NCERT Solutions Class 12 Physics Chapter 9

Q.1 A small candle, 2.5 cm in size is placed at 27 cm in front of a concave mirror of radius of curvature 36 cm. At what distance from the mirror should a screen be placed in order to obtain a sharp image? Describe the nature and size of the image. If the candle is moved closer to the mirror, how would the screen have to be moved?

Ans.

Given, size of candle, h₁ = 2.5 cm
Object distance, u = −27 cm
Radius of curvature of the concave mirror, R = −36 cm

$\begin{array}{l}\text{Focal length of the concave mirror\hspace{0.33em}is\hspace{0.33em}given\hspace{0.33em}as:}\\ \text{f =}\frac{\text{R}}{\text{2}}\text{=}\frac{\text{-36}}{\text{2}}\text{\hspace{0.17em}cm=-18\hspace{0.33em}cm\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}}\end{array}$

Let size of image = h₂
Let image distance = v
From the mirror formula, the image distance can be obtained as:

$\begin{array}{l}\frac{1}{\mathrm{v}}+\frac{1}{\mathrm{u}}=\frac{1}{\mathrm{f}}\\ \therefore \frac{1}{\mathrm{v}}=\frac{1}{\mathrm{f}}-\frac{1}{\mathrm{u}}\\ =\frac{1}{-18\mathrm{cm}}+\frac{1}{27\mathrm{cm}}=\frac{-3+2}{54\mathrm{cm}}=-\frac{1}{54\mathrm{cm}}\\ \therefore \text{Image\hspace{0.33em}distance},\mathrm{v}=-54\text{\hspace{0.33em}cm}\end{array}$

Therefore, in order to obtain sharp image of the candle on the screen, the screen should be placed 54 cm away from the mirror.
Magnification of the image is given as:

$\begin{array}{l}\text{m=}\frac{{\text{-h}}_{\text{2}}}{{\text{h}}_{\text{1}}}\\ \text{=}\frac{\text{-v}}{\text{-u}}\text{=}\frac{\text{v}}{\text{u}}\\ \therefore \frac{{\text{-h}}_{\text{2}}}{\text{2.5 cm}}\text{=}\frac{\left(\text{-54 cm}\right)}{\left(\text{-27 cm}\right)}\text{= 2}\\ \therefore {\text{Size\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}image,\hspace{0.33em}h}}_{\text{2}}\text{=-5\hspace{0.33em}cm}\\ \therefore \text{The\hspace{0.33em}image\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}candle\hspace{0.33em}is\hspace{0.33em}real,\hspace{0.33em}inverted\hspace{0.33em}and\hspace{0.33em}magnified.}\end{array}$

If the candle is moved closer to the mirror, then the screen should be moved away from the mirror in order to obtain the image on the screen.

Q.2 A 4.5 cm needle is placed 12 cm away from a convex mirror of focal length 15 cm. Give the location of the image and the magnification. Describe what happens as the needle is moved farther from the mirror.

Ans.

$\begin{array}{l}\begin{array}{l}{\text{Height of the needle, h}}_{\text{1}}\text{= 4.5 cm}\\ \text{Object distance, u = -12 cm}\\ \text{Focal length of the convex mirror, f = 15 cm}\\ \text{Let image distance = v}\\ \text{From the mirror formula, the image distance can be obtained as:}\end{array}\\ \frac{\text{1}}{\text{v}}\text{+}\frac{\text{1}}{\text{u}}\text{=}\frac{\text{1}}{\text{f}}\\ \therefore \frac{\text{1}}{\text{v}}\text{=}\frac{\text{1}}{\text{f}}\text{–}\frac{\text{1}}{\text{u}}\\ \frac{\text{1}}{\text{v}}\text{=}\frac{\text{1}}{\text{15 cm}}\text{+}\frac{\text{1}}{\text{12 cm}}\\ \frac{\text{1}}{\text{v}}\text{=}\frac{\text{4 + 5}}{\text{60 cm}}\text{=}\frac{\text{9}}{\text{60 cm}}\\ \therefore \text{Image\hspace{0.33em}distance,\hspace{0.33em}v =}\frac{\text{60 cm}}{\text{9}}\text{= 6.7\hspace{0.33em}cm}\\ \text{Therefore, the virtual image is formed at 6.7 cm behind the mirror.}\\ \text{The magnification of the image is given as:}\\ \text{m =}\frac{{\text{h}}_{\text{2}}}{{\text{h}}_{\text{1}}}\text{= –}\frac{\text{v}}{\text{u}}\\ \therefore \frac{{\text{h}}_{\text{2}}}{\text{4.5 cm}}\text{= –}\frac{\text{6.7 cm}}{\text{12 cm}}\\ \therefore {\text{h}}_{\text{2}}\text{= –}\frac{\text{6.7}}{\text{12}}\text{× 4.5 cm = 2.5\hspace{0.33em}cm}\\ \therefore {\text{Size\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}image, h}}_{\text{2}}\text{= 2.5\hspace{0.33em}cm}\\ \text{m\hspace{0.17em} = \hspace{0.17em}}\frac{{\text{h}}_{\text{2}}}{{\text{h}}_{\text{1}}}\text{=}\frac{\text{\hspace{0.17em}2.5 cm}}{\text{4.5 cm}}\text{= 0.56}\\ \therefore \text{The\hspace{0.33em}image\hspace{0.33em}formed\hspace{0.33em}is\hspace{0.33em}virtual\hspace{0.33em}and\hspace{0.33em}erect.}\\ \text{If the needle is moved farther from the mirror, then the image moves away from the mirror up}\\ \text{to its principal focus and its magnification goes on decreasing.}\end{array}$

Q.3 A tank is filled with water to a height of 12.5 cm. The apparent depth of a needle lying at the bottom of the tank is measured by a microscope to be 9.4 cm. What is the refractive index of water? If water is replaced by a liquid of refractive index 1.63 up to the same height, by what distance would the microscope have to be moved to focus on the needle again?

Ans.

Given, actual depth of the needle in water,

h₁ = 12.5 cm

Apparent depth of the needle in water,

h₂ = 9.4 cm

Let refractive index of water = μ

The refractive index of water is given as:

\begin{array}{l}\mu =\frac{\text{Real}\text{depth}}{\text{Apparent}\text{depth}}=\frac{12.5}{9.4}\\ =1.33\\ \text{For}\text{the}\text{second}\text{case:}\\ \text{Refractive}\text{index}\text{of}\text{the}\text{liquid},\mu =1.63\\ \text{Real}\text{depth}\text{of}\text{needle}=12.5cm\\ \text{Let}\text{apparent}\text{depth}=y\\ \text{The}\text{relation}\text{for}\text{refractive}\text{index}\text{is}\text{given}\text{as:}\\ \mu =\frac{\text{Real}\text{depth}}{\text{Apparent}\text{depth}}\\ \therefore 1.63=\frac{12.5}{y}\\ \therefore y=\frac{12.5}{1.63}\\ =7.67\text{cm}\end{array}

Therefore, new apparent depth of the needle =7.67 cm

Therefore, the distance by which the microscope has to be moved upwards = 9.4 – 7.67 = 1.73 cm

Q.4 Figures (a) and (b) show refraction of a ray in air incident at 60° with the normal to a glass-air and water-air interface, respectively. Predict the angle of refraction in glass when the angle of incidence in water is 45^o with the normal to a water-glass interface [Fig. (c)].

Ans.

From the given figure, for the glass − air interface:
Angle of incidence, i = 60°
Angle of refraction, r = 35°
According to Snell’s law, the relative refractive index of glass with respect to air is given as:

\begin{array}{l}\text{μ}_{\text{air}}{}_{\text{glass}}\text{=}\frac{{\text{sin60}}^{\text{o}}}{{\text{sin35}}^{\text{o}}}\\ \text{=}\frac{\text{0}\text{.8660}}{\text{0}\text{.5736}}\\ \text{= 1}\text{.51}\to \text{(i)}\end{array}

From the given figure, for the air − water interface:
Angle of incidence, i = 60°
Angle of refraction, r = 47°
According to Snell’s law, the relative refractive index of water with respect to air is given as:

\begin{array}{l}\text{μ}_{\text{air}}{}_{\text{water}}\text{=}\frac{{\text{sin60}}^{\text{o}}}{{\text{sin47}}^{\text{o}}}\\ \text{=}\frac{\text{0}\text{.8660}}{\text{0}\text{.7314}}\\ \text{= 1}\text{.184}\to \text{(ii)}\end{array}

From equation (i) and (ii), the relative refractive index of glass with respect to water is given as:

$\begin{array}{l}\mathrm{\mu }_{\text{glass}}^{\text{water}}=\frac{\mathrm{\mu }_{\text{glass}}^{\text{air}}}{\mathrm{\mu }_{\text{water}}^{\text{air}}}\\ =\frac{1.51}{1.184}\\ =1.275\to \left(\mathrm{iii}\right)\end{array}$

$\begin{array}{l}\text{From\hspace{0.17em}the\hspace{0.17em}given\hspace{0.17em}figure,\hspace{0.17em}for\hspace{0.17em}the\hspace{0.17em}water}-\text{glass\hspace{0.17em}interface:}\\ \text{Given,\hspace{0.17em}angle\hspace{0.17em}of\hspace{0.17em}incidence},\mathrm{i}={45}^{\circ }\\ \text{Let\hspace{0.17em}angle\hspace{0.17em}of\hspace{0.17em}refraction\hspace{0.17em}}=\mathrm{r}\end{array}$

$\begin{array}{l}\text{According\hspace{0.17em}to\hspace{0.17em}Snell’s\hspace{0.17em}law,\hspace{0.17em}the\hspace{0.17em}refractive\hspace{0.17em}index\hspace{0.17em}of\hspace{0.17em}glass\hspace{0.17em}}\\ \text{with\hspace{0.17em}respect\hspace{0.17em}to\hspace{0.17em}water\hspace{0.17em}is\hspace{0.17em}given\hspace{0.17em}as}:\\ \mathrm{\mu }_{\text{glass}}^{\text{water}}=\frac{\mathrm{sini}}{\mathrm{sinr}}\\ =\frac{\sin {45}^{\circ }}{\mathrm{sinr}}\to \left(\mathrm{iv}\right)\\ \text{From\hspace{0.17em}equation\hspace{0.17em}(iii)\hspace{0.17em}and\hspace{0.17em}(iv),\hspace{0.17em}we\hspace{0.17em}have:}\\ 1.275=\frac{\sin {45}^{\circ }}{\mathrm{sinr}}\\ \therefore \mathrm{sinr}=\frac{0.7071}{1.275}\\ =0.5546\\ \therefore \mathrm{r}={\sin }^{-1}(0.5546)\\ =33{.68}^{\circ }\end{array}$

Q.5 A small bulb is placed at the bottom of a tank containing water to a depth of 80 cm. What is the area of the surface of water through which light from the bulb can emerge out? Refractive index of water is 1.33. (Consider the bulb to be a point source.)

Ans.

The given situation is shown in the following figure.

Here, actual depth of bulb, MO = 80 cm = 0.8 m

Refractive index of water, μ =1.33

Assuming the bulb to a point source,

\begin{array}{l}\text{Area of the surface through which the light from the bulb}\\ \text{can emerge out =Area of circle of radius, r =}\frac{\text{NP}}{\text{2}}\text{= ON = OP}\\ \text{For}\text{angle}\text{of}\text{incidence,}\text{i = Critical}\text{angle = C}\\ \text{Angle}\text{of}\text{refraction,}{\text{r = 90}}^{\text{o}}\\ \text{According}\text{to}\text{Snell’s}\text{law,}\text{the}\text{relation}\text{for}\text{refractive}\text{index}\text{of}\\ \text{water}\text{is}\text{given}\text{as:}\\ \mu =\frac{\sin r}{\sin i}\\ \therefore \text{1}\text{.33 =}\frac{{\text{sin90}}^{\text{o}}}{\text{sinC}}\text{=}\frac{\text{1}}{\text{sinC}}\\ \therefore \text{sin C =}\frac{\text{1}}{\text{1}\text{.33}}\text{= 0}\text{.75}\\ \therefore {\text{C = sin}}^{\text{-1}}\left(\text{0}\text{.75}\right)\text{= 48}{\text{.6}}^{\text{o}}\\ \text{From}\text{the}\text{given}\text{figure,}\text{in}\Delta OPM,\text{we}\text{have}:\\ \text{tani =}\frac{\text{OP}}{\text{OM}}\\ \therefore \text{OP = OM tan48}{\text{.6}}^{\text{o}}\\ \text{= 0}\text{.8 × 1}\text{.1345}\\ \text{= 0}\text{.907}\text{m}\\ \text{Area of the surface through which the light from the bulb}\\ \text{can emerge out}\text{=}\pi {\text{r}}^{\text{2}}\\ \text{= 3}\text{.14}{\left(\text{OP}\right)}^{\text{2}}\\ \text{= 3}\text{.14}{\left(\text{0}\text{.907}\right)}^{\text{2}}\\ \text{= 2}\text{.59}{\text{m}}^{\text{2}}\end{array}

Q.6 A prism is made of glass of unknown refractive index. A parallel beam of light is incident on a face of the prism. The angle of minimum deviation is measured to be 40°. What is the refractive index of the material of the prism? The refracting angle of the prism is 60°. If the prism is placed in water (refractive index 1.33), predict the new angle of minimum deviation of a parallel beam of light.

Ans.

$\begin{array}{l}{\text{Angle of minimum deviation,δ}}_{\text{m}}\text{= 40°}\\ \text{Angle of the prism,A = 60°}\\ \text{Refractive index of water,μ = 1.33}\\ \text{Let refractive index of the material of the prism =The angle of deviation is related to refractive index as:}\\ \text{Relation\hspace{0.33em}connecting\hspace{0.33em}refractive\hspace{0.33em}index\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}material\hspace{0.33em}}\\ \text{of\hspace{0.33em}the\hspace{0.33em}prism\hspace{0.33em}and\hspace{0.33em}angle\hspace{0.33em}of\hspace{0.33em}deviation\hspace{0.33em}is\hspace{0.33em}given\hspace{0.33em}as:}\\ {\text{μ}}_{\text{P}}\text{=}\frac{\text{sin}\left(\frac{{\text{A + δ}}_{\text{m}}}{\text{2}}\right)}{\text{sin}\frac{\text{A}}{\text{2}}}\\ \text{=}\frac{\text{sin}\left(\frac{{\text{60}}^{\text{o}}{\text{+ 40}}^{\text{o}}}{\text{2}}\right)}{\text{sin}\frac{{\text{60}}^{\text{o}}}{\text{2}}}\text{=}\frac{{\text{sin50}}^{\text{o}}}{{\text{sin30}}^{\text{o}}}\text{= 1.532}\\ \therefore \text{Refractive\hspace{0.33em}index\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}material\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}prism=1.532}\\ \text{When\hspace{0.33em}the\hspace{0.33em}placed\hspace{0.33em}in\hspace{0.33em}water:}\\ {\text{Let\hspace{0.33em}new\hspace{0.33em}minimum\hspace{0.33em}angle\hspace{0.33em}of\hspace{0.33em}deviation=δ}}_{\text{m}}\text{‘}\\ \text{Refractive\hspace{0.33em}index\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}material\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}prism\hspace{0.33em}with\hspace{0.33em}respect\hspace{0.33em}}\\ \text{to\hspace{0.33em}water\hspace{0.33em}is\hspace{0.33em}given\hspace{0.33em}as:}\\ \text{μ}_{\text{P}}^{\text{w}}\text{=}\frac{{\text{μ}}_{\text{P}}}{\text{μ}}\\ \text{=}\frac{\text{sin}\left(\frac{{\text{A + δ}}_{\text{m}}\text{‘}}{\text{2}}\right)}{\text{sin}\left(\frac{\text{A}}{\text{2}}\right)}\\ \therefore \text{sin}\left(\frac{{\text{A+δ}}_{\text{m}}\text{‘}}{\text{2}}\right)\text{= sin}\frac{\text{A}}{\text{2}}\text{×}\frac{{\text{μ}}_{\text{P}}}{\text{μ}}\\ \therefore \text{sin}\left(\frac{{\text{A+δ}}_{\text{m}}\text{‘}}{\text{2}}\right)\text{= sin}\left(\frac{{\text{60}}^{\text{o}}}{\text{2}}\right)\text{×}\frac{\text{1.532}}{\text{1.33}}\\ \text{=}\frac{\text{1}}{\text{2}}\text{×}\frac{\text{1.532}}{\text{1.33}}\text{= 0.5759}\\ {\text{= sin35.16}}^{\text{o}}\\ \therefore \text{sin}\left(\frac{{\text{A+δ}}_{\text{m}}\text{‘}}{\text{2}}\right){\text{=sin35.16}}^{\text{o}}\\ \therefore \frac{{\text{A+δ}}_{\text{m}}\text{‘}}{\text{2}}{\text{=35.16}}^{\text{o}}\\ \therefore {\text{A+δ}}_{\text{m}}{\text{‘=70.32}}^{\text{o}}\\ \therefore {\text{δ}}_{\text{m}}{\text{‘=70.32}}^{\text{o}}\text{– A}\\ {\text{=70.32}}^{\text{o}}{\text{– 60}}^{\text{o}}{\text{=10.32}}^{\text{o}}\\ \text{Therefore, the new minimum angle of deviation of the parallel beam of light= 10.20°}\end{array}$

Q.7 Double-convex lenses are to be manufactured from a glass of refractive index 1.55, with both faces of the same radius of curvature. What is the radius of curvature required if the focal length is to be 20 cm?

Ans.

Here, refractive index of glass, μ =1.55
Focal length of the double-convex lens, f = 20 cm
Since radius of curvature of both the faces of the given double convex lens are the same,
Let radius of curvature of one face of the lens, R₁=R
Let radius of curvature of the other face of the lens, R₂ = -R
From lens maker’s formula, we have:

\begin{array}{l}\frac{\text{1}}{\text{f}}\text{=}\left(\text{μ – 1}\right)\left[\frac{\text{1}}{{\text{R}}_{\text{1}}}\text{–}\frac{\text{1}}{{\text{R}}_{\text{2}}}\right]\\ \frac{\text{1}}{\text{20 cm}}\text{=}\left(\text{1}\text{.55 – 1}\right)\left[\frac{\text{1}}{\text{R}}\text{+}\frac{\text{1}}{\text{R}}\right]\\ \frac{\text{1}}{\text{20 cm}}\text{= 0}\text{.55 ×}\frac{\text{2}}{\text{R}}\\ \therefore \text{R = 0}\text{.55 × 2 × 20 cm}\\ \text{= 22}\text{cm}\end{array}

Therefore, radius of curvature of the given double-convex lens = 22 cm

Q.8 A beam of light converges at a point P. Now a lens is placed in the path of the convergent beam 12 cm from P. At what point does the beam converge if the lens is (a) a convex lens of focal length 20 cm, and (b) a concave lens of focal length 16 cm?

Ans.

In this situation, the point P on the right side of the lens acts as a virtual object.
Object distance, u = 12 cm
(a) Here, focal length of the convex lens, f = 20 cm
Let image distance = v
From the lens formula, we have:

$\begin{array}{l}\frac{\text{1}}{\text{v}}\text{–}\frac{\text{1}}{\text{u}}\text{=}\frac{\text{1}}{\text{f}}\\ \Rightarrow \frac{\text{1}}{\text{v}}\text{=}\frac{\text{1}}{\text{f}}\text{+}\frac{\text{1}}{\text{u}}\\ \frac{\text{1}}{\text{v}}\text{=}\frac{\text{1}}{\text{20 cm}}\text{+}\frac{\text{1}}{\text{12 cm}}\text{=}\frac{\text{3 + 5}}{\text{60 cm}}\\ \therefore \text{v =}\frac{\text{60 cm}}{\text{8}}\text{= 7.5 cm}\\ \therefore \text{The image is formed at 7.5 cm to the right of the lens.}\end{array}$

(b) Here, focal length of the concave lens,f = −16 cm
Let image distance = v
From the lens formula,

\begin{array}{l}\frac{\text{1}}{\text{v}}\text{–}\frac{\text{1}}{\text{u}}\text{=}\frac{\text{1}}{\text{f}}\\ \therefore \frac{\text{1}}{\text{v}}\text{=}\frac{\text{1}}{\text{f}}\text{+}\frac{\text{1}}{\text{u}}\\ \frac{\text{1}}{\text{v}}\text{= –}\frac{\text{1}}{\text{16 cm}}\text{+}\frac{\text{1}}{\text{12 cm}}\\ \frac{\text{1}}{\text{v}}\text{=}\frac{\text{-3 + 4}}{\text{48 cm}}\text{=}\frac{\text{1}}{\text{48}}\\ \therefore \text{v =}\text{48}\text{cm}\\ \therefore \text{The}\text{image}\text{is}\text{formed}\text{at}\text{48}\text{cm}\text{to}\text{the}\text{right}\text{of}\text{the}\text{lens}\text{.}\end{array}

Q.9 An object of size 3.0 cm is placed 14 cm in front of a concave lens of focal length 21 cm. Describe the image produced by the lens. What happens if the object is moved further away from the lens?

Ans.

$\begin{array}{l}{\text{Here, size of the object, h}}_{\text{1}}\text{= 3 cm}\\ \text{Object distance, u = -14 cm}\\ \text{Focal length of the concave lens, f = -21 cm}\\ \text{Let image distance = v}\\ {\text{Let size of the object=h}}_{\text{2}}\\ \text{From the lens formula, we have:}\end{array}$

$\begin{array}{l}\frac{\text{1}}{\text{v}}\text{–}\frac{\text{1}}{\text{u}}\text{=}\frac{\text{1}}{\text{f}}\\ \therefore \frac{\text{1}}{\text{v}}\text{=}\frac{\text{1}}{\text{f}}\text{+}\frac{\text{1}}{\text{u}}\\ \text{= –}\frac{\text{1}}{\text{21 cm}}\text{–}\frac{\text{1}}{\text{14 cm}}\\ \text{=}\frac{\text{-2 – 3}}{\text{42 cm}}\text{=}\frac{\text{-5}}{\text{42 cm}}\\ \therefore \text{v = –}\frac{\text{42}}{\text{5}}\text{\hspace{0.33em}cm = -8.4\hspace{0.33em}cm}\\ \therefore \text{The\hspace{0.33em}image\hspace{0.33em}formed\hspace{0.33em}is\hspace{0.33em}vertual,\hspace{0.33em}erect\hspace{0.33em}and\hspace{0.33em}8.4\hspace{0.33em}cm\hspace{0.33em}away\hspace{0.33em}from\hspace{0.33em}}\\ \text{the\hspace{0.33em}lens\hspace{0.33em}on\hspace{0.33em}the\hspace{0.33em}same\hspace{0.33em}side\hspace{0.33em}as\hspace{0.33em}the\hspace{0.33em}object.}\\ \text{Magnification\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}lens\hspace{0.33em}is\hspace{0.33em}given\hspace{0.33em}by\hspace{0.33em}the\hspace{0.33em}relation:}\\ \text{m =}\frac{{\text{h}}_{\text{2}}}{{\text{h}}_{\text{1}}}\text{=}\frac{\text{v}}{\text{u}}\\ \therefore {\text{h}}_{\text{2}}\text{=}\frac{\text{-8.4 cm}}{\text{-14 cm}}\text{× 3}\\ \text{= 0.6 cm × 3 = 1.8\hspace{0.33em}cm}\end{array}$

Q.10 What is the focal length of a convex lens of focal length 30 cm in contact with a concave lens of focal length 20 cm? Is the system a converging or a diverging lens? Ignore thickness of the lenses.

Ans.

Here, focal length of the convex lens,
f₁ = 30 cm
Focal length of the concave lens,
f₂ = −20 cm
Let focal length of the system of lenses = f
The equivalent focal length of the combination of two lenses in contact is given as:

$\begin{array}{l}\frac{\text{1}}{\text{f}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{1}}}\text{+}\frac{\text{1}}{{\text{f}}_{\text{2}}}\\ \text{=}\frac{\text{1}}{\text{30 cm}}\text{–}\frac{\text{1}}{\text{20 cm}}\\ \text{=}\frac{\text{2 – 3}}{\text{60 cm}}\\ \text{=-}\frac{\text{1}}{\text{60 cm}}\\ \therefore \text{f = -60\hspace{0.33em}cm}\\ \begin{array}{l}\text{The negative sign indicates it is a diverging lens with}\\ \text{the focal length of the combination of lenses=60 cm}\end{array}\end{array}$

Q.11 A compound microscope consists of an objective lens of focal length 2.0 cm and an eyepiece of focal length 6.25 cm separated by a distance of 15 cm. How far from the objective should an object be placed in order to obtain the final image at (a) the least distance of distinct vision (25 cm), and (b) at infinity? What is the magnifying power of the microscope in each case?

Ans.

\begin{array}{l}{\text{Here, focal length of the objective lens, f}}_{\text{o}}\text{= 2}\text{.0 cm}\\ {\text{Focal length of the eyepiece, f}}_{\text{e}}\text{= 6}\text{.25 cm}\\ \text{Distance between the objective lens and the eyepiece, d = 15 cm}\\ \left(\text{a}\right)\text{Least distance of distinct vision, d’ = 25 cm}\\ {\text{Image distance for the eyepiece, v}}_{\text{e}}\text{= -25 cm}\\ {\text{Let object distance for the eyepiece = u}}_{\text{e}}\\ \text{From the lens formula, we have}\\ \frac{\text{1}}{{\text{v}}_{\text{e}}}\text{–}\frac{\text{1}}{{\text{u}}_{\text{e}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{e}}}\\ \therefore \frac{\text{1}}{{\text{u}}_{\text{e}}}\text{=}\frac{\text{1}}{{\text{v}}_{\text{e}}}\text{–}\frac{\text{1}}{{\text{f}}_{\text{e}}}\\ \frac{\text{1}}{{\text{u}}_{\text{e}}}\text{=}\frac{\text{1}}{\text{-25 cm}}\text{–}\frac{\text{1}}{\text{6}\text{.25 cm}}\text{=}\frac{\text{-1}}{\text{5 cm}}\\ \therefore {\text{u}}_{\text{e}}\text{= -5}\text{cm}\\ \text{Image distance for the objective lens is given as}\\ {\text{v}}_{\text{o}}{\text{= d + u}}_{\text{e}}\text{= 15 cm – 5 cm = 10 cm}\\ {\text{Object distance for the objective lens = u}}_{\text{o}}\\ \text{From the lens formula, we have}\\ \frac{\text{1}}{{\text{v}}_{\text{o}}}\text{–}\frac{\text{1}}{{\text{u}}_{\text{o}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{o}}}\\ \therefore \frac{\text{1}}{{\text{u}}_{\text{o}}}\text{=}\frac{\text{1}}{{\text{v}}_{\text{o}}}\text{–}\frac{\text{1}}{{\text{f}}_{\text{o}}}\\ \frac{\text{1}}{{\text{u}}_{\text{o}}}\text{=}\frac{\text{1}}{\text{10 cm}}\text{–}\frac{\text{1}}{\text{2 cm}}\text{=}\frac{\text{-2}}{\text{5 cm}}\\ \therefore {\text{u}}_{\text{o}}\text{= -2}\text{.5}\text{cm}\\ \text{Magnifying}\text{power}\text{of}\text{the}\text{compound}\text{microscope}\text{is}\text{given}\text{as:}\\ \text{m =}\frac{{\text{v}}_{\text{o}}}{\left|{\text{u}}_{\text{o}}\right|}\left(\text{1+}\frac{\text{d’}}{{\text{f}}_{\text{e}}}\right)\text{=}\frac{\text{10 cm}}{\text{2}\text{.5 cm}}\left(\text{1+}\frac{\text{25 cm}}{\text{6}\text{.25 cm}}\right)\text{= 20}\\ \therefore \text{Magnifying}\text{power}\text{of}\text{the}\text{compound}\text{microscope = 20}\end{array}

\begin{array}{l}\text{(b)}\text{Since}\text{the}\text{image}\text{is}\text{formed}\text{at}\text{infinity,}\\ \therefore \text{Image}\text{distance}\text{for}\text{the}\text{eyepiece,}{\text{v}}_{\text{e}}\text{=}\infty \\ \text{Let}\text{object}\text{distance}\text{for}\text{the}{\text{eyepiece be u}}_{\text{e}}\\ \text{From}\text{lens}\text{formula,}\text{we}\text{have}\\ \frac{\text{1}}{{\text{v}}_{\text{e}}}\text{–}\frac{\text{1}}{{\text{u}}_{\text{e}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{e}}}\\ \frac{\text{1}}{\infty }\text{–}\frac{\text{1}}{{\text{u}}_{\text{e}}}\text{=}\frac{\text{1}}{\text{6}\text{.25}}\\ \therefore {\text{u}}_{\text{e}}\text{=-6}\text{.25}\text{cm}\\ \text{Image}\text{distance}\text{for}\text{the}\text{objective}\text{lens}\text{is}\text{given}\text{as}\\ {\text{v}}_{\text{o}}{\text{= d + u}}_{\text{e}}\\ {\text{v}}_{\text{o}}\text{= 15 cm – 6}\text{.25 cm = 8}\text{.75}\text{cm}\\ \text{Let}\text{object}\text{distance}\text{for}\text{the}\text{objective}{\text{lens be u}}_{\text{o}}\\ \text{From}\text{lens}\text{formula,}\text{we}\text{have}\\ \frac{\text{1}}{{\text{v}}_{\text{o}}}\text{–}\frac{\text{1}}{{\text{u}}_{\text{o}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{o}}}\\ \therefore \frac{\text{1}}{{\text{u}}_{\text{o}}}\text{=}\frac{\text{1}}{{\text{v}}_{\text{o}}}\text{–}\frac{\text{1}}{{\text{f}}_{\text{o}}}\\ \frac{\text{1}}{{\text{u}}_{\text{o}}}\text{=}\frac{\text{1}}{\text{8}\text{.75 cm}}\text{–}\frac{\text{1}}{\text{2 cm}}\\ \therefore {\text{u}}_{\text{o}}\text{=-}\frac{\text{17}\text{.5}}{\text{6}\text{.75}}\text{cm = -2}\text{.59}\text{cm}\\ \text{Magnifying power of the microscope is given as}\\ \text{m =}\frac{{\text{v}}_{\text{o}}}{\left|{\text{u}}_{\text{o}}\right|}\text{×}\frac{{\text{v}}_{\text{e}}}{\left|{\text{u}}_{\text{e}}\right|}\\ \text{m =}\frac{\text{8}\text{.75 cm}}{\text{2}\text{.59 cm}}\text{×}\frac{\text{25 cm}}{\text{6}\text{.25 cm}}\text{= 13}\text{.5}\\ \text{Therefore, magnifying power of the microscope is 13}\text{.51}\text{.}\end{array}

Q.12 A person with a normal near point (25 cm) using a compound microscope with objective of focal length 8.0 mm and an eyepiece of focal length 2.5 cm can bring an object placed at 9.0 mm from the objective in sharp focus. What is the separation between the two lenses? Calculate the magnifying power of the microscope.

Ans.

\begin{array}{l}\text{Here, least distance of distinct vision, d = 25 cm}\\ \text{Focal length of the objective of the compound microscope, fo = 8 mm = 0}\text{.8 cm}\\ \text{Focal length of the eyepiece of the compound microscope, fe = 2}\text{.5 cm}\\ {\text{Object distance,u}}_{\text{o}}\text{= -9}\text{.0 mm = -0}\text{.9 cm}\\ \text{From the lens formula, we have:}\\ \frac{\text{1}}{{\text{v}}_{\text{e}}}\text{–}\frac{\text{1}}{{\text{u}}_{\text{e}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{e}}}\\ \therefore \frac{\text{1}}{{\text{u}}_{\text{e}}}\text{=}\frac{\text{1}}{{\text{v}}_{\text{e}}}\text{–}\frac{\text{1}}{{\text{f}}_{\text{e}}}\\ \text{Here,}\text{image}\text{distance,}\\ {\text{v}}_{\text{e}}\text{= -d = -25}\text{cm}\\ \therefore \frac{\text{1}}{{\text{u}}_{\text{e}}}\text{=}\frac{\text{1}}{\text{-25 cm}}\text{–}\frac{\text{1}}{\text{2}\text{.5 cm}}\\ \text{=}\frac{\text{-1 – 10}}{\text{25 cm}}\text{=}\frac{\text{-11}}{\text{25 cm}}\\ {\text{u}}_{\text{e}}\text{=}\frac{\text{-25}}{\text{11}}\text{= -2}\text{.27}\text{cm}\\ \text{In}\text{case}\text{of}\text{objective}\text{lens:}\\ \text{From}\text{lens}\text{formula,}\text{we}\text{have:}\\ \frac{\text{1}}{{\text{v}}_{\text{o}}}\text{–}\frac{\text{1}}{{\text{u}}_{\text{o}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{o}}}\\ \therefore \frac{\text{1}}{{\text{v}}_{\text{o}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{o}}}\text{+}\frac{\text{1}}{{\text{u}}_{\text{o}}}\text{=}\frac{\text{1}}{\text{0}\text{.8 cm}}\text{–}\frac{\text{1}}{\text{0}\text{.9 cm}}\\ \frac{\text{1}}{{\text{v}}_{\text{o}}}\text{=}\frac{\text{0}\text{.9 – 0}\text{.8}}{\text{0}\text{.72 cm}}\text{=}\frac{\text{0}\text{.1}}{\text{0}\text{.72}}\\ \therefore {\text{v}}_{\text{o}}\text{=}\frac{\text{0}\text{.72}}{\text{0}\text{.1}}\text{= 7}\text{.2}\text{cm}\\ \text{Thus, image}\text{distance}\text{for}\text{objective,}{\text{v}}_{\text{o}}\text{=7}\text{.2}\text{cm}\\ \therefore \text{Distance}\text{between}\text{the}\text{two}\text{lenses =}\left|{\text{u}}_{\text{e}}\right|{\text{+v}}_{\text{o}}\\ \text{2}\text{.27 cm + 7}\text{.2 cm = 9}\text{.47}\text{cm}\\ \text{Magnifying}\text{power}\text{of}\text{the}\text{microscope}\text{is}\text{given}\text{as:}\\ \text{m =}\frac{{\text{v}}_{\text{o}}}{\left|{\text{u}}_{\text{o}}\right|}\left(\text{1+}\frac{\text{d}}{{\text{f}}_{\text{e}}}\right)\\ \text{m =}\frac{\text{7}\text{.2 cm}}{\text{0}\text{.9 cm}}\left(\text{1+}\frac{\text{25 cm}}{\text{2}\text{.5 cm}}\right)\text{=88}\\ \therefore \text{Magnifying}\text{power}\text{of}\text{the}\text{microscope = 88}\end{array}

Q.13 A small telescope has an objective lens of focal length 144 cm and an eyepiece of focal length 6.0 cm. What is the magnifying power of the telescope? What is the separation between the objective and the eyepiece?

Ans.

Here, focal length of objective, f_o = 144 cm

Focal length of eyepiece, f_e = 6.0 cm

$\begin{array}{l}\text{m =}\frac{{\text{f}}_{\text{o}}}{{\text{f}}_{\text{e}}}\text{=}\frac{\text{144 cm}}{\text{6 cm}}=24\hfill \\ \begin{array}{l}\text{Therefore, for normal adjustment, the magnifying power of the telescope = 24}\\ \text{Separation between the objective and the eyepiece is given as: L = fo + fe}\\ \text{L = 144 cm + 6}\text{.0 cm = 150 cm}\end{array}\hfill \\ \begin{array}{l}\\ \end{array}\hfill \end{array}$

Q.14 (a) A giant refracting telescope at an observatory has an objective lens of focal length 15 m. If an eyepiece of focal length 1.0 cm is used, what is the angular magnification of the telescope?
(b) If this telescope is used to view the moon, what is the diameter of the image of the moon formed by the objective lens? The diameter of the moon is 3.48 × 10⁶ m, and the radius of lunar orbit is 3.8 × 10⁸ m.

Ans.

$\begin{array}{l}{\text{Here, focal length of the objective lens, f}}_{\text{o}}{\text{= 15 m = 15 × 10}}^{\text{2}}\text{cm}\\ {\text{Focal length of the eyepiece, f}}_{\text{e}}\text{= 1.0 cm}\\ \left(\text{a}\right)\text{Angular magnification of the telescope is given as:}\\ \text{m =}\frac{{\text{f}}_{\text{o}}}{{\text{f}}_{\text{e}}}\\ \text{=}\frac{{\text{15×10}}^{\text{2}}\text{cm}}{\text{10 cm}}\text{= 1500\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}\hspace{0.33em}}\\ \text{Therefore, angular magnification of the given refracting telescope = 1500}\\ {\text{b) Here, diameter of moon,D = 3.48 × 10}}^{\text{6}}\text{m}\\ {\text{Radius of lunar orbit,r}}_{\text{a}}{\text{= 3.8 × 10}}^{\text{8}}\text{m}\\ \text{Let diameter of the image of moon = d}\\ \text{Angle subtended by the diameter of the moon is given as:}\\ {\text{θ}}_{\text{m}}\text{=}\frac{\text{Diameter\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}moon}}{\text{Radius\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}lunar\hspace{0.33em}obbit}}\\ \text{=}\frac{\text{D}}{{\text{r}}_{\text{a}}}\text{=}\frac{{\text{3.48×10}}^{\text{6}}}{{\text{3.8×10}}^{\text{8}}}\\ \text{Angle\hspace{0.33em}subtended\hspace{0.33em}by\hspace{0.33em}the\hspace{0.33em}image\hspace{0.33em}is\hspace{0.33em}given\hspace{0.33em}as:}\\ {\text{θ}}_{\text{I}}\text{=}\frac{\text{Diameter\hspace{0.33em}of\hspace{0.33em}image}}{\text{Focal\hspace{0.33em}length\hspace{0.33em}of\hspace{0.33em}objective\hspace{0.33em}lens}}\\ \text{=}\frac{\text{d}}{{\text{f}}_{\text{o}}}\text{=}\frac{\text{d}}{\text{15}}\\ \text{Since,\hspace{0.33em}angle\hspace{0.33em}subtended\hspace{0.33em}by\hspace{0.33em}the\hspace{0.33em}diameter\hspace{0.33em}of\hspace{0.33em}moon=angle}\\ \text{subtended\hspace{0.33em}by\hspace{0.33em}image}\\ \therefore {\text{θ}}_{\text{m}}{\text{= θ}}_{\text{I}}\\ \therefore \frac{{\text{3.48×10}}^{\text{6}}}{{\text{3.8×10}}^{\text{8}}}\text{=}\frac{\text{d}}{\text{15}}\\ \therefore \text{d = 15 ×}\frac{{\text{3.48×10}}^{\text{6}}}{{\text{3.8×10}}^{\text{8}}}\\ {\text{= 13.73×10}}^{\text{-2}}\text{\hspace{0.33em}m = 13.73\hspace{0.33em}cm}\\ \begin{array}{l}\text{Since, angle subtended by the diameter of the moon = angle subtended by the image}\\ \text{Therefore, the diameter of the image of the moon formed by the objective lens = 13.74 cm}\end{array}\end{array}$

Q.15 Use the mirror equation to deduce that:
(a) an object placed between f and 2f of a concave mirror produces a real image beyond 2f.
(b) a convex mirror always produces a virtual image independent of the location of the object.
(c) the virtual image produced by a convex mirror is always diminished in size and is located between the focus and the pole.
(d) an object placed between the pole and focus of a concave mirror produces a virtual and enlarged image.
[Note: This exercise helps you deduce algebraically properties of images that one obtains from explicit ray diagrams.]

Ans.

(a) The mirror equation is given as:

\begin{array}{l}\frac{\text{1}}{\text{v}}\text{+}\frac{\text{1}}{\text{u}}\text{=}\frac{\text{1}}{\text{f}}\\ \therefore \frac{\text{1}}{\text{v}}\text{=}\frac{\text{1}}{\text{f}}\text{–}\frac{\text{1}}{\text{u}}\\ \text{For}\text{a}\text{concave}\text{mirror,}\text{the}\text{focal}\text{length}\text{is}\text{negative}\text{.}\\ \therefore \text{f < 0}\\ \text{Since}\text{object}\text{lies}\text{on}\text{the}\text{left,}\\ \therefore \text{Object}\text{distance,}\text{u < 0}\\ \text{Since}\text{the}\text{object}\text{is}\text{placed}\text{between}\text{f}\text{and}\text{2f,}\\ \therefore \text{2f < u < f}\\ \therefore \frac{\text{1}}{\text{2f}}\text{>}\frac{\text{1}}{\text{u}}\text{>}\frac{\text{1}}{\text{f}}\\ \therefore \text{–}\frac{\text{1}}{\text{2f}}\text{< –}\frac{\text{1}}{\text{u}}\text{< –}\frac{\text{1}}{\text{f}}\\ \therefore \frac{\text{1}}{\text{f}}\text{–}\frac{\text{1}}{\text{2f}}\text{<}\frac{\text{1}}{\text{f}}\text{–}\frac{\text{1}}{\text{u}}\text{< 0}\\ \therefore \frac{\text{1}}{\text{2f}}\text{<}\frac{\text{1}}{\text{v}}\text{< 0}\to \text{(i)}\left(\frac{\text{1}}{\text{f}}\text{–}\frac{\text{1}}{\text{u}}\text{=}\frac{\text{1}}{\text{v}}\right)\\ \text{Equation}\text{(i)}\text{shows}\text{that}\frac{\text{1}}{\text{v}}\text{is}\text{negative}\text{.}\\ \therefore \text{The}\text{value}\text{of}\text{v}\text{is}\text{negative}\text{.}\\ \text{It}\text{implies}\text{that}\text{the}\text{real}\text{image}\text{is}\text{formed}\text{.}\\ \text{Since,}\frac{\text{1}}{\text{2f}}\text{<}\frac{\text{1}}{\text{v}}\\ \therefore \text{2f > v}\\ \therefore \text{-v > -2f}\\ \therefore \text{Real}\text{image}\text{is}\text{formed}\text{beyond}\text{2f}\text{.}\\ \text{(b)}\text{From}\text{the}\text{mirror}\text{formula}\text{for}\text{a}\text{convex}\text{mirror,}\text{we}\text{have:}\\ \frac{\text{1}}{\text{f}}\text{=}\frac{\text{1}}{\text{v}}\text{+}\frac{\text{1}}{\text{u}}\\ \therefore \frac{\text{1}}{\text{v}}\text{=}\frac{\text{1}}{\text{f}}\text{–}\frac{\text{1}}{\text{u}}\to \text{(a)}\\ \text{Since}\text{for}\text{a}\text{convex}\text{mirror,}\text{the}\text{value}\text{of}\text{focal}\text{length}\text{is}\\ \text{always}\text{positive}\text{and}\text{object}\text{distance}\text{(u)}\text{is}\text{always}\text{negative}\text{.}\\ \therefore \text{f > 0}\text{and}\text{u < 0}\to \text{(b)}\\ \text{From}\text{equation}\text{(a)}\text{and}\text{(b),}\text{we}\text{obtain:}\\ \frac{\text{1}}{\text{v}}\text{=}\frac{\text{1}}{\text{f}}\text{–}\frac{\text{1}}{\left(\text{-u}\right)}\\ \text{=}\frac{\text{1}}{\text{f}}\text{+}\frac{\text{1}}{\text{u}}\text{>0}\\ \therefore \frac{\text{1}}{\text{v}}\text{> 0}\\ \therefore \text{The}\text{value}\text{of}\text{v}\text{is}\text{positive}\text{.}\\ \therefore \text{For}\text{a}\text{convex}\text{mirror,}\text{whatever}\text{may}\text{be}\text{the}\text{value}\text{of}\text{u,}\\ \text{the}\text{value}\text{of}\text{image}\text{distance}\text{(v)}\text{always}\text{remains}\text{positive}\text{.}\\ \therefore \text{Independent}\text{of}\text{the}\text{object}\text{distance,}\text{a}\text{convex}\text{mirror}\\ \text{always}\text{forms}\text{virtual}\text{images}\text{.}\\ \text{(c)}\text{Since}\text{focal}\text{length}\text{of}\text{a}\text{convex}\text{lens}\text{is}\text{positive}\text{.}\\ \therefore \text{f > 0}\\ \text{Since}\text{the}\text{object}\text{lies}\text{on}\text{the}\text{left,}\\ \therefore \text{Object}\text{distance,}\text{u < 0}\\ \text{From}\text{the}\text{mirror}\text{formula}\text{for}\text{convex}\text{mirror,}\text{we}\text{obtain:}\\ \frac{\text{1}}{\text{f}}\text{=}\frac{\text{1}}{\text{v}}\text{+}\frac{\text{1}}{\text{u}}\\ \therefore \frac{\text{1}}{\text{v}}\text{=}\frac{\text{1}}{\text{f}}\text{–}\frac{\text{1}}{\text{u}}\\ \text{Since}\text{f > 0}\text{and}\text{u < 0}\\ \therefore \frac{\text{1}}{\text{v}}\text{>}\frac{\text{1}}{\text{f}}\\ \therefore \text{v < f}\\ \therefore \text{The}\text{image}\text{formed}\text{by}\text{the}\text{convex}\text{mirror}\text{is}\text{diminished}\text{and}\\ \text{located}\text{between}\text{the}\text{focus}\text{and}\text{the}\text{pole}\text{.}\\ \text{(d)}\text{Since}\text{the}\text{focal}\text{length}\text{of}\text{a}\text{concave}\text{mirror}\text{is}\text{negative,}\\ \therefore \text{f < 0}\\ \text{Since}\text{the}\text{object}\text{is}\text{placed}\text{on}\text{the}\text{left}\text{of}\text{the}\text{concave}\\ \text{mirror,}\\ \therefore \text{u < 0}\\ \text{From}\text{the}\text{mirror}\text{formula}\text{for}\text{concave}\text{mirror,}\text{we}\text{obtain:}\\ \frac{\text{1}}{\text{f}}\text{=}\frac{\text{1}}{\text{v}}\text{+}\frac{\text{1}}{\text{u}}\\ \therefore \frac{\text{1}}{\text{v}}\text{=}\frac{\text{1}}{\text{f}}\text{–}\frac{\text{1}}{\text{u}}\\ \text{Since}\text{f < 0}\text{and}\text{u < 0}\\ \therefore \frac{\text{1}}{\text{v}}\text{=}\frac{\text{1}}{\text{-f}}\text{–}\frac{\text{1}}{\text{-u}}\\ \therefore \frac{\text{1}}{\text{v}}\text{=}\frac{\text{1}}{\text{u}}\text{–}\frac{\text{1}}{\text{f}}\to \text{(A)}\\ \text{Since}\left|\text{u}\right|\text{<}\left|\text{f}\right|\\ \therefore \frac{\text{1}}{\text{u}}\text{>}\frac{\text{1}}{\text{f}}\to \text{(B)}\\ \text{From}\text{equation}\text{(A)}\text{and}\text{(B),}\text{we}\text{obtain:}\\ \frac{\text{1}}{\text{v}}\text{> 0}\\ \therefore \text{v}\text{is}\text{positive}\text{.}\\ \text{It}\text{shows}\text{that}\text{the}\text{image}\text{is}\text{formed}\text{on}\text{the}\text{right}\text{side}\text{of}\\ \text{the}\text{mirror}\text{.}\\ \therefore \text{The}\text{virtual}\text{image}\text{is}\text{formed}\text{.}\\ \text{For}\text{u < 0}\text{and}\text{v > 0}\text{.}\text{we}\text{have:}\\ \frac{\text{1}}{\text{u}}\text{>}\frac{\text{1}}{\text{v}}\\ \therefore \text{v > u}\\ \text{Magnification}\text{is}\text{given}\text{as:}\\ \text{m =}\frac{\text{v}}{\text{u}}\\ \text{Since}\text{v > u}\\ \therefore \text{Magnification}\text{is}\text{positive}\text{and}\text{the}\text{enlarged}\text{image}\text{is}\\ \text{formed}\text{.}\\ \therefore \text{When}\text{an}\text{object}\text{is}\text{placed}\text{between}\text{the}\text{pole}\text{and}\text{focus}\\ \text{of}\text{the}\text{concave}\text{mirror,}\text{the}\text{virtual}\text{and}\text{enlarged}\text{image}\\ \text{is}\text{formed}\text{.}\end{array}

Q.16 A small pin fixed on a table top is viewed from above from a distance of 50 cm. By what distance would the pin appear to be raised if it is viewed from the same point through a 15 cm thick glass slab held parallel to the table? Refractive index of glass = 1.5. Does the answer depend on the location of the slab?

Ans.

Here, actual depth of pin,

d = 15 cm

Refractive index of glass,

μ =1.5

Lat apparent depth of pin=d’

The refractive index of glass is given as the ratio of actual depth to the apparent depth.

\begin{array}{l}\text{Refractive}\text{index}\text{of}\text{glass,}\text{μ =}\frac{\text{Real}\text{depth}}{\text{Apparent}\text{depth}}\\ \therefore \text{μ =}\frac{\text{d}}{\text{d’}}\\ \therefore \text{d’ =}\frac{\text{d}}{\text{μ}}\\ =\frac{15\text{cm}}{1.5}=10cm\\ \therefore \text{Distance through which the pin appears to be raised}\\ \text{= Real}\text{depth – Apparent}\text{depth = 15 cm – 10 cm}\\ \text{= 5}\text{cm}\end{array}

Q.17 (a) Figure 9.32 shows a cross-section of a ‘light pipe’ made of a glass fibre of refractive index 1.68. The outer covering of the pipe is made of a material of refractive index 1.44. What is the range of the angles of the incident rays with the axis of the pipe for which total reflections inside the pipe take place, as shown in the figure

(b) What is the answer if there is no outer covering of the pipe?

Ans.

(a) Refractive index of the glass fibre, μ₁ =1.68
Refractive index of the material of outer covering, μ₂ = 1.44
Refractive index of the interface of the inner and outer core of the pipe is given as:

$\begin{array}{l}\text{μ =}\frac{{\text{μ}}_{\text{2}}}{{\text{μ}}_{\text{1}}}\text{=}\frac{\text{1}}{{\text{sini}}_{\text{c}}}\\ {\text{Here,\hspace{0.33em}i}}_{\text{c}}\text{= Critical\hspace{0.33em}angle}\\ \therefore {\text{sin i}}_{\text{c}}\text{=}\frac{{\text{μ}}_{\text{1}}}{{\text{μ}}_{\text{2}}}\\ \text{=}\frac{\text{1.44}}{\text{1.68}}\text{= 0.8571}\\ \therefore {\text{i}}_{\text{c}}{\text{= sin}}^{\text{-1}}\left(\text{0.8571}\right){\text{= 59}}^{\text{o}}\\ \text{Total\hspace{0.33em}internal\hspace{0.33em}reflection\hspace{0.33em}takes\hspace{0.33em}place\hspace{0.33em}only\hspace{0.33em}when,}\\ \text{Angle\hspace{0.33em}of\hspace{0.33em}incidence},\mathrm{i}>{\mathrm{i}}_{\mathrm{c}}\\ {\text{i.e.,\hspace{0.33em}i>59}}^{\text{o}}\\ \text{The\hspace{0.33em}maximum\hspace{0.33em}value\hspace{0.33em}of\hspace{0.33em}angle\hspace{0.33em}of\hspace{0.33em}reflection\hspace{0.33em}is\hspace{0.33em}given\hspace{0.33em}as:}\\ {\text{\hspace{0.33em}r}}_{\text{max}}{\text{=90}}^{\text{o}}{\text{-59}}^{\text{o}}{\text{=31}}^{\text{o}}\\ \text{From\hspace{0.33em}Snell’s\hspace{0.33em}law,\hspace{0.33em}we\hspace{0.33em}obtain:}\\ {\text{μ}}_{\text{1}}\text{=}\frac{{\text{sin\hspace{0.33em}i}}_{\text{max}}}{{\text{sinr}}_{\text{max}}}\\ \therefore {\text{sin\hspace{0.33em}i}}_{\text{max}}{\text{= μ}}_{\text{1}}{\text{sin r}}_{\text{max}}\\ {\text{=1.68 × sin31}}^{\text{o}}\\ \text{= 0.8662}\\ \therefore {\text{\hspace{0.33em}i}}_{\text{max}}{\text{= sin}}^{\text{-1}}\left(\text{0.8662}\right){\text{= 60}}^{\text{o}}\\ \therefore {\text{Range\hspace{0.33em}of\hspace{0.33em}angles\hspace{0.33em}of\hspace{0.33em}incident\hspace{0.33em}rays\hspace{0.33em}with\hspace{0.33em}the\hspace{0.33em}axis\hspace{0.33em}of\hspace{0.33em}pipe£60}}^{\text{o}}\\ \text{The\hspace{0.33em}lower\hspace{0.33em}limit\hspace{0.33em}of\hspace{0.33em}angle\hspace{0.33em}of\hspace{0.33em}incidence\hspace{0.33em}is\hspace{0.33em}decided\hspace{0.33em}by\hspace{0.33em}the\hspace{0.33em}ratio}\\ \text{of\hspace{0.33em}diameter\hspace{0.33em}to\hspace{0.33em}length\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}pipe.}\\ \text{(b)\hspace{0.33em}If\hspace{0.33em}there\hspace{0.33em}is\hspace{0.33em}no\hspace{0.33em}outer\hspace{0.33em}covering\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}pipe:}\\ {\text{Refractive\hspace{0.33em}index\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}outer\hspace{0.33em}core\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}pipe,\hspace{0.33em}μ}}_{\text{1}}\text{= 1}\\ {\text{Refractive\hspace{0.33em}index\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}inner\hspace{0.33em}core\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}pipe,\hspace{0.33em}μ}}_{\text{2}}\text{= 1.68}\\ \text{From\hspace{0.33em}Snell’s\hspace{0.33em}law,\hspace{0.33em}we\hspace{0.33em}obtain:}\\ \text{μ =}\frac{{\text{μ}}_{\text{2}}}{{\text{μ}}_{\text{1}}}\\ \text{=}\frac{\text{1}}{{\text{sini}}_{\mathrm{c}}\text{‘}}\\ \therefore {\text{sini}}_{\mathrm{c}}\text{‘=}\frac{{\text{μ}}_{\text{1}}}{{\text{μ}}_{\text{2}}}\\ \text{=}\frac{\text{1}}{\text{1.68}}\\ \text{=0.5952}\\ \therefore {\mathrm{i}}_{\mathrm{c}}‘={\sin }^{-1}\left(0.5952\right)\\ =36{.5}^{\mathrm{o}}\\ \text{Here,\hspace{0.33em}for\hspace{0.33em}angle\hspace{0.33em}of\hspace{0.33em}incidence},\mathrm{i}={90}^{\mathrm{o}}\\ \text{We\hspace{0.33em}obtain,\hspace{0.33em}angle\hspace{0.33em}of\hspace{0.33em}reflection,\hspace{0.33em}}\mathrm{r}=36{.5}^{\mathrm{o}}\\ \therefore \mathrm{i}‘={90}^{\mathrm{o}}-\mathrm{r}\\ ={90}^{\mathrm{o}}-36{.5}^{\mathrm{o}}\\ =53{.5}^{\mathrm{o}}\\ \text{Since\hspace{0.33em}the\hspace{0.33em}value\hspace{0.33em}of\hspace{0.33em}}\mathrm{i}‘>{\mathrm{i}}_{\mathrm{c}}‘\\ \therefore \text{All\hspace{0.33em}the\hspace{0.33em}rays\hspace{0.33em}of\hspace{0.33em}light\hspace{0.33em}incident\hspace{0.33em}in\hspace{0.33em}the\hspace{0.33em}range\hspace{0.33em}}\le {90}^{\mathrm{o}}\text{\hspace{0.33em}will\hspace{0.33em}}\\ \text{undergo\hspace{0.33em}total\hspace{0.33em}internal\hspace{0.33em}reflection.}\end{array}$

Q.18 Answer the following questions:

(a) You have learnt that plane and convex mirrors produce virtual images of objects. Can they produce real images under some circumstances? Explain.
(b) A virtual image, we always say, cannot be caught on a screen. Yet when we ‘see’ a virtual image, we are obviously bringing it on to the ‘screen’ (i.e., the retina) of our eye. Is there a contradiction?
(c) A diver under water, looks obliquely at a fisherman standing on the bank of a lake. Would the fisherman look taller or shorter to the diver than what he actually is?
(d) Does the apparent depth of a tank of water change if viewed obliquely? If so, does the apparent depth increase or decrease?
(e) The refractive index of diamond is much greater than that of ordinary glass. Is this fact of some use to a diamond cutter?

Ans.

(a) Yes, plane and convex mirrors can produce real images if the object is virtual. For example: If the rays of light converging at a point behind the mirror are reflected to a point on the screen in front of the mirror. In this way, a real image is formed on the screen.

(b) No, there is not any contradiction. Since our eye lens is a double convex lens, it produces real and inverted images of the objects on the retina of the eye. In human eye, the virtual image acts as the object for the eye lens to produce the real image on the retina.

(c) Since the diver is under water and the fisherman is in the air, the light travels from the denser medium to the rarer medium. Therefore, it bends away from the normal and the fisherman looks taller to the diver.

(d) Yes, the apparent depth of tank of water will decrease further, when viewed obliquely as compared to the depth when seen normally. This is because, the direction of light changes when it travels from one medium to another.

(e) Since the refractive index of diamond is much greater as compared to that of an ordinary glass, the critical angle for diamond is much smaller as compared to that of an ordinary glass. Therefore, a skilled diamond cutter will put to use a large range of angles of incidence (less than critical angle) of light to ensure that the light entering the diamond undergoes multiple total internal reflections inside the diamond.

Q.19 The image of a small electric bulb fixed on the wall of a room is to be obtained on the opposite wall 3 m away by means of a large convex lens. What is the maximum possible focal length of the lens required for the purpose?

Ans.

Here, distance between the object and the image, s = 3 m

Let maximum focal length of the convex lens = f_max

For real image on the wall, the maximum focal length is given as:

\begin{array}{l}{\text{f}}_{\text{max}}\text{=}\frac{\text{s}}{\text{4}}\\ \text{=}\frac{\text{3 m}}{\text{4}}\\ \text{= 0}\text{.75}\text{m}\\ \text{Therefore, the maximum focal length of the lens required for this purpose = 0}\text{.75 m}\end{array}

Q.20 A screen is placed 90 cm from an object. The image of the object on the screen is formed by a convex lens at two different locations separated by 20 cm. Determine the focal length of the lens.

Ans.

Distance between object and the screen, D = 90 cm

Separation between two locations of the convex lens, d = 20 cm

Let focal length of the lens = f

The relation connecting focal length to d and D is given as:

\begin{array}{l}\text{f =}\frac{{\text{D}}^{\text{2}}{\text{– d}}^{\text{2}}}{\text{4D}}\\ \text{=}\frac{{\left(\text{90 cm}\right)}^{\text{2}}\text{–}{\left(\text{20 cm}\right)}^{\text{2}}}{\text{4×90 cm}}\\ \text{=}\frac{\text{770 cm}}{\text{36}}\\ \text{= 21}\text{.39}\text{cm}\\ \text{Therefore, focal length of the convex lens = 21}\text{.39 cm}\end{array}

Q.21 (a) Determine the ‘effective focal length’ of the combination of the two lenses in Exercise 9.10, if they are placed 8.0 cm apart with their principal axes coincident. Does the answer depend on which side of the combination a beam of parallel light is incident? Is the notion of effective focal length of this system useful at all?
(b) An object 1.5 cm in size is placed on the side of the convex lens. The distance between the object and the convex lens is 40 cm. Determine the magnification produced by the two-lens system, and the size of the image.

Ans.

Here, focal length of the convex lens, f₁ = 30 cm
Focal length of the concave lens, f₂ = −20 cm
Distance between the two lenses, d = 8.0 cm

(a) When the parallel beam of light is incident on the convex lens first:
For convex lens:
Here, object distance, u₁= ∞
Let image distance=v₁
From the lens formula, we have:

$\begin{array}{l}\frac{1}{{\mathrm{v}}_1}–\frac{1}{{\mathrm{u}}_1}=\frac{1}{{\mathrm{f}}_1}\\ \frac{1}{{\mathrm{v}}_1}=\frac{1}{{\mathrm{f}}_1}–\frac{1}{{\mathrm{u}}_1}\\ =\frac{1}{30}–\frac{1}{\mathrm{\infty }}\\ \therefore {\mathrm{v}}_1=30\mathrm{cm}\\ \text{For concave lens:}\\ \text{In this case, the image will act as a virtual object.}\\ {\text{Here, object distance, u}}_{\text{2}}\text{=}\left(\text{30 – d}\right)\text{=30 – 8=22 cm}\\ {\text{Let image distance=v}}_{\text{2}}\\ \text{From lens formula for the concave lens, we obtain:}\\ \frac{\text{1}}{{\text{v}}_{\text{2}}}\text{–}\frac{\text{1}}{{\text{u}}_{\text{2}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{2}}}\\ \therefore \frac{\text{1}}{{\text{v}}_{\text{2}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{2}}}\text{–}\frac{\text{1}}{{\text{u}}_{\text{2}}}\\ \text{=}\frac{\text{1}}{\text{22 cm}}\text{–}\frac{\text{1}}{\text{20 cm}}\text{=}\frac{\text{10 – 11}}{\text{220 cm}}\\ \therefore {\text{v}}_{\text{2}}\text{= -220\hspace{0.33em}cm}\\ \text{Therefore, the parallel incident beam appears to diverge from a point that is}\left(\text{220-4}\right)\text{216 cm from}\\ \text{the centre of the system of the two lenses.}\\ \left(\text{ii}\right)\text{When the parallel beam of light is incident from the left on the concave lens first:}\\ \text{For concave lens:}\\ {\text{Here, object distance, u}}_{\text{2}}\text{=-}\mathrm{\infty }\\ {\text{Let image distance=v}}_{\text{2}}\\ \text{From the lens formula, we have:}\\ \frac{\text{1}}{{\text{v}}_{\text{2}}}\text{–}\frac{\text{1}}{{\text{u}}_{\text{2}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{2}}}\\ \therefore \frac{\text{1}}{{\text{v}}_{\text{2}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{2}}}\text{+}\frac{\text{1}}{{\text{u}}_{\text{2}}}\\ \text{=}\frac{\text{1}}{\text{-20 cm}}\text{–}\frac{\text{1}}{\text{–}\mathrm{\infty }}\text{=-}\frac{\text{1}}{\text{20 cm}}\\ \therefore {\text{v}}_{\text{2}}\text{= -20\hspace{0.33em}cm}\\ \text{For convex lens:}\\ {\text{Here, object distance, u}}_{\text{1}}\text{=-}\left(\text{20 cm + 8 cm}\right)\text{= -28 cm}\\ {\text{Let image distance = v}}_{\text{2}}\\ \text{From lens formula for the convex lens, we obtain:}\\ \frac{\text{1}}{{\text{v}}_{\text{1}}}\text{–}\frac{\text{1}}{{\text{u}}_{\text{1}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{1}}}\\ \therefore \frac{\text{1}}{{\text{v}}_{\text{1}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{1}}}\text{+}\frac{\text{1}}{{\text{u}}_{\text{1}}}\\ \text{=}\frac{\text{1}}{\text{30 cm}}\text{+}\frac{\text{1}}{\text{-28 cm}}\\ \text{=}\frac{\text{14-15}}{\text{420 cm}}\text{=-}\frac{\text{1}}{\text{420 cm}}\\ \therefore {\text{v}}_{\text{2}}\text{= -420\hspace{0.33em}cm}\\ \text{Therefore, the parallel beam of incident light appears to diverge from a point 420-4=416 cm}\\ \text{from the centre of the two lens system.}\\ \left(\text{b}\right){\text{Given, height of the object, h}}_{\text{1}}\text{= 1.5 cm}\\ {\text{Object distance for convex lens, u}}_{\text{1}}\text{=- 40 cm}\\ \text{From the lens formula, we obtain:}\\ \frac{\text{1}}{{\text{v}}_{\text{1}}}\text{–}\frac{\text{1}}{{\text{u}}_{\text{1}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{1}}}\\ \therefore \frac{\text{1}}{{\text{v}}_{\text{1}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{1}}}\text{+}\frac{\text{1}}{{\text{u}}_{\text{1}}}\\ \text{=}\frac{\text{1}}{\text{30 cm}}\text{–}\frac{\text{1}}{\text{40 cm}}\text{=}\frac{\text{4-3}}{\text{120}}\\ \text{=}\frac{\text{1}}{\text{120}}\\ \therefore {\text{v}}_{\text{1}}\text{=120\hspace{0.33em}cm}\\ \text{Magnitude\hspace{0.33em}of\hspace{0.33em}magnification\hspace{0.33em}produced\hspace{0.33em}by\hspace{0.33em}convex\hspace{0.33em}lens\hspace{0.33em}is\hspace{0.33em}}\\ \text{given\hspace{0.33em}as:}\\ {\text{m}}_{\text{1}}\text{=}\frac{{\text{v}}_{\text{1}}}{\left|{\text{u}}_{\text{1}}\right|}\text{=}\frac{\text{120 cm}}{\text{40 cm}}\text{= 3}\\ \text{Therefore, the magnitude of magnification produced by convex lens = 3}\\ \text{The image formed by the convex lens acts as an object for the concave lens.}\\ \text{For concave lens:}\\ \text{Object distance,}\\ {\text{u}}_{\text{2}}\text{=120 cm – 8 cm = 112 cm}\\ \text{From the lens formula,}\\ \text{we obtain:}\\ \frac{\text{1}}{{\text{v}}_{\text{2}}}\text{–}\frac{\text{1}}{{\text{u}}_{\text{2}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{2}}}\\ \therefore \frac{\text{1}}{{\text{v}}_{\text{2}}}\text{=}\frac{\text{1}}{{\text{f}}_{\text{2}}}\text{+}\frac{\text{1}}{{\text{u}}_{\text{2}}}\\ \text{=}\frac{\text{1}}{\text{-20 cm}}\text{+}\frac{\text{1}}{\text{112 cm}}\\ \text{=}\frac{\text{-112+20}}{\text{2240 cm}}\\ \text{=}\frac{\text{-92}}{\text{2240 cm}}\\ \therefore {\text{v}}_{\text{2}}\text{=}\frac{\text{-2240}}{\text{92}}\text{\hspace{0.33em}cm}\\ \text{Magnitude\hspace{0.33em}of\hspace{0.33em}magnification\hspace{0.33em}produced\hspace{0.33em}by\hspace{0.33em}concave\hspace{0.33em}lens\hspace{0.33em}is\hspace{0.33em}}\\ \text{given\hspace{0.33em}as:}\\ {\text{m}}_2\text{=}\left|\frac{{\text{v}}_2}{{\text{u}}_2}\right|\\ \text{=}\frac{\text{2240}}{\text{92}}\text{×}\frac{\text{1}}{\text{112}}\text{=}\frac{\text{20}}{\text{92}}\\ {\text{Net\hspace{0.33em}magnification\hspace{0.33em}of\hspace{0.33em}the\hspace{0.33em}lens\hspace{0.33em}combination,\hspace{0.33em}m=m}}_{\text{1}}{\text{×m}}_{\text{2}}\\ \text{=3×}\frac{\text{20}}{\text{92}}\text{=0.652}\\ \therefore {\text{Height\hspace{0.33em}of\hspace{0.33em}image,\hspace{0.33em}h}}_{\text{2}}{\text{= emh}}_{\text{1}}\\ \text{= 0.652×1.5 = 0.98\hspace{0.33em}cm}\end{array}$

Q.22 At what angle should a ray of light be incident on the face of a prism of refracting angle 60° so that it just suffers total internal reflection at the other face? The refractive index of the material of the prism is 1.524.

Ans.

The given figure shows the incident, refracted and emergent rays associated with the glass prism ABC.

Here, angle of prism, A = 60°

Refractive index of the prism, μ = 1.524

As shown in the given figure, a ray of light is incident at the face AB of the prism, gets refracted and strikes the face AC of the prism. Here, i₁ and r₁ represent the angle of incidence and refraction at AB respectively. r₂ and e represent angle of incidence and angle of emergence at face AC respectively.

As per Snell’s law, we have:

\begin{array}{l}\frac{\sin e}{\sin r_2}=\mu \\ \therefore \sin r_2=\frac{\sin e}{\mu }\\ \text{For total internal reflection at face AC}:\\ \text{e}=\text{9}{0}^{\text{o}}\\ \therefore \sin r_2=\frac{\sin {90}^o}{\mu }\\ =\frac{\sin {90}^o}{1.524}\\ =\frac{1}{1.524}\\ =0.6562\\ \therefore r_2={\sin }^{-1}\left(0.6562\right)\approx {41}^o\\ \text{Since}\text{angle}\text{of}\text{prism}\text{is}\text{given}\text{as}:\\ A=r_1+r_2\\ \therefore r_1=A-r_2\\ ={60}^{\text{o}}-{41}^o\\ ={19}^o\\ \text{For}\text{face}AB:\\ \text{From}\text{Snell’s}\text{law,}\text{we}\text{have}:\\ \mu =\frac{\sin i_1}{\sin r_1}\\ \therefore \sin i_1=\mu \sin r_1\\ =1.524\times \sin {19}^o\\ =0.496\\ \therefore i_1={\sin }^{-1}\left(0.496\right)\\ ={29.75}^o\\ \therefore \text{Angle}\text{of}\text{incidence}={29.75}^o\end{array}