside
the denser medium instead of refracting. This phenomenon is known as Total
Internal Reflection.
E.g. mirages, and optical fibres.
SPHERICAL LENS
REFRACTION AT CURVED SURFACES
When light is incident
on a curved surface and passes through, the laws of refraction still hold true,
for example, lenses.
SPHERICAL LENSES
Spherical lenses are
lenses formed by binding two spherical transparent surfaces together. Spherical
lenses formed by binding two spherical surfaces bulging outward are known as
convex lenses while spherical lenses formed by binding two spherical surfaces
such that they are curved inward are known as concave lenses.
IMPORTANT TERMS RELATED TO SPHERICAL LENSES
a.
Pole (P): The
midpoint or the symmetric centre of a spherical lens is known as its Optical
Centre. It is also called the pole.
b.
Principal Axis:
The line passing through the optical centre and the centre of curvature.
c.
Paraxial Ray:
A ray close to the principal axis and also parallel to it.
d.
Centre of curvature (C): The centres of the spheres that the spherical lens
was a part of. A spherical lens has two centres of curvature.
e.
Focus (F):
It is the point on the axis of a lens to which parallel rays of light converge
or from which they appear to diverge after refraction.
f.
Focal length:
Distance between optical centre and focus.
g.
Concave lens: Diverging
lens
h.
Convex lens: Converging
lens
RULES OF RAY DIAGRAM FOR REPRESENTATION OF IMAGES
FORMED
a.
A ray of light parallel to the principal axis passes/appears to pass through
the focus.
b.
A ray passing through the optical centre undergoes zero deviation.
IMAGE FORMATION BY SPHERICAL LENSES
The following table
shows image formation by a convex lens.
S. No. |
POSITION OF THE OBJECT |
POSITION OF THE IMAGE |
RELATIVE SIZE OF THE IMAGE |
NATURE OF THE IMAGE |
1 |
At
Infinity |
At Focus f |
Highly diminished point sized |
Real and inverted |
2 |
Beyond 2f |
Between f and 2f |
Duminished |
Real and inverted |
3 |
At 2f |
At 2f |
Same Size |
Real and inverted |
4 |
Between f and 2f |
Beyond 2f |
Enlarged |
Real and inverted |
5 |
At focus f |
At infinity |
Infinitely large or highly enlarged |
Real and inverted |
6 |
Between focus f and optical centre O |
On the same side of the lens as the object |
Enlarged |
Virtual and erect |
LENS FORMULA, MAGNIFICATION AND POWER OF LENS
LENS FORMULA AND MAGNIFICATION
Lens formula: 1/v =
1/u = 1/f, gives the relationship between the object distance (u), image
distance (v), and the focal length (f) of a spherical lens.
USES OF SPHERICAL LENS
Applications such as
visual aids: spectacles, binoculars, magnifying lenses, and telescopes.
POWER OF A LENS
The power of a lens is
the reciprocal of its focal length i.e. 1/f (in metre). The SI unit of power of
a lens is dioptre (D).
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