Ray Optics

10 - RAY OPTICS AND OPTICAL INSTRUMENTS Page 1

10.1 Laws of reflection ( applicable to both the plane as well as the curved surfaces ) ( 1 ) The angle of incidence is equal to the angle of reflection. ( 2 ) Inc ident ray, reflected ray and the normal drawn at the point of incidence are in the

same plane. 10.2 Reflection of Light by Spherical Mirrors Concave mir ror is formed by making the inner surface of the circular cross-section of a spherical shell reflecting while the convex mirror is formed by making the outer surface reflecting. Some definitions with reference to the mirror ( Refer to the figures as under. ) ( 1 ) Pole ( P ) - centre of the reflecting surface ( 2 ) Principal Axis - the imaginary line passing through the pole and centre of curvature of the mirror ( 3 ) Aperture ( QQ’ ) - diameter of the reflecting surface ( 4 ) Principal Focus - the point where the rays parallel to the principal axis meet ( concave mirror ), or appear to meet ( convex mirror ), after reflection ( 5 ) Focal Plane - plane passing through the principal focus and normal to the principal axis ( 6 ) Focal Length - the distance between the pole and the principal focus ( 7 ) Paraxial Rays - rays close to the principal axis

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10.3 Relation Between Focal Length and Radius of Curvature As shown in the figure, a paraxial ray is incident at point Q on a concave mirror. θ θ θ θ = angle of incidence = angle of reflection = ∠∠∠∠ CQF = ∠∠∠∠ QCF ( by geometry ) So, for ∆∆∆∆ CFQ, exterior ∠∠∠∠ QFP = ∠∠∠∠ CQF + ∠∠∠∠ QCF = 2θθθθ . For paraxial inc ident ray and small aperture, CP’ ≈≈≈≈ CP = R and FP’ ≈≈≈≈ FP = f. For small ape rture, 2θθθθ is very small.

∴∴∴∴ from the f igure, 2 θ θ θ θ ≈ FPQP

= f

QP … ( 1 ) and θθθθ =

CPQP

= R

QP … ( 2 )

From equation s ( 1 ) and ( 2 ), R = 2f ⇒⇒⇒⇒ f = R / / / / 2 Thus, focal length of a concave mirror is half its radius of curvature. Sign Convention Sign convention for the object distance ( u ), image distance ( v ), focal length ( f ) and radius of curvature ( R ) in the formulae to be derived are as under. ( 1 ) All distances are measured on the principal axis from the pole of the mirror. ( 2 ) Distance in the direction of incident ray is positive and opposite to it negative. ( 3 ) Height above the principal axis is positive and below it is negative. Mirror Formula As shown in the figure, a ray from object O, at a distance u, is incident at point Q on the concave mirror of small aperture making an angle αααα with the principal axis. It gets reflected in the direction Q ΙΙΙΙ making the same angle θθθθ with the normal CQ as the in cid ent ray. Another ray from O, moving along the axis, is incident at point P and gets reflected in the direction PC. Both these rays meet at Ι Ι Ι Ι on the principal axis forming image of the object at a distance v from the pole. According to the laws of reflection, angle of incidence, ∠∠∠∠ OQC = angle of reflection, ∠∠∠∠ CQΙΙΙΙ = θθθθ

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CQ and ΙΙΙΙQ make angles β β β β and γ γ γ γ respe ctively with the principal axis. In ∆∆∆∆ OCQ, exterior angle β β β β = α α α α + θθθθ In ∆∆∆∆ CQΙΙΙΙ, exterior angle γγγγ = β β β β + θθθθ Eliminating θθθθ, α α α α + γ γ γ γ = 2ββββ

Now, α α α α ( rad ) ≈ OP

QP arc, β β β β =

P CQP arc

and γ γ γ γ ≈ P QP arc

ΙΙΙΙ

Putting these values in the above equation,

OPQP arc

+ P QP arc

ΙΙΙΙ = 2

P CQP arc

∴∴∴∴ OP1

+ P 1

ΙΙΙΙ =

P C2

But as all dist ances are in direction opposite to the incident ray, OP = - u, C P = - R and Ι Ι Ι Ι P = - v,

∴∴∴∴ u 1

- +

---- v1

= R2----

∴∴∴∴ u1

+ v1

= R2

This is called Ga uss’ equation for a curved mirror. It is also valid for a convex mirror. Magnification due to a Mirror AB is the object at a distance u on the axis of a concave mirror as shown in the figure. A ray AQ, parallel to the principal axis and ray AP, incident on the pole, meet at point A’ after reflection and form the image of A. A’B’ normal to the axis is the image of AB. The ratio of the height of the image to the height of the object is called the transverse magnification or lateral magnification.

∴∴∴∴ lateral magnification, m = object the ofheight image the of height

= h'h

∆∆∆∆s ABP and A’B’P are similar. ∴∴∴∴ AB

'B'A =

BPP'B

Hence, using p roper sign convention, h

'h ---- =

uv ----

---- =

uv

∴∴∴∴ Lateral magnification = h

'h ---- =

uv

The same equ ation is obtained for a convex mirror.

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10.4 Refraction of Light When a ray of light goes from one transparent medium to another, its direction changes at the boundary surface ( unless it is incident normally to the surface ). This phenomenon is called refraction. Laws of Refraction ( 1 ) The incident ray, refracted ray and the normal drawn to the point of incidence are in

the same plane. ( 2 ) “For the two given media if θθθθ1 is the angle of incidence and θθθθ2 is th e angle of

refraction , then the ratio 2

1 sin

sin

θθθθθθθθ

is a constant.” ( Snell’s law )

This ratio, n 21, is called the refractive index of medium ( 2 ) with respect to medium ( 1 ).

∴∴∴∴ n21 = 2

1sin

sin

θθθθθθθθ

=

2

1vv

where v 1 and v 2 are the velocities of light in medium ( 1 ) and ( 2 ) respectively.

n21 depend s upon ( i ) the type of the media, ( ii ) their temperatures and ( iii ) the wavelength of light. The refractive index, n, of a medium with respect to vacuum ( or in practice air ) is called its absolute refractive index.

∴∴∴∴ n = vc

, where c is the velocity of light

in vacuum and v its velocity in the medium. In the figure, ray PQ is incident at an angle θθθθ1 to the no rmal drawn at point Q on the surface separating medium ( 1 ) and medium ( 2 ). QR is the refracted ray making an angle θθθθ2 with the normal. Abso lut e refractive index of medium ( 1 ) and medium ( 2 ) are respectively,

n1 = 1v

c and n 2 =

2vc

,

∴∴∴∴ 1

2nn

= 2

1vv

= n21 = 2

1 sin

sin

θθθθθθθθ

⇒⇒⇒⇒ n1 sin θθθθ1 = n2 sin θθθθ2 The ratio of the absolute refractive index of medium ( 2 ) to the absolute refractive index of medium ( 1 ) is the relative refractive index of medium ( 2 ) with respect to medium ( 1 ).

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For the media shown in the figure, n 2 > n1 ⇒⇒⇒⇒ sin θθθθ1 > sin θθθθ2 ⇒⇒⇒⇒ θθθθ1 > θθθθ2. Thus , when a ray of light goes from a rarer medium to a denser medium, the angle of refraction is smaller than the angle of incidence and the ray bends towards the normal and when it goes from a denser medium to a rarer medium, it bends away from the normal.

As above, n 21 = 2

1vv

. ∴∴∴∴ n12 = 1

2vv

⇒⇒⇒⇒ n21 ×××× n12 = 1

This re su lt can be generalized for any number of mediums. Lateral shift As shown in the figure, if a ray of light travelin g in a rarer, homogeneous medium, remains in the same medium, it will move along the path PQR’S’. But if it enters into a rectangular slab of denser medium, it will get refracted twice at surfaces, AB and CD. As the media on both sides of the rectangular slab is the same, n21 = 1 / / / / n12 and θθθθ1 = θ θ θ θ1’ Thus t he emer gent ray RS is parallel to the incident ray but due to refraction it shifts by an amount RN = x. Such a deviation of the incident ray is called lateral shift. From the figure, Lateral shift, x = QR sin ( θθθθ1 - θθθθ2 ) = QT sec θθθθ2 sin ( θθθθ1 - θθθθ2 ) = t sec θθθθ2 sin ( θθθθ1 - θθθθ2 ) If θθθθ1 is ve ry small, θθθθ2 is also sm all ⇒⇒⇒⇒ sin ( θθθθ1 - θθθθ2 ) ≈≈≈≈ ( θθθθ1 - θθθθ2 ) radian and sec θθθθ2 ≈≈≈≈ 1

∴∴∴∴ x = t ( θθθθ1 - θθθθ2 ) = t θθθθ1

θθθθθθθθ2222

1 - 1

Now according to Snell’s law,

1θθθθθθθθ2222 ≈

1 sin

sin

θθθθθθθθ2222 =

2

1nn

∴∴∴∴ x = t θθθθ1

2

1n

n 1 -

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Another example of refraction: An object inside water when viewed from outside appears raised due to the phenomenon of refraction. As shown in the figure, suppose an object is at real depth h o in a denser medium ( like water of refractive index, n2 ). Ray OQ from O refracts at Q and reaches e ye of the observer along QE. EQ extended in denser medium meets the normal PN at ΙΙΙΙ. So the observer sees the image at ΙΙΙΙ at an apparent depth, h i. If the ang le of incidence, θθθθ1 is very small , θθθθ2 will also be small.

∴∴∴∴ sin θ θ θ θ ≈ θ θ θ θ ≈ tan θθθθ By Snell's law, n 1 sin θθθθ1 = n2 sin θθθθ2 ⇒⇒⇒⇒ n1 tan θθθθ1 = n2 tan θθθθ2

∴∴∴∴ n1 (ΙΙΙΙP

PQ ) = n2 (ΟΟΟΟP

PQ ) ⇒ o

ih height, real

h ,height apparent =

2

1n

n =

) denser ( n) rarer ( n

Now suppose t hat the observer is a fish inside the water and it views the eye of the person along OQ ( as shown in the figure ). Ray OQ extended in air meets the normal drawn from point E to the surface at E’. Thus the fish sees the person’s eye at E’ instead of E. Here, EP = real height and E’P = apparent height. This example shows that if an object in a rarer medium is viewed from denser medium, it appears to be raised. Thus, if an object is kept in a rarer medium, at height h o from the interface and is viewed normally f rom the denser medium, then it appears to be at a height h i ( h i > ho ) and in this case

o

ih height, real

h ,height apparent =

1

2n

n =

) rearer ( n) denser ( n

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One more interesting case: As we go higher in the Earth’s atmosphere, it becomes optically rarer. Thus light coming from the sun and stars reaches the observer on Earth passing through the medium of continuously increasing refractive index and hence its direction continuously changes.

As shown in the figure, light rays from actual position, S 1, of the sun below the horizon reach the observer after continuous refraction in the Earth’s atmosphere. The tangent to the curved path of the ray at point P passes through the apparent position, S 2, of the sun above the hor izon. Taking the refractive index of air as 1.00029, the apparent shift in the position of the sun is approximately half a degree which corresponds to a time interval of 2 minutes. Thus sunrise is seen 2 minutes earlier and sunset is seen 2 minutes later than the actual event. 10.5 Total Internal Reflection Higher the refractive index of the medium, more is its optical density which is independent of the material density ( mass / / / / volume ) of the medium. When light is refracted, it is partially reflected also. For a given intensity, ΙΙΙΙ0, of the incident light, the in tensity of the reflected light, ΙΙΙΙ r, depends upon the angle of incidence. For normal incidence on a surface separating two media of refractive indices, n 1 and n 2, the intensity of reflected light is

ΙΙΙΙ r = 2) 1n2

2) 1n2

-

n (

n (

++++ΙΙΙΙ 0000

For a ir ( n = 1.0 ) and glass ( n = 1.5 ), nearly 4 %%%% of the incident energy is reflected. Refer to the figure on the next page. A is a point object ( or a light source ) in a denser medium. Rays AB, AB 1, AB2, … undergo partial refraction and partial reflection at points of incidence B , B1, B2, etc. on the surface separating the two media. As the angle of incidence keeps on incr easing, the angle of refraction also increases and for the incident ray AB 3, the

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refracted ray is along the surface separating two media, i.e., the angle of refraction is 90 °°°°. “The angle of incidence for which the angle of refraction is 90 °°°° is called the critical angle, C, of the denser medium with respect to the rarer medium.” Using Snell’s law, n1 sin θθθθ1 = n2 sin θθθθ2

For critic al angle of incidence, θθθθ1 = C and θθθθ2 = 90°°°°

∴∴∴∴ n1 sin C = n 2

∴∴∴∴ sin C = 1

2nn

= n1

( taking th e refractive index, n 2, of rarer medium air as 1 and of the denser medium, n 1, as n ) At the critica l angle of incidence, the reflected ray is called the critical ray. If the angle of incidence is more than the critical angle, there is no refraction and the incident ray gets completely reflected and its intensity also increases. This is known as total internal reflection and it obeys the laws of reflection. Uses of Total Internal Reflection: ( 1 ) The refractive index of diamond is 2.42 and its critical angle is 24.41 °°°°. Hence w ith

proper cutting of its faces, light entering into it undergoes many reflections and the diamond sparkles.

( 2 ) Using isosceles right angled prisms and taking advantage of total internal reflection,

light can be deviated by 90 °°°° and 180 °°°° as shown in the figures.

As can be seen from the figures that in both cases, the critical angle of the prism w.r.t. to air must be less than 45 °°°°.

Prisms of crown

glass ( C = 41.14 °°°° ) and flint glass

( C = 37.31°°°° ) are used for this.

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In the adjoining figure, the direction of light rays does not change but the image is inverted. This prism is called ‘amici prism’. In all the above cases, the size of the image remains the same as the size of the object. ( 3 ) Mirage formation in hot regions during summer due to total internal reflection: In summer, due to intense heat, the air in contact with the ground becomes hot and optically rarer as compared to the air above which is cold and optically denser.

As shown in the figure, a ray of light going from the top of the tree ( D ) to the ground travel continuously from a denser medium to a rarer medium. Its angle of incidence to the successive layers continuously increases due to refraction and when it exceeds the critical angle, the ray undergoes total internal reflection and reaches the eye of the observer. This ray appears to the observer as coming from a point D’ directly below D as if it is coming from water. This kind of image formation is called a mirage ( often seen in the deserts ). ( 4 ) Optical Fibres: Optical fibres are long thin fibres made of glass or fused quartz of 10 to 100 µµµµm diameter. The outer cladding of the fibres has a lower refractive index than the core of the fibre. The core ( refractive index = n 2 ) and the cladding ( refractive index = n 1 ) are so chosen that the critical angle o f incidence is small.

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As shown in the figure , a ray of light entering the optical fibre, entering at an angle of incidence greater than the critical angle, comes out of it after undergoing multiple total internal reflections. Even if the fibre is bent light remains within it. This is how endoscopy is done for viewing the human lungs, stomach, intestines, etc. In communications, optical fibres are used to make distortionless signal transmission. In absence of the cladding layer, due to dust particles, oil or other impurities, some leakage of light occurs. Fused quartz is used for making optical fibres because it is highly transparent. As shown in the figure, a ray incident at an angle θ θ θ θ i to the axis of th e fibre is refracted at an angle θ θ θ θ f. This ra y is incident on the wall of the fibre at an angle 90 °°°° - θ θ θ θ f, which if gr eater than the critical angle for fibre-air ( or cladding ) interface, will undergo total internal reflection. Thus, 90 °°°° - θ θ θ θ f > C ⇒⇒⇒⇒ sin ( 90°°°° - θ θ θ θ f ) > sin C ( = 1 / / / / n ), wher e n = refractive index of the material of the fibre.

∴∴∴∴ n cos θ θ θ θ f > 1 … … ( 1 ) Accord ing to Snell’s law, sin θθθθ i = n sin θ θ θ θ f

∴∴∴∴ n cos θ θ θ θ f = 2sinn n f22

θ - = i22θ - sin n > 1

Now the ma ximu m value of sin θθθθ i = 1. Hence if the above condition is satisfied for θθθθ I = 90°°°°, it would be satisfied for any value of θθθθ i.

∴∴∴∴ 1 n -2 > 1 ⇒⇒⇒⇒ n > 2

Thus, if the valu e of refractive index is greater than 2 , then the rays incident at any angle will undergo tot al internal reflection.

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10.6 Refraction at a Spherically Curved Surface As shown in the figure, a point object P is kept at a distance u from the centre, O, of the refracting curved surface on its axis OC. C is the centre of curvature of the refracting surface and R its radius. According to the sign convention, u is negative and R is positive. ( 1 ) The ray PO is incident at O normal to the curved surface and hence travels undeviated

along the axis OC of the curved surface. ( 2 ) Another ray PA is incident at the point A on the curved surface at an angle θθθθ1 to the

normal A C. Suppose the refractive index, n 1, of medium 1 is less than the refractive index, n 2, of medium 2. As a result, the refracted ray bends towards the normal and moves along A P’. θθθθ2 is the angle of refraction.

Both thes e rays meet at P’ forming the image of P. Applying Snell’s law and noting that the angles θθθθ1 and θθθθ2 are small, n1 sin θθθθ1 = n2 sin θθθθ2 ⇒⇒⇒⇒ n1 θθθθ1 = n2 θθθθ2 … … … ( 1 )

θθθθ1 is the e xterior angle in ∆∆∆∆ PAC, ∴∴∴∴ θθθθ1 = α α α α + + + + ββββ ββββ is the exterior angle in ∆∆∆∆ P’AC, ∴∴∴∴ θθθθ2 = β β β β - γγγγ Putting t hese values of θθθθ1 and θθθθ2 in equa tion ( 1 ) above,

n1 ( α α α α ++++ β β β β ) = n2 ( β β β β - γ γ γ γ ) ∴∴∴∴ n1 α α α α + + + + n2 γ γ γ γ = (n2 - n1 ) ββββ … … … ( 2 )

As angle s αααα, β β β β and γ γ γ γ are small, using proper sign convention and neglecting ∆∆∆∆ which is small as co mpared to u, v and R,

α α α α ≈ tan α α α α = u

h ----

, β β β β ≈ tan β β β β = Rh

and γ γ γ γ ≈ tan γ γ γ γ = vh

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Putting these values in equation ( 2 ),

n1

uh ----

+ n2

vh

= ( n2 - n1 ) Rh

⇒⇒⇒⇒ R

n n

vn

u

n 1221 ---- ---- ====++++

This equ atio n is valid for a concave surface also. While using this equation, proper sign convention has to be used. If the image distance v is positive, then the refracted rays are to the right of origin O where they actually meet and the image has to be real. If the image distance v is negative, then the refracted rays are to the left of origin O where they can meet only by extending backwards and hence the image has to be virtual. 10.7 Thin Lenses In general, a transparent medium bounded by two refracting surfaces is called a lens. The radii of curvature of the two refracting surfaces need not be equal. The lens for which the distance between the two refracting surfaces is negligible as compared to u, v and R is called a thin lens. For a thin lens, the distances can be measured from either surface. Consider a convex lens as shown in the figure. Radius of curvature of surface ( 1 ) = R 1 Radius of curv ature of surface ( 2 ) = R 2 Refractive ind ices of : medium to the left of the lens = n 1 material of the lens = n 2 medium to the right of the lens = n 3 ( Contact lens is an example of different media on both sides of the lens. On one side is air

and on the other side is the medium of the eye. )

For surface ( 1 ), - u

n1 + 1

2vn

= 1

12R

n n - … … … ( 1 )

For surface ( 1 ), R 1 is positive as it is to the right. For surface ( 2 ), v1 is the object distance and is positive as it is to the right of the surface. For refrac tion by the second surface, the rays go from medium of refractive index n 2 to the medium of refr active index n 3.

∴∴∴∴ - 1

2vn

+ v

n3 = 2

3R

2n n - … … … ( 2 )

Adding equations ( 1 ) and ( 2 ),

- u

n1 + v

n3 = 1

12R

n n - +

2

3R

2n n -

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This is a general equation for a thin lens and is valid for concave lens also. If both sides of the lens has the same medium, then n 1 = n3.

∴∴∴∴ - u

n1 + vn1 =

1

12R

n n - +

2

1R

2n n -

∴∴∴∴ n1

u1

v1 - = ( n2 - n1 )

2R1

R1 -1

∴∴∴∴ u1

v1 - =

211

1 2R1

R1

n

) nn ( ----

----

Focal Point of a Thin Lens A group of paraxial rays, incident on a convex lens, converge at a point F 2 after refraction on the ot her side of the lens. This point is called the principal focus of the lens and its distance from the optical centre, P, is the focal length, f, of the lens. For a concave lens, the incident paraxial rays are refracted away from the axis and when extended backwards meet at the principal focus, F 2, of the concave lens.

f is positiv e for a convex lens and negative for a concave lens. R 1 and R2 have opposite signs for co nvex and concave lenses. Putting u = ∞∞∞∞ and v = f in the formula

u1

v1 - =

211

1 2R1

R1

n

) nn ( ----

----, we get

f1

=

211

1 2R1

R1

n

) nn ( ----

----

This is called lens-maker’s formula as for a given material and given focal length, it gives the radii of curvature of the surfaces. Combining the above equations,

u1

v1 - =

f1

This is called th e Gaussian equation for a thin lens valid for both types of lenses.

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Magnification of the image formed by a lens As shown in the figure, AB is the object placed normal to the axis of the convex lens. Paraxial ray AQ after refraction passes through the principal focus F 2 on the other side. Ray AP passes thr ough the optical centre of the lens and moves ahead as ray PA’. Rays QF2A’ and PA’ meet each other at point A’ forming image of A. B’ is the foot of normal from A’ to the axis. Ray BP travels along the axis and after passing through the lens moves along path PB’. By symmetry, B’ is the image of B and A’B’ is the image of AB.

Now, magnification, m = object ofheight image ofheight

= h'h =

uv

positive m ⇒⇒⇒⇒ erect and virtual image and negative m ⇒⇒⇒⇒ inverted and real image. This formula can be used for a concave lens also. Power of a Lens: Converging capacity of a convex lens and diverging capacity of a concave lens is defined by the power of a lens. Power of a lens is the reciprocal of its focal length.

∴∴∴∴ Power of a lens, P = f1

Power of a lens is so defined because a convex lens of a short focal length focuses the rays within a very short distance and hence its converging capacity or power is more. In the same way, lens of longer focal length has less power. Hence, the power of a lens is defined as the reciprocal of its focal length. Power of a convex lens is positive as its focal length is positive and that of the concave lens is negative as its focal length is negative.

S Ι Ι Ι Ι unit of power of a lens is dioptre. Its symbol is D. 1 D = 1 m - 1 10.8 Combination of Thin Lenses in Contact As shown in the figure ( next page ), two convex lenses L 1 and L 2 with focal lengths f 1 and f2 are kept in contact in such a way that their principal axes coincide. A point like object O is kept away from the principal focus of lens L 1 and its image due to this lens alone would have been at ΙΙΙΙ’. This image behaves like a virtual object for lens L 2 and its image, fo rmed by lens L 2, is obtained at Ι.Ι.Ι.Ι.

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As the lenses are thin, their contact point can be taken as the optical centre of the combination. Distances u, v and v’ are shown in the figure.

For lens L 1, u1

'v

1 - = f1

1

For lens L 2, v'1

v1 - =

f

1

2

Adding these two results, u1

v1 - =

2f1

f1 1

++++ … … … ( 1 )

If the focal len gth of the lens equivalent to the given combination of lenses is f, then

u1

v1 - =

f1

… … … ( 2 )

From equation s ( 1 ) and ( 2 ), f1

= 2f1

f1 1

++++ and, in gener al,

f1

= 2f1

f1 1

++++ + nf1

f1 ................ 3

++++++++

Here f is sma ller than the smallest of f 1, f2, f3, ……….. fn. Power:

Replacing f1

= P, f1

1= P1, ……………

f1

n= Pn respectively in the above equation, we get

P = P1 + P2 + P3 + ………….. + Pn This sum is algebraic. P for some lenses ( convex ) will be positive and for some lenses ( concave ) will b e negative.

From the figure above, magnification for lens L 1, m1 = u'v

magn ification for lens L 2, m2 = v'v

and magnific ation for the lens-combination, m = uv

∴∴∴∴ m = uv

= v'v ××××

u'v

= m2 m1

For a combination of more than two lenses, m = m1 ×××× m2 ×××× m3 ×××× ………….. ×××× mn

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Position and Nature of Image formed by Mirrors / / / / Lenses Type of Mirror / / / / Lens

Position of Object

Position of Image

Nature of Image

1

At infinity

At focus

Real, inverted, Extremely diminished

2

Beyond the centre of curvature ( Mirror ) Beyond 2f ( Lens )

Between focus and centre of curvature ( Mirror ) Between f and 2f ( Lens )

Real, Inverted Diminished

3

At the centre of curvature ( Mirror ) At 2f ( Lens )

At the centre of curvature ( Mirror ) At 2f ( Lens )

Real, Inverted, Same Size

4

Between focus and centre of curvature ( Mirror ) Between f and 2f ( Lens )

Beyond the centre of curvature ( Mirror ) Beyond 2f ( Lens )

Real, Inverted, Magnified

5

At Focus

At infinity

Extremely Magnified

Concave Mirror OR Convex Lens

6

Between the pole and principal focus ( Mirror ) Within f ( Lens )

Behind the mirror, beyond the pole (Mirror) On the object side ( Lens )

Virtual, Erect, Magnified

1

At infinity

At focus

Virtual, Erect, Diminished

Convex Mirror OR Concave Lens

2

Between infinity and Mirror //// Lens

Between the focus and the pole ( Mirror ) Between the lens and f

”

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10.9 Refraction of Light Due to a Prism The cross- section perpendicular to the rectangular surfaces of a prism, made up of a transparent material, is shown in the figure. A ray of monochromatic light incident at point Q on the surface AB of the prism gets refracted and travels along QR undergoing deviation δδδδ1 at point Q. It is then incident at point R on the surface AC and emerges after refraction along RS undergoing deviation δδδδ2 at R. When th e emergent ray RS is extended backwards, it meets the extended incident ray PE in D. Angle, δδδδ, between the incident and the emergent rays is called the angle of deviation. As shown in the figure, in AQLR, ∠∠∠∠ AQL and ∠∠∠∠ ARL are right angles.

∴∴∴∴ ∠∠∠∠ A + ∠∠∠∠ QLR = 180°°°° … … … ( 1 )

and in ∆∆∆∆ QLR, r1 + r2 + ∠∠∠∠ QLR = 180°°°° … … … ( 2 )

∴∴∴∴ r1 + r2 + ∠∠∠∠ A = 180°°°° ( from eq uations ( 1 ) and ( 2 ) )

∴∴∴∴ r1 + r2 = A … … … ( 3 ) In ∆∆∆∆ DQR, exterior angle δ δ δ δ = δδδδ1 + δδδδ2 = i - r1 + e - r2

= i + e - ( r1 + r2 )

∴∴∴∴ δ δ δ δ = i + e - A … … … ( 4 ) ( from equation ( 3 ) ) Thus, the angle of deviation depends on the angle of incidence. The graph of angle of deviation vs. angle of incidence for an equilateral prism is shown in the figure. As can be seen from the graph, the angle of deviation is the same for two values of angle of incidence. This means that if the ray PQRS is reversed along path SRQP, i.e., if the angle of incidence is e, the angle of emergence will be i, but the angle of deviation will remain the same. As shown in the graph, for a particular value of the angle of deviation, δ δ δ δ = δ δ δ δ m which is minimum, t here is only one angle of incidence. Putting δ δ δ δ = δ δ δ δ m and i = e in equation ( 4 ), δ δ δ δ m = 2i - A

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Using Snell’s law for incident ray PQ at Q and SR at R, n1 sin i = n 2 sin r 1 and n 1 sin e = n 2 sin r 2 For minimum an gle of deviation, e = i .

∴∴∴∴ sin r 1 = sin r 2 ⇒⇒⇒⇒ r1 = r2 = r ( suppose )

∴∴∴∴ n1 sin i = n 2 sin r 1 = n2 sin r = n2 sin (2A ) ( Q r =

2A

from equation ( 3 ) )

∴∴∴∴ 1

2nn

= r sini sin

=

++++ δδδδ

2A

sin

2

m A sin

( Q δ δ δ δ m = 2i - A )

If the prism is k ept in air, n 1 = 1 and n 2 = n,

∴∴∴∴ n =

++++ δδδδ

2A

sin

2

m A sin

This equation shows that for a given prism, the value of δ δ δ δ m depends upon ( i ) the angle of th e pr ism, ( ii ) the refractive index of the material of prism and ( iii ) the refractive index of the medium in which the prism is kept. When δ δ δ δ is minimum, the ray QR passing through the prism is parallel to the base BC of the prism ( taking AB = AC ). Using the above equation, one can calculate the refractive index of the prism with respect to the medium by measuring A and δ δ δ δ m . For a pr ism with small A, δ δ δ δ m is also small.

Hence t aking

++++ δδδδ

2m A

sin ≈≈≈≈ 2

m A δδδδ++++ ( radian ) and

2A

sin ≈≈≈≈ 2A

( radian ),

n = (2

m A δδδδ++++ )/(2A ) =

Am A δδδδ++++

∴∴∴∴ δ δ δ δ m = A ( n - 1 )

10.10 Dispersion of light due to a prism The phenomenon in which light gets divided into its constituent colours is known as dispersion of lig ht. As shown in the figure ( next page ), when a beam of white light or sun rays pass through a prism, the emergent light is seen to be dispersed into various colours. Newton arranged two identical prisms of the same material as shown in the second figure and observed that when white light is incident on the first prism, emergent light from the second prism was also white. Hence it is clear that the first prism disperses the colours of white light and the second prism brings them together again to produce white light.

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Visible light is made up of electromagnetic waves of wavelengths

between 4000 oA and 8000

oA having

different colours. All these waves have equal velocity in vacuum. Hence vacuum is called non-dispersive medium. But their velocities in some other medium of refractive index, n, are different. Such a medium is called a dispersive medium. So, as per n = c ////v, the refractive indices of light having different wavelengths are different in a dispersive medium. For example, the velocity of violet light ( v v ) is less than the velocity of red light ( v r ). So the refrac tive index of violet light ( n v ) is greater than the refractive index for red light ( n r ). ( nv > n r ). For other colours, values of refractive indices lie between n r and n v . If the angles of minimum deviation for red and violet colours are δδδδR and δ δ δ δV

respectively , then δδδδR = A ( n r - 1 ) and δδδδV = A ( n v - 1 ) n v > n r ⇒⇒⇒⇒ δδδδV > δδδδR . Thus, viole t colour deviates more than red colour. For two given colours, the difference of their angles of deviation is known as the angular deviation corresponding to those colours. Value of n v - n r is more for flint glass than for common crown glass. So, the spectrum obtained from such a prism is wider, more dispersed and more detailed. 10.11 Rainbow Sunlight refracted and dispersed by the water droplets suspended in the atmosphere during monsoon form the rainbow pattern. Rainbow is a good example of dispersion and internal reflection of light. As shown in the figure, P and Q are two of the innumerable water droplets. Two rays R 1 and R2 from the sun behind the observer incident on water droplets P and Q get refracted and dispersed. All colours undergo internal reflection and emerge after second refraction.

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From the drop P, red colour light reaches the eye of the observer at an angle, θθθθ2 = 42.8°°°°, with the horizontal. Thus, from all such droplets on the arc of a circle making this angle with the horizontal, red colour light reaches the eye of the observer. Similarly, from the drop Q, violet colour light reaches the eye of the observer at an angle θθθθ1 = 40.8°°°°, with the horizontal and from all such droplets making this angle with the horizontal, violet colour light reaches the eye of the observer. All the remaining colours of light are seen between red and violet. Thus rainbow is seen in the form of a semicircle. This rainbow is known as primary rainbow. All the colours of a primary rainbow are accommodated within 2 °°°° near the eye. Sometimes, a faint secondary rainbow is seen above the primary rainbow in which order of the colours gets reversed. Here, the internal reflection of light occurs twice as compared to once in the primary rainbow. The red and violet colours of secondary rainbow coming from water droplets D 1 and D2 at an angle of θθθθ3 = 50.8°°°° and θθθθ4 = 54.5°°°° respec tively are shown in the figur e. All the colours of a secondary rainbow are accommodated within 3.7 °°°° near the eye. If the rainbow is observed from the height of a mountain or the top of a tower, some portion of rainbow below the horizon can also be seen. 10.12 Scattering of Light Light inciden t on atmospheric atoms and molecules and small suspended particles like cloud droplets is absorbed by them and immediately reradiated in different directions in different proportions of intensity. This process is called the scattering of light. If the size of the particle which scatters the light is smaller than wavelength of the incident light, the scattering is known as Rayleigh’s scattering. Rayleigh observed that the scattering of light is inversely proportional to the fourth power of the wavelength of light. As the wavelength of blue light is 1.7 times smaller than that of red light, it scatters 8 to 9 times more than the red light. Although violet and indigo light also have short wavelengths, their proportion in light is much less and our eyes are not sensitive to these colours. So their scattering is not so important. The light having wavelength close to the wavelength of yellow colour has maximum intensity and even our eyes are more sensitive to the light of these colours. The figure shows the light of the rising sun reaching the earth’s atmosphere. In this condition, white light has to travel more distance through the atmosphere during which light of most of the colours is scattered and only red colour reaches the observer on the earth. So the sun appears reddish and the sky above appears bluish due to scattered blue colour. Similar situation prevails at the time of sunset also. The same reason is responsible for a reddish full-moon, while rising or setting. If the size of particles due to which light is scattered are larger than the wavelength, the

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scattering is known as Mie-scattering. This type of scattering was first studied by Gustav Mie in 1908 A.D. In this type of scattering, the relation between the intensity and wavelength of the scattered light is complicated. However, as the size of the particle increases, the proportion of diffused reflection also increases. Size of the water particles forming white clouds being large, diffused reflection of sun-light takes place. As the diffused reflection is independent of the wavelength, all the wavelengths of visible light are reflected and so the clouds appear white. 10.13 Optical Instruments 10.13 ( a ) Simple Microscope: Apparent size of an object as seen by us depends on the actual size of the object and the angle subte nded by it with our eye. When we see the railway tracks standing between the tracks, at far distance rails seem to be meeting each other. This is because the rays coming from the points far away on the rails, one from each rail, subtend a very small angle with our eye. For this reason, to see a microscopic object clearly, we tend to keep it very near our eyes. But this strains the eyes and we can’t see the object clearly. In fact, to see any object clearly without straining the eyes we have to keep it at some minimum distance from the eyes. This minimum distance is called the near point or the distance of most distinct vision. Hence to see a microscopic object clearly, we place it within the focal length of a convex lens so that its virtual, magnified, erect image is formed at a comfortable distance of distinct vision and we can see it clearly. This convex lens is known as simple microscope. Suppose a linear object with height h o, kept at t he near point ( ≈≈≈≈ 25 cm ) from our eye, subtends an angle θ θ θ θ o with our eye as shown in the fig ure. Now, suppose the object is kept at such a distance within the focal length, f, of a convex lens that its virtual, erect and magnified image is formed at the near point as shown in the figure. Here, as the eye is very near the lens, the angle, θθθθ, subtended by the object and image with the lens is the same as the angle subtended with the eye. According to the definition: Angular magnification or Magnifying power of the lens ( M )

= eye the hpoint wit near the on object, the by subtended Angle

eye the hpoint wit near the on image, the by subtended Angle,

,0000θθθθ

θθθθ =

D hD h

o

i/ / / / / / / /

( Q θθθθ and θ θ θ θ o are very small )

= o

ihh

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Magnifying power is same as linear magnification.

∴∴∴∴ m = uv

= uD

( Q v = D, the distance of most distinct vision )

Now, f1

u1

v1 - ==== ∴∴∴∴

f1

u1

D1 - ====++++ ( Q v = D and u are negative )

∴∴∴∴ m = uv

= 1 + fD

If the imag e is at a very large distance ( theoretically at infinity ), magnification will be very large and 1 can be neglected as compared to D / / / / f.

Thus the value of m would be between fD

and 1 + fD

.

To obtain the enlarged, clear object which can be seen without straining the eyes, the object should be kept near f, but at a distance less than f.

10.13 ( b ) Compound Microscope: In a simple microscope, magnifying power depends on D / / / / f. So to obtain more magnification, we may be tempted to use a small focal length. But this distorts the image. Hence, f cannot be taken very small and a simple microscope gives a maximum magnification of 20 X. Now if we use this magnified image as an object for another convex lens, we can further magnify it. Thus a compound microscope is made using two convex lenses. Ray diagram for a compound microscope is shown in the figure on the next page. The lens kept near the object is called ‘objective’ and the lens kept near the eye is known as ‘eye-piece’. Distance between the second focal point ( P ) of the objective and the first focal point ( Q ) of the eye-piece is known as ‘tube-length ( L )’ of the microscope. As can be seen from the figure, the real, inverted and magnified image obtained by the objective near the focal-point ( Q ) of the eye-piece acts as an object for the eye-piece which behaving as a simple microscope gives a virtual and highly magnified final image at a very large distance.

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Magnification obtained by a compound microscope From the figure, magnification due to the objective,

mo = o

ihh

= ofL

( Q h i ≈ PQ tan β β β β = L tan ββββ; ho = fo tan β β β β ), where h i = size o f the first image, fo = focal length of objective Now, magnification due to the eye-piece,

me = efD

, where

fe = focal length of the eye-piece.

∴∴∴∴ magnification of the compound microscope, m = m o me

∴∴∴∴ m = eo fD

fL ××××

10.13 ( c ) Astronomical Telescope: Astronomical Telescope is used to observe very huge celestial bodies and stars which are far away from us and from each other. Its ray diagram is shown in the figure. Here two convex lenses are kept on the same principal axis. The lens facing the object is called objective whose diameter and focal length are greater than the lens known as eye-piece kept near the eye.

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When the telescope is focused on a distant object, parallel rays coming from this object form a real, inverted and small image A 1B1 on the second principal focus of the objective. This image is th e object for the eye-piece. Eye-piece is moved to or fro to get the final and magnified inverted image A 2B2 of the original object at a certain distance. Magnification of the telescope,

m = eye or objective the thobject wi the by subtended Angle

eye withimage final the by subtended Angle =

ααααββββ

= 1BA

of

ef1BA

1

1 ××××

∴∴∴∴ m = efof

Hence, to increase the magnification of the telescope, f o should be increased and f e should be decreased . fo + fe is the optical length of the telescope. So, length of the telescope, L ≥≥≥≥ fo + fe. If fo = 200 cm and f e = 1 cm; m = 200. Using such a telescope, if the stars having angular distance 1’ a re observed, they would be seen at 200’ = 3.33 °°°° angular distance between them. For a telescope light gathering power and resolving power ( power to view two nearby objects distinctly ) are very important. Amount of light entering the objective of the telescope is directly proportional to the square of the diameter of the objective. With increase in the diameter of the objective, resolving power also increases. In the telescope described above, rays from the object are refracted by the objective to form the image. Such a telescope is called a refractive telescope. Image formed in this type of telescope is inverted. To get rid of this problem, there is an extra pair of inverting lenses in the terrestrial telescope so that the erect image of the distant object is obtained. For better resolution and magnification, mirrors are used in modern telescopes. Such a telescope is known as a reflecting telescope. In such a telescope, problems of chromatic and spherical aberration are also overcome if a parabolic mirror is used. Construction of such a telescope is shown in the following figure. Parallel rays coming from a distant object are incident on the reflecting surface of the primary parabolic concave mirror. A convex mirror is kept in the path of the reflected rays which would have focused at F forming the image. Rays reflected by the secondary mirror are focused on the eye-piece after passing through the hole kept in the primary mirror. Diameter and focal length of the primary mirror are kept large in such a telescope.

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10.13 ( d ) Human Eye: As shown in the figure, the ray entering the eye is first refracted in the cornea and then in the eye lens which is the main refractor. This forms inverted, real image on the retina which is processed in the brain and a final erect image is seen. Retina has two types of cells: ( 1 ) Rods: These cells receive the sensations of less intense light. ( 2 ) Cones: These cells receive the sensations of colour and more intense light. In the eye, the distance between the retina and the lens is fixed. Hence to form the image of objects at different distances exactly on the retina, focal length of the lens has to be changed. This is done by ciliary muscles which make the lens thick or thin as required. The iris controls the amount of light entering the eye by controlling the size of the pupil ( front aperture ). When we see the object kept on the side, lens of the eye rotates and brings the image on the central region of the retina ( fovea ). Defects of Vision

If the thickness of the eye lens cannot be altered as needed, then the rays coming from distant objects which are parallel, undergo extra refraction and focus in front of the retina as shown in the first figure. So distant objects cannot be seen clearly. But the image of the nearby object is formed on the retina as shown in the second figure. This type of defect is called ‘near sightedness ( myopia )’ . To correct th is defect, concave lenses are used as shown in the third figure above.

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If the lens remains thin and does not become thick as needed, the rays from a nearby object undergo less refraction and focus behind the retina as shown in the first figure. Such an image cannot be seen clearly. Image of a distant object is formed on the retina and can be seen clearly, but nearby objects cannot be seen clearly. This type of defect is called ‘far sightedness ( hypermetropia )’.

This type of defect is due to less convergence of rays and can be corrected by using a convex lens of proper focal length as shown in the second figure above. Some persons can see only horizontal or vertical wires in a wire mesh clearly but not both. This defect is called ‘astigmatism’. This defect is due to unequal curvatures of the lens and corne a. Here horizontal curvatures are same but not the vertical. So rays are refracted equally in the horizontal plane but unequally in the vertical plane. As a result horizontal wires are seen clearly, but not the vertical wires. To remove this defect, cylindrical lenses are used. 10.13 ( e ) Photographic Camera: As shown in the figure, in a photographic camera, a combination of 3 convex lenses at one end and a photo sensitive surface at the other end are kept in a light proof box. When a photograph is taken, the shutter opens and shuts quickly. Light enters through the lens and is incident on the film during the time when the shutter remains open. Thus, due to the lens, a real and inverted image of the object is formed on the film. The amount of light entering the camera is controlled using the aperture of the lens. The distance between the lens and the film can be adjusted for better pictures.

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As the focal length of a lens in a camera is small ( app. 50 mm ), the changes required in the distance between the lens and the film are very small even for large object distance. For clear and good quality photographs, the following points are important. ( 1 ) Exposure Time: The time for which the light is incident on the film is known as the exposure time. Less exposure time is kept in sunlight or more light. For indoor photography amount of light is less, so more exposure time is kept. For fast moving objects, less exposure time is kept. For

a given aperture in a camera, usual exposure times are 500

1s,

2501

s, 125

1s,

601

s,

301

s,…

( 2 ) Apertur e of the Lens: Diameter of the circular passage of light kept in a camera is the aperture. Some useful

apertures known as f-number are ... ,16f

,11f

,8f

,5.6f

,4f

,2.8f

,2f

where f is the focal

length of the le ns. If the film is exposed equally for aperture diameter, d 1 = 4f

and d 2 = 8f

,

then for diameter d 1, the shutter should be kept open for 4 times longer compared to that for diameter d 2. Thus exposure time is inversely proportional to the area of the aperture. ( 3 ) Speed of t he film: How quickly the film can be exposed is known as its speed. Fast film needs less exposure time and is used when light is less whereas slow film needs more exposure time and is suitable for the still photography. ( 4 ) Exposure meter: Some cameras are furnished with exposure meters which consists of a photosensitive surface. Electric current is produced in accordance with the intensity of light incident on the photosensitive surface which automatically adjusts the aperture and exposure time. ( 5 ) Depth of Focus or Depth of Field: If an object at a distance u can be perfectly focused on a film, ∆∆∆∆u is the depth of focus which me ans that all objects within ∆∆∆∆u distance of the object can be satisfactorily focused. More the a per ture size, less is the depth of focus. 10.13 ( f ) Spectrometer: Spectrometer is used in the laboratory to get a clear spectrum and determine the refractive index of the ma terial of the prism. It consists of a collimator, telescope and prism table. There is the scales below the prism table and the base of the spectrometer and leveling screws at the base. In the collimator, light entering through the adjustable slit is made parallel and incident on the refracting surface of the prism kept in a specific position on the prism table. Telescope is arranged to receive the refracted light and its eye-piece is moved to focus and get a clear spectrum of

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the original light. We can know the angular position ( θθθθ ) of the spectral lines of various colours b y using a cross-wire and can be read from the scale. Prism table and telescope are arranged such that the angle of minimum deviation ( δδδδm ) is obtained for each colour. Thus refractive index for the material of prism for a particular wavelength can be determined using the formula

n =

++++ δδδδ

2A

sin

2

m A sin

To measure the angle of the prism, A, prism table and telescope are so arranged that the rays refra cted from one surface forming angle A enters the telescope and the same happens for the second surface. By knowing the angular position of the telescope in these two cases, angle of the prism can be calculated. The complete path of light is shown in the figure below.

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19 - RAY OPTICS Page 1 ( Answers at the end of all questions )

1 ) A fish looking up through the water sees the outside world contained in a circular

horizon. If the refractive index of water is 4 / 3 and the fish is 12 cm below the surface, the radius of this circle in cm is ( a ) 7 36 / ( b ) 7 36 ( c ) 54 ( d ) 5 36 / [ AIEEE 2005 ]

2 ) A thin glass ( refractive index 1.5 ) lens has optical power - 5 D in air. Its optical power

in a liquid medium with refractive index 1.6 will be ( a ) - 1 D ( b ) 1 D ( c ) - 25 D ( d ) 25 D [ AIEEE 2005 ] 3 ) A light ray is incident perpendicular to one face of a 90° prism and is totally internally reflected at the glass-air interface. If the angle of reflection is 45°, we conclude that the refractive index, n: ( a ) n < 1 / √2 ( b ) n > √2 ( c ) n > 1 / √2 ( d ) n < √2 [ AIEEE 2004 ] 4 ) A plano-convex lens of refractive index 1.5 and radius of curvature 30 cm is silvered

at the curved surface. Now this lens has been used to form the image of an object. At what distance from this lens, an object be placed in order to have a real image of the size of the object ?

( a ) 20 cm ( b ) 30 cm ( c ) 60 cm ( d ) 80 cm [ AIEEE 2004 ]

5 ) To get three images of a single object, one should have two plane mirrors at an angle of

( a ) 30° ( b ) 60° ( c ) 90° ( d ) 120° [ AIEEE 2003 ]

6 ) The image formed by an objective of a compound microscope is ( a ) real and enlarged ( b ) virtual and enlarged ( c ) real and diminished ( d ) virtual and diminished [ AIEEE 2003 ] 7 ) A candle placed 23 cm from a lens, forms an image on a screen placed 75 cm on the other end of the lens. The focal length and type of the lens should be ( a ) + 18.75 cm and convex lens ( b ) - 18.75 cm and concave lens ( c ) + 20.25 cm and convex lens ( d ) - 20.25 cm and concave lens [ AIEEE 2003 ] 8 ) A person having the nearest distance of distinct vision of 32 cm uses a reading lens of 8 cm focal length. The magnification of his reading lens is ( a ) 5 ( b ) 4 ( c ) 3 ( d ) 2 [ AIEEE 2002] 9 ) Consider telecommunication through optical fibres. Which of the following statements is not true ? ( a ) Optical fibres can be of graded refractive index. ( b ) Optical fibres have extremely low transmission loss. ( c ) Optical fibres are subject to electromagnetic interference from outside. ( d ) Optical fibres may have homogeneous core with a suitable cladding. [ AIEEE 2002 ] 10 ) A ray of light passing through a prism having µ = √2 suffers minimum deviation. If

angle of incidence is double the angle of refraction within prism, the angle of prism is ( a ) 30° ( b ) 45° ( c ) 60° ( d ) 90° [ AIEEE 2002 ]

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11 ) The combined power of two lenses in contact is + 10 D. When they are separated by 20 cm, their power becomes + 6.25 D. The powers of these lenses are ( a ) - 3.5 D, + 6.5 D ( b ) - 7.5 D, + 2.5 D ( c ) + 7.5 D, + 2.5 D ( d ) + 9.0 D, + 1.0 D [ AIEEE 2002 ] 12 ) A ray of light is incident on the face AB of a prism of refracting angle 60° as shown in the figure. The angle of incidence at which the ray of light just suffers total internal reflection on the face AC is ( µ = 1.5 ) ( a ) 19.6° ( b ) 23.6° ( c ) 27.6° ( d ) 35.6° [ AIEEE 2002 ] 13 ) A double convex lens of refractive index µ 2 is immersed in a liquid of refractive index

µ 1. This lens will act as converging lens, if ( a ) µ 1 > µ 2 ( b ) µ 2 > µ 1 ( c ) µ 1 = µ 2 ( d ) µ 1 = µ 2 = 0 [ AIEEE 2002 ] 14 ) A convex lens is in contact with concave lens. The magnitude of the ratio of their

focal lengths is 2 / 3. Their equivalent focal length is 30 cm. Their individual focal lengths are

( a ) - 75, 50 ( b ) - 10, 15 ( c ) 75, 50 ( d ) - 15, 10 [ IIT 2005 ] 15 ) A container is filled with water ( m = 1.33 ) upto a height of 33.25 cm. A concave mirror

is placed 15 cm above the water level and the image of an object placed at the bottom is formed 25 cm below the water level. The focal length of the mirror is

( a ) 10 cm ( b ) 15 cm ( c ) 20 cm ( d ) 25 cm [ IIT 2005 ] 16 ) White light is incident on the interface of glass and

air as shown in the figure. If green light is just totally internally reflected, then the emerging ray in air contains

( a ) yellow, orange, red ( b ) violet, indigo, blue ( c ) all colours ( d ) all colours except green [ IIT 2004 ] 17 ) A ray of light is incident on an equilateral glass

prism placed on a horizontal table. Which of the following is true for maximum deviation ?

( a ) PQ is horizontal ( b ) QR is horizontal ( c ) RS is horizontal ( d ) either PQ or RS is horizontal [ IIT 2004 ] 18 ) A point object is placed at the centre of a glass sphere of radius 6 cm and refractive

index 1.5. The distance of the virtual image from the surface of the sphere is ( a ) 2 cm ( b ) 4 cm ( c ) 6 cm ( d ) 12 cm [ IIT 2004 ]

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19 ) The size of the image of an object, which is at infinity, as formed by a convex lens of

focal length 30 cm is 2 cm. If a concave length of focal length 20 cm is placed between the convex lens and the image at a distance of 26 cm from the convex lens, the size of the new image will be

( a ) 1.25 cm ( b ) 2.5 cm ( c ) 1.05 cm ( d ) 2 cm [ IIT 2003 ] 20 ) A ray of light is incident at the glass-water interface at an angle i. If it emerges finally

parallel to the surface of water, then the value of µg would be ( a ) ( 4 / 3 ) sin i ( b ) 1 / sin i ( c ) 4 / 3 ( d ) 1 [ IIT 2003 ] 21 ) An observer can see through a pin-hole the top end of a thin

rod of height h, placed as shown in the figure. The beaker height is 3h and its radius is h. When the beaker is filled with a liquid upto a height 2h, he can see the lower end of the rod. Then the refractive index of the liquid is

( a ) 25 ( b )

25 ( c )

23 ( d )

23

[ IIT 2002 ] 22 ) Which one of the following spherical lenses does not exhibit dispersion ? The radii of

curvature of the surfaces of the lenses are given in the diagrams. [ IIT 2002 ]

23 ) Two plane mirrors A and B are aligned parallel to

each other as sown in the figure. A light ray is incident at an angle of 30° at a point just inside one end of A. The plane of incidence coincides with the plane of the figure. The maximum number of times the ray undergoes reflections ( including the first one ) before it emerges out is

( a ) 28 ( b ) 30 ( c ) 32 ( d ) 34 [ IIT 2002 ] 24 ) A ray of light passes through four transparent media with

refractive indices µ1, µ2, µ3 and µ4 as shown in the figure. The surfaces of all media are parallel. If the emergent ray CD is parallel to the incident ray AB, we must have

( a ) µ1 = µ2 ( b ) µ2 = µ3 ( c ) µ3 = µ4 ( d ) µ4 = µ1 [ IIT 2001 ]

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25 ) A given ray of light suffers minimum deviation in an

equilateral prism P. Additional prisms Q and R of identical shape and of the same material as P are now added as shown in the figure. The ray will suffer

( a ) greater deviation ( b ) same deviation as before ( c ) no deviation ( d ) total internal reflection [ IIT 2001 ] 26 ) A point source of light B, placed at a distance L in front of

the centre of a mirror of width d, hangs vertically on a wall. A man walks in front of the mirror along a line parallel to the mirror at a distance 2L from it as shown. The greatest distance over which he can see the image of the light source in the mirror is

( a ) d / 2 ( b ) d ( c ) 2d ( d ) 3d [ IIT 2000] 27 ) In a compound microscope, the intermediate image is ( a ) virtual, erect and magnified ( b ) real, erect and magnified ( c ) real, inverted and magnified ( d ) virtual, erect and reduced [ IIT 2000 ] 28 ) A diverging beam of light from a point source S

having divergence angle α is incident symmetrically on a glass slab as shown. The angles of incidence of the two extreme rays are equal. If the thickness of the glass slab is t and its refractive index is n, then the divergent angle of the emergent beam is

( a ) zero ( b ) α ( c ) sin -1(1/n) ( d ) 2 sin - 1 ( 1 / n ) [ IIT 2000 ] 29 ) A rectangular glass slab ABCD of refractive index

n1 is immersed in water of refractive index n2 ( n1 > n2 ). A ray of light is incident at the surface AB of the slab as shown. The maximum value of the angle of incidence αmax, such that the ray comes out only from the other surface CD, is given by

( a )

121

211

nn

sin cos nn

sin -- ( b )

2 1

11

n1 sin cos n sin - -

( c )

211

nn

sin - ( d )

121

nn

sin - [ IIT 2000 ]

30 ) A hollow double concave lens is made of very thin transparent material. It can be

filled with air or either of two liquids L1 or L2 having refractive indices n1 and n2 respectively ( n2 > n1 > 1 ). The lens will diverge a parallel beam of light if its is filled with

( a ) air and placed in air ( b ) air and immersed in L1 ( c ) L1 and immersed in L2 ( d ) L2 and immersed in L1 [ IIT 2000 ]

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31 ) A concave lens of glass, refractive index 1.5 has both surfaces of same radius of

curvature R. On immersion in a medium of refractive index 1.75, it will behave as a ( a ) convergent lens of focal length 3.5 R ( b ) convergent lens of focal length 3.0 R ( c ) divergent lens of focal length 3.5 R ( d ) divergent lens of focal length 3.0 R [ IIT 1999 ] 32 ) A real image of a distant object is formed by a planoconvex lens on its principal axis.

Spherical aberration ( a ) is absent ( b ) is smaller if the curved surface of the lens faces the object ( c ) is smaller if the plane surface of the lens faces the object ( d ) is the same whichever side of the lens faces the object [ IIT 1998 ] 33 ) A ray of light traveling in a transparent medium is incident on a surface separating the

medium from air at an angle of incidence 45°. The ray undergoes total internal reflection. If n is the refractive index f the medium with respect to air, select the possible value ( s ) of n from the following.

( a ) 1.3 ( b ) 1.4 ( c ) 1.5 ( d ) 1.6 [ IIT 1998 ] 34 ) A concave mirror is placed on a horizontal table with its axis directed vertically

upwards. Let O be the pole of the mirror and C its centre of curvature. A point object is placed at C. It has a real image, also located at C. If the mirror is now filled with water, the image will be

( a ) real and will remain at C ( b ) real and located at a point between C and ∞ ( c ) virtual and located at a point between C and O ( d ) real and located at a point between C and O [ IIT 1998 ] 35 ) A spherical surface of radius of curvature R, separates air ( refractive index 1.0 ) from

glass ( refractive index 1.5 ). The centre of curvature is in the glass. A point object P placed in air is found to have a real image Q in the glass. The line PQ cuts the surface at a point O and PO = OQ. The distance PO is equal to

( a ) 5R ( b ) 3R ( c ) 2R ( d ) 1.5R [ IIT 1998 ] 36 ) Which of the following form ( s ) a virtual and erect image for all positions of the

object ? ( a ) convex lens ( b ) concave lens ( c ) convex mirror ( d ) concave mirror [ IIT 1996 ] 37 ) Spherical aberration in a thin lens can be reduced by ( a ) using a monochromatic light ( b ) using a doublet combination ( c ) using a circular annular mask over the lens ( d ) increasing the size of the lens [ IIT 1994 ] 38 ) A planet is observed by an astronomical refracting telescope having an objective of

focal length 16 m and an eyepiece of focal length 2 cm. Which of the following statements are true ?

( a ) The distance between the objective and the eyepiece is 16.02 m. ( b ) The angular magnification of the planet is - 800. ( c ) The image of the planet is inverted. ( d ) The objective is larger than the eyepiece. [ IIT 1992 ]

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39 ) A thin prism P1 with angle 4° and made of glass having refractive index 1.54 is

combined with another thin prism P2 made of glass having refractive index 1.72 to produce dispersion without deviation. The angle of the prism P2 is

( a ) 5.33° ( b ) 4° ( c ) 3° ( d ) 2.6° [ IIT 1990 ] 40 ) Two thin convex lenses of focal

lengths f1 and f2 are separated by a horizontal distance d ( where d < f1 and d < f2 ), and their centres are displaced by a vertical separation ∆ as shown in the figure. Taking the origin of coordinates, O, at the centre of the first lens, the x and y coordinates of the focal point of the lens system, for a parallel beam of rays coming from the left, are given by

( a ) x = 21

21

ff

ff+

, y = ∆ ( b ) x = d ) d (

2121

-ffff

++

, y = 21

2

∆

ff +

( c ) x = d

) d ( d 21

121-

-ff

fff++

, y = d ) d ( ∆

211

--

fff

+

( d ) x = d

) d ( d 21

121-

-ff

fff++

, y = 0 [ IIT 1993 ]

41 ) A beam of light consisting of red green and blue colours

is incident on a right-angled prism as shown in the figure. The refractive indices of the material of the prism for the red, green and blue wavelengths are 1.39, 1.44 and 1.47 respectively. The prism will

( a ) separate part of the red colour from the green and blue colours

( b ) separate part of the blue colour from the red and green colours

( c ) separate all the three colours from one another ( d ) not separate even partially any colour from the other two colours [ IIT 1989 ] 42 ) An astronomical telescope has an angular magnification of magnitude 5 for distant

objects. The separation between the objective and the eye-piece is 36 cm and the final image is formed at infinity. The focal length f0 of the objective and fe of the eye-piece are

( a ) 45 cm and - 9 cm ( b ) 50 cm and 10 cm ( c ) 7.2 cm and 5 cm ( d ) 30 cm and 6 cm [ IIT 1989 ] 43 ) A short linear object of length b lies along the axis of a concave mirror of focal

length f at a distance u from the pole of the mirror. The size of the image is approximately equal to

( a ) 21

u b

f

f - ( b ) 21

u b

f

f -

( c )

f

f - u b ( d ) 2

u b

f

f -

[ IIT 1988 ]

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44 ) A converging lens is used to form an image on a screen. When the upper half of the

lens is covered by an opaque screen ( a ) half the image will disappear ( b ) complete image will be formed ( c ) intensity of the image will increase ( d ) intensity of the image will decrease [ IIT 1986 ] 45 ) A ray of light from a denser medium strikes a rarer

medium at an angle of incidence i ( see figure ). The reflected and refracted rays make an angle of 90° with each other. The angles of reflection and refraction are r and r’. The critical angle is

( a ) sin - 1 ( tan r ) ( b ) sin - 1 ( tan r’ ) ( c ) sin - 1 ( tan i ) ( d ) tan - 1 ( sin i ) [ IIT 1983 ] 46 ) A convex lens of focal length 40 cm is in contact with a concave lens of focal length

25 cm. The power of the combination in diopters is ( a ) - 1.5 ( b ) - 6.5 ( c ) + 6.5 ( d ) + 6.67 [ IIT 1982 ] 47 ) A glass prism of refractive index 1.5 is immersed in water ( refractive index 4 / 3 ). A light beam incident normally on the face AB ( see figure ) is totally reflected to reach the face BC, if

( a ) sin θ ≥ 98 ( b )

32 < sin θ <

98 ( c ) sin θ ≤

32

[ IIT 1981 ] 48 ) When a ray of light enters a glass slab from air ( a ) its wavelength increases ( b ) neither its wavelength nor its frequency changes ( c ) its frequency increases ( d ) its wavelength decreases [ IIT 1980 ] 49 ) An electric bulb illuminates a plane surface. The intensity of illumination on the surface

at a point 2 m away from the bulb is 5 x 10 - 4 phot ( lumens per sq. cm. ). The line joining the bulb to the point makes an angle of 60° with the normal to the surface. The intensity of the bulb in candela (candle power ) is

( a ) 40√3 ( b ) 40 ( c ) 20 ( d ) 40 x 10 - 4 [ IIT 1980 ] 50 ) Two plane mirrors are inclined to each other at an angle θ. If a ray of light incident on

the first mirror is parallel to the second mirror and that reflected from the second mirror is parallel to the second mirror, then the angle θ is

( a ) 30° ( b ) 45° ( c ) 60° ( d ) 75°

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51 ) A lens made of a material of refractive index µ2 is immersed in a medium of refractive

index µ1. If the radii of curvature of the lens surfaces are R1 and R2, then the focal length f of the lens is given by

( a )

= µ

2R1

1R1 ) 1 2 ( 1 --

f ( b )

=

µµ

2R1

1R1

11 1 2 --

f

( c )

= +

µµ

2R1

1R1 1 1

12 -

f ( d )

= +

µµ

2R1

1R1 1 1

21 -

f

Answers

1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 a b b a c a a a c d c c b d a c b c b b

21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 b c b d b d c b a d a b c,d d a b,c c a,c,d c c,d

41 42 43 44 45 46 47 48 49 50 51 c d d b,d a,c a a d b c b

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