CBSE 12th Physics 2017 Guess Paper By 4ono 12th Physics 2017 Guess Paper By 4ono.com ... This is...

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Perfect solution to all problems Tips, Tricks, General Knowledge, Current Affairs, Latest Sample, Previous Year, Practice Papers with solutions. CBSE 12 th Physics 2017 Guess Paper By 4ono.com Download for Other Subjects: http://www.4ono.com/cbse-12th-science-sample-papers/ Note This pdf file is downloaded from www.4ono.com. Editing the content or publicizing this on any blog or website without the written permission of Rewire Media is punishable, the suffering will be decided under DMC

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Perfect solution to all problems

Tips, Tricks, General Knowledge, Current Affairs, Latest Sample, Previous Year, Practice Papers with solutions.

CBSE 12th Physics 2017 Guess Paper

By 4ono.com

Download for Other Subjects:

http://www.4ono.com/cbse-12th-science-sample-papers/

Note This pdf file is downloaded from www.4ono.com. Editing the content or publicizing this on any blog

or website without the written permission of Rewire Media is punishable, the suffering will be decided under DMC

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CBSE 12th Physics 2017 Guess Paper By 4ono.com

TIME - 3HR. | QUESTIONS - 26

THE MARKS ARE MENTIONED ON EACH QUESTION _________________________________________________________________________

SECTION โ€“ A

Q.1. Magnetic field lines can be entirely confined within the core of a toroid, but not within a straight solenoid. Why? 1 mark

Ans. Since, the magnetic field induction outside the toroid is zero.

Q.2. A plot of magnetic flux (๐“) versus current (I) is shown in the figure for two inductors A and B. Which of the two has larger value of

self-inductance? 1 mark

Ans. Since ๐œ™ = LI โ‡’ L = ๐œ™

1 = slope of ๐œ™ โˆ’ I graph โˆด slope of inductor A = slope of

inductor B. Hence the inductor A has larger value of self-inductance.

Q.3. Show graphically, the variation of the de-Broglie wavelength (ฮป) with the potential (V) through which an electron is accelerated from rest. 1 mark

Ans.

Q.4. A 10 V battery of negligible internal resistance is connected across a 200 V battery and a resistance of 38 ฮฉ as shown in the figure. Find the value of the current in circuit. 1 mark

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Ans. Since, the positive terminal of the batteries are connected together, so the equivalent emf of the batteries is given by

= 200 -10 = 190v.

Hence, the current in the circuit is given by ๐ผ =ฮต

๐‘….

๐ผ =190

38= 5๐ด

Q.5. Define electric dipole moment. Write its S.I. unit. 1 mark

Ans. Electric dipole moment: Dipole moment ( ) is a measure of strength of electric dipole. It is a vector quantity whose magnitude is equal to product of the magnitude of either charge and the distance between them. Si unit of dipole moment is coulomb-meter (cm).

SECTION - B

Q.6. How does the resistivity of a conductor depend upon temperature electrical conductivity? 2 marks

Ans. (i) The resistivity of a conductor increases with increase with increase in temperature

โˆด ๐œŒ๐‘‡ = ๐œŒ0[1 + ๐›ผ(๐‘‡ โˆ’ ๐‘‡0)]

(ii) The resistivity of a conductor is the reciprocal of electrical conductivity

โˆด ๐œŒ =1

๐œŽ

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Q.7. In the meter bridge experiment, balance point was observed at J with

AJ = l. 2 mark

(i) The values of R and X were doubled and then interchanged. What would be the new position of balance point?

(ii) If the galvanometer and battery are interchanged at the balance position, how will the balance point get affected? 2 mark

Ans. (i) the value of R and X were doubled and then interchanged. Hence the new position of balance point will 100 โˆ’ ๐ผ.

(ii) ๐ด๐ฝ = ๐‘™.

From the principle of Wheat Stones Bridge,

๐‘…

๐‘‹=

๐‘™

100 โˆ’ ๐‘™

๐‘‹ = ๐‘… (100 โˆ’ ๐‘™

๐‘™)

Hence, the galvanometer and tell are interchanged, the condition for a balance bridge is still satisfied. Therefore, the galvanometer will not show any deflection.

Q. 8. State Kirchhoff's rules. Explain briefly how these rules are justified. 2 marks

(a) Kirchhoffโ€™s First law:

Ans. Junction rule: The algebraic sum of all the emf meeting at a point in an electrical circuit is always zero.Let the currents be ๐ผ1, ๐ผ2, ๐ผ3 ๐‘Ž๐‘›๐‘‘ ๐ผ4

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Convention: Current towards the junction is always positive, while current away from the junction is negative

๐ผ3 + (โˆ’๐ผ1) + (โˆ’๐ผ2) + (โˆ’๐ผ) = 0

Kirchhoffโ€™s Second law: Loop rule

In a closed loop, the algebraic sum of the emfโ€™s is equal to the algebraic sum of the products of the resistance and current flowing through them.

For closed part BACB, ๐ธ1 โˆ’ ๐ธ2 = ๐ผ1๐‘…1 + ๐ผ2๐‘…2 โˆ’ ๐ผ3๐‘…3

For closed part CADC, ๐ธ2 = ๐ผ3๐‘…3 + ๐ผ4๐‘…4 + ๐ผ5๐‘…5

Demonstration:

Wheatstone Bridge: - The Wheatstone Bridge is an arrangement pf four resistance as shown in the following figure.

๐‘…1, ๐‘…2, ๐‘…3 ๐‘Ž๐‘›๐‘‘ ๐‘…4 are the four resistances.

Galvanometer(a) has a current ๐ผ๐‘”flowing through it at

balanced condition ๐ผ๐‘” = 0

Applying junction rule at B,

โˆด ๐ผ2 = ๐ผ4

Applying junction rule at D,

โˆด ๐ผ1 = ๐ผ3

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Applying loop rule to closed loop ADBA,

โˆ’๐‘…1 + ๐‘‚ + ๐ผ1๐‘…2 = 0

โˆด ๐ผ1๐ผ2

=๐‘…2

๐‘…1โ€ฆ(๐‘–)

Applying loop rule to closed loop CBDC,

๐‘…1๐‘…1 + ๐‘‚ โˆ’ ๐‘…1๐‘…1 = ๐‘‚ [๐ผ3 = ๐ผ1, ๐ผ4 = ๐ผ2]

โˆด ๐‘…2

๐‘…1=

๐‘…4

๐‘…3โ€ฆ(๐‘–๐‘–)

From Eq. (i) and (ii)

๐‘…2

๐‘…1=

๐‘…4

๐‘…3

This is the required balanced condition of wheatstone bridge.

Q.9. Plot a graph showing the variation of stopping potential with the frequency of incident radiation for two different photosensitive materials having work functions ๐‘พ๐Ÿ and (๐‘พ๐Ÿ > ๐‘พ๐Ÿ). On what factors does the (i) slope and (ii) intercept of the lines depend? 2 mark

Ans. The graph showing the variation of stopping potential (๐‘‰0) with the frequency of incident radiation (๐‘ฃ0) for two different photosensitive materials having work functions W1 and W2(W1>W2) is shown in fig.

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(i) Slope of the line = โˆ†V

โˆ†๐‘ฃ =

โ„Ž

๐‘’

[โˆด ๐‘’โˆ†V = h โˆ†๐‘ฃ] โˆด Slope of the line depends on the Planckโ€™s constant h and the electronic charge ๐‘’.

(ii) Intercept of graph A on the potential axis

=work function(W)

๐‘’= โˆ’

โ„Ž๐‘ฃ0

๐‘’

โˆด Intercept of the line depends upon Planckโ€™s constant h, threshold frequency (๐‘‰0) and the electronic charge (e).

Q.10. Using Rutherfordโ€™s model of the atom, derive the expression for the total energy of the electron in hydrogen atom. What is the significance of total negative energy possessed by the electron? 2 mark

Ans. From Rutherfordโ€™s model of the atom, the magnitude of this force is

๐น =1

4 ๐œ‹๐œ–0 .2๐‘’. (๐‘๐‘’)

๐‘Ÿ2

For hydrogen atom, Let, ๐น๐‘ โˆ’Centripetal force required to keep a revolving electron in orbit. Fe-Electrostatic force of attraction between the revolving electron and the nucleus. Then, for a dynamically stable orbit in hydrogen atom, where Z = 1

๐น๐‘ = ๐น๐‘’

๐‘š๐‘ฃ2

๐‘Ÿ=

(๐‘’)(๐‘’)

4๐œ‹๐œ€0๐‘Ÿ2 โ€ฆ (๐‘–)

๐‘Ÿ =๐‘’

4๐œ‹๐œ€0๐‘š๐‘ฃ2 โ€ฆ (๐‘–๐‘–)

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K.E. of electron in the orbit,

K =1

2๐‘š๐‘ฃ2,

Form equation (๐‘–),

K =๐‘’2

8๐œ‹๐œ€0๐‘Ÿ

Potential energy of electron in

Orbit, U = (๐’†)(๐’†)

4๐œ‹๐œ€0๐‘Ÿ=

โˆ’๐‘’2

4๐œ‹๐œ€0๐‘Ÿ

โˆด Total energy of electron in hydrogen atom

E = k + U = ๐‘’2

8๐œ‹๐œ€0๐‘Ÿโˆ’

๐‘’2

4๐œ‹๐œ€0๐‘Ÿ; E = โˆ’

๐‘’2

8๐œ‹๐œ€0๐‘Ÿ

Here, negative sign indicates that the revolving electron is bound to the positive nucleus.

OR

Using Bohrโ€™s postulates of the atomic model, derive the expression for radius of

nth electron orbit, thus obtaining the expression for Bohrโ€™s radius.

Ans. Form de-Broglie hypothesis, wavelength associated with electron

๐œ† =โ„Ž

๐‘š๐‘ฃ

๐‘š๐‘ฃ =โ„Ž

๐œ†

Substituting this value in ๐‘š๐‘ฃ๐‘Ÿ = ๐‘›h

2๐œ‹,

we get, โ„Ž

๐œ† ๐‘Ÿ = ๐‘›

h

2๐œ‹

2๐œ‹ ๐‘Ÿ = ๐‘›๐œ†

๐‘–. ๐‘’., circurmference (๐‘† = 2๐œ‹๐‘Ÿ) of nth permitted orbit for the electron can contains exactly ๐‘› wavelength of de-Broglie wavelength associated with electron in that orbit.

SECTION - C

Q.11. A convex lens made up of glass of refractive index 1ยท5 is dipped, in turn, in (i) a medium of refractive index 1ยท65, (ii) a medium of refractive index 1ยท33.

(a) Will it behave as a converging or a diverging lens in the two cases?

(b) How will its focal length change in the two media? 3 marks

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Ans. Here,

๐œ‡๐‘” = 1.5๐‘Ž

Let ๐‘“๐‘Ž๐‘–๐‘Ÿ be the focal length of the lens in air, Then, 1

๐‘“๐‘Ž๐‘–๐‘Ÿ( ๐œ‡๐‘”

๐‘Ž โˆ’ 1) (1

๐‘…1โˆ’

1

๐‘…2)

or (1

๐‘…1โˆ’

1

๐‘…2) =

1

๐น๐‘Ž๐‘–๐‘Ÿ( ๐œ‡๐‘”๐‘Ž โˆ’1)

=1

๐‘“๐‘Ž๐‘–๐‘Ÿ(1.5โˆ’1)

Or (1

๐‘…1โˆ’

1

๐‘…2) =

1

๐น๐‘Ž๐‘–๐‘Ÿ โ€ฆ. (i)

(i) When lens is dipped in medium A Here, ( ๐œ‡๐‘Ž

๐‘Ž = 1.65)

Let ๐น๐ด be the focal length of the lens, when dipped in medium A. Then,

1

๐น๐ด( ๐œ‡๐‘”

๐‘Ž โˆ’ 1) (1

๐‘…1โˆ’

1

๐‘…2)

= ( ๐œ‡๐‘”

๐‘Ž

๐œ‡๐‘Ž๐‘Ž โˆ’ 1)(

1

๐‘…1โˆ’

1

๐‘…2)

using the equation (i), we have

1

๐‘“๐ด= (

1.5

1.65โˆ’ 1)ร—

1

๐‘“๐‘Ž๐‘–๐‘Ÿ= โˆ’

1

5.5๐‘“๐‘Ž๐‘–๐‘Ÿ

As the sign of ๐‘“๐ดis opposite to that of ๐‘“๐‘Ž๐‘–๐‘Ÿ the lens will behave as a diverging lens.

(ii) When lens is dipped in medium B:

Here, ๐œ‡๐‘”๐‘Ž = 1.33

Let ๐น๐ตbe the focal length of the lens, when dipped in medium B. Then,

1

๐น๐ต( ๐œ‡๐‘” โˆ’ 1๐ต ) (

1

๐‘…1โˆ’

1

๐‘…2) = (

๐œ‡๐‘”๐‘Ž

๐œ‡๐‘๐‘Ž โˆ’ 1)(

1

๐‘…1โˆ’

1

๐‘…2)

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Using the equation (i), we have

1

๐น๐ต= (

1.5

1.33โˆ’ 1)ร—

2

๐‘“๐‘Ž๐‘–๐‘Ÿ=

0.34

1.33๐‘“๐‘Ž๐‘–๐‘Ÿ

Or ๐‘“๐ต = 3.91 ๐‘“๐‘Ž๐‘–๐‘Ÿ

As the sign of ๐‘“๐ตis same as that of ๐‘“๐‘Ž๐‘–๐‘Ÿ the lens will behave as a converging lens.

Q.12. (a) The energy levels of an atom are as shown below. Which of them will result in the transition of a photon of wavelength 275 nm? 3 marks

(b) Which transition corresponds to emission of radiation of maximum wavelength?

Ans. (a) For element A

Ground state energy, ๐ธ1 = โˆ’2๐‘’๐‘‰

Exicted state energy, ๐ธ2 = 0 ๐‘’๐‘‰

Energy of photon emitted, E = ๐ธ2 โˆ’ ๐ธ1

= 0 โˆ’ (โˆ’2) = 2๐‘’๐‘‰

โˆด Wavelength of photon emitted,

๐œ† =โ„Ž๐‘

๐ธ=

6.626ร—10โˆ’34ร—3ร—108

2ร—1.6ร—10โˆ’19=

19.878ร—108

3.2

6.211ร—10โˆ’7๐‘š = ๐Ÿ”๐Ÿ๐Ÿ. ๐Ÿ๐ง๐ฆ

For element B

๐ธ๐Ÿ = โˆ’4.5 ๐‘’ ๐‘‰, ๐ธ2 = 0๐‘’ ๐‘‰

๐ธ = 0 โˆ’ (โˆ’4.5) = 4.5 ๐‘’ ๐‘‰

โˆด ๐œ† =6.626ร—10โˆ’34ร—3ร—108

4.5ร—1.6ร—10โˆ’19

19.878ร—10โˆ’7

7.2= 2.760ร—10โˆ’7 = ๐Ÿ๐Ÿ•๐Ÿ” ๐ง๐ฆ

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For element C

๐ธ๐Ÿ = โˆ’4.5 ๐‘’ ๐‘‰, ๐ธ2 = โˆ’2๐‘’ ๐‘‰

๐ธ = โˆ’2 โˆ’ (โˆ’4.5) = โˆ’2 + 4.5 = 2.5 ๐‘’๐‘‰

โˆด ๐œ† =6.626ร—10โˆ’34ร—3ร—108

2.5ร—1.6ร—10โˆ’19

19.878ร—10โˆ’7

4= 4.969ร—10โˆ’7๐‘š = ๐Ÿ’๐Ÿ—๐Ÿ”. ๐Ÿ— ๐ง๐ฆ

For element D

๐ธ๐Ÿ = โˆ’10 ๐‘’ ๐‘‰, ๐ธ2 = โˆ’2๐‘’ ๐‘‰

๐ธ = โˆ’2 โˆ’ (โˆ’10) = 8 ๐‘’๐‘‰

โˆด ๐œ† =6.626ร—10โˆ’34ร—3ร—108

8ร—1.6ร—10โˆ’19

=19.878ร—10โˆ’7

12.8= 1.552ร—10โˆ’7๐‘š = ๐Ÿ๐Ÿ“๐Ÿ“. ๐Ÿ ๐ง๐ฆ

โˆด Element B has a proton of wavelength ๐Ÿ๐Ÿ•๐Ÿ“ ๐ง๐ฆ

(b) Element A has radiation of maximum wavelength 621nm

Q.13. An air solenoid of length 0.3m, area of cross section is 1.2 x ๐Ÿ๐ŸŽโˆ’๐Ÿ‘๐’Ž๐Ÿand has 2500 turns. Around its central section, a coil of 350 turns is wound. The solenoid and the coil are electrically insulated from each other. Calculate the emf induced in the coil if the initial current of 3A in the solenoid is reversed in 0.25s. 3 marks

Ans. N1 = 2500

N2 = 350

A = 1.2 ร—10โˆ’3๐‘š2

l = 0.3m.

dl = 3-(-3) = 3+3 = 6A

dt = 0.25s

Since Mutual inductance,

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๐‘€ = ๐œ‡0๐‘1๐‘2๐ด

๐‘™=

4๐œ‹ร—10โˆ’7ร—2500ร—350ร—1.2ร—10โˆ’3

0.3

=4ร—3.14ร—1.05ร—10โˆ’4

0.3= 43.96ร—10โˆ’4 = 4.39ร—10โˆ’3H

Induced ๐‘’๐‘š๐‘“|E| = MdI

dt

=4.39ร—10โˆ’3ร—6

0.25= 105.36ร—10โˆ’3 = 0.10536 V.

Q.14. Draw a labelled ray diagram of a refracting telescope. Define its magnifying power write the expression for it. Write two important limitations of a refracting telescope over reflecting type

telescope. 3 marks

Ans. Refracting telescope:

Magnifying power- The magnifying power is in the ratio of the angle โˆ subtended at the eye by the final image to the angle ๐›ฝ which the object subtends at the lens or the eye.

๐‘š โ‰ˆ๐›ฝ

โˆโ‰ˆ

โ„Ž

๐‘“๐‘’.๐‘“0โ„Ž

=๐‘“0๐‘“๐‘’

Limitations of refracting telescope over the reflecting type telescope โ€“

(i) Refracting telescope suffers from chromatic aberration as it uses large sized lenses.

(ii) The requirements of big lenses tend to be very heavy and therefore difficult to make and support by their edges.

Q.15. In a Geiger-Marsden experiment, calculate the distance of closet approach to the nucleus of ๐’ = ๐Ÿ–๐ŸŽ, when an ๐œถ-particle of 8 MeV energy impinges on it before it comes momentarily to rest and reverses its direction. How will the distance of closet approach be affected when the kinetic energy of the ๐œถ-particle is doubled? 3 marks

Ans. Z=80, KE=8MeV.

Potential energy =๐พ๐‘๐‘’2

๐‘‘0=

1

2 ๐‘š1๐‘ฃ0

2

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๐‘‘0 =๐พ๐‘๐‘’2

(๐‘€2๐‘‰0

2

2)

=9 ร— 109 ร— 80 ร— (1.6ร— 1019)2

8 ร— 1.6 ร— 10โˆ’13

[โˆต 1๐‘€๐‘’๐‘‰ = 1.6ร—10โˆ’13๐ฝ]

=18 ร— 18 ร— 109 ร— 1.6 ร— 1010

8 ร— 106= 128.8 ๐‘“๐‘š

Since ๐‘‘0๐›ผ1

๐ธ๐‘˜

So, when kinetic energy is doubled the distance of closet to halved. If, the kinetic energy is doubled the distance of ๐›ผ- particles is halved.

OR

The ground state energy of hydrogen atom is -13.6 eV. If an electron makes a transition form an energy level -0.85 eV to -3.4eV, calculate the wavelength of the spectral line emitted. To which series of hydrogen spectrum does this wavelength belong?

Ans. ๐ธ๐‘› = โˆ’13.6

๐‘›2 ๐‘’๐‘ฃ. Here ground state energy for ๐‘ = 1, ๐ธ1 = โˆ’13.6 ๐‘’๐‘‰

Now electron transits form ๐ธ๐‘ž = โˆ’0.85๐‘’๐‘‰ ๐‘ก๐‘œ ๐ธ๐‘ž = โˆ’3.4๐‘’๐‘‰

โˆ’0.85 =โˆ’13.6

๐‘›๐‘2

๐‘›๐‘2 =

13.6

0.85= 16

Thus,

๐‘›๐‘ = 4

Again, โˆ’3.4 = 13.6/๐‘›๐‘ž2

๐‘›๐‘ž2 =

13.6

3.4= 4

๐‘›๐‘ž = 2

Thus electron makes transition from n = 4 to n = 2. Hence, it is blamer series. Now

๐‘… = 1.0974 ร— 107

1

๐œ†= ๐‘… (

1

22โˆ’

1

๐‘›2)

1

๐œ†= 1.0974ร— 107

(1

22โˆ’

1

42) =

1.09ร—107ร—12

4ร—16

1

2

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1

๐œ†= 0.2057 ร— 107

๐œ† = 4.861 ร— 107

๐œ† = 4861

intensity of light after passing through second polarizer ๐‘ƒ2 is given by ๐ผ = ๐ผ0 ๐‘๐‘œ๐‘ 2๐œƒ .

Q.16. An illuminated object and a screen are placed 90cm apart. Determine the focal length and nature of the lens required to produce a clear image on the screen, twice the size of the object. 3 marks

Ans.

m =๐‘ฃ

๐‘ขโ‡’ 2 =

๐‘ฃ

๐‘ขโ‡’ ๐‘ฃ = 2๐‘ข โ€ฆ . . (๐‘–๐‘–)

Putting the value of v in (i), we get

u + 2u = 90 โ‡’ ๐‘ข =90

30= 30

โˆด ๐‘ฃ = 2ร—30 = 60

Using lens formula, we get

1

๐‘“=

1

๐‘ฃโˆ’

1

๐‘ขโ‡’

1

๐‘“=

1

60โˆ’

1

โˆ’30

โ‡’1

๐‘“=

1

60+

1

30โ‡’

1

๐‘“=

1 + 2

60=

3

60

โ‡’ ๐‘“ =60

3โˆด ๐‘“ = 20 cm.

Q. 17. (a) In what way is diffraction from each slit related to the interference pattern in a double slit experiment?

(b) Two wavelength of sodium light 590 nm and 596 nm are used, in turn, to study the diffraction taking place at a single slit of aperture ๐Ÿร—๐Ÿ๐ŸŽโˆ’๐Ÿ’๐’Ž.The distance between the slit and the screen is 1.5.m. Calculate the separation between the positions of the first maxima of the diffraction pattern obtained in the two cases. 3marks

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Ans.(a). If the width of each slit is comparable to the wavelength of light used, the interference pattern thus obtained in the double-slit experiment is modified by diffraction from each of two slits.

(b). Given that: Wavelength of the light beam

๐œ†1 = 590๐‘›๐‘š = 5.9ร—10โˆ’7๐‘š

Wavelength of another light beam,

๐œ†2 = 596๐‘›๐‘š = 5.96ร—10โˆ’7๐‘š

Distance of the slits from the screen = D = 1.5m

Distance of the two slits = a = 2ร—10โˆ’4๐‘š

For the first secondary maxima

sin๐œƒ =3๐œ†1

2๐‘Ž=

๐‘ฅ1

๐ท

OR

๐‘ฅ1 =3๐œ†1๐ท

2๐‘Ž๐‘Ž๐‘›๐‘‘ ๐‘ฅ1 =

3๐œ†2๐ท

2๐‘Ž

โˆด Spacing between the positions of first secondary maxima of two sodium lines

๐‘ฅ1 โˆ’ ๐‘ฅ2 =3๐ท

2๐‘Ž(๐œ†1 โˆ’ ๐œ†2) = 6.75 ร—10โˆ’5๐‘š.

Q.18. (a) Draw a ray diagram showing the image formation by a compound microscope. Hence obtain expression for total magnification when the image is formed at infinity. 3 marks

Ans. (a)

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(b) Magnifying power: The linear magnification (๐‘š0) due to the objective is

๐‘š0 =๐ดโ€ฒ๐ตโ€ฒ

๐ด๐ต=

โ„Žโ€ฒ

โ„Žโ€ฆโ€ฆ(๐‘–)

Also tan๐›ฝ =โ„Ž

๐‘“0=

โ„Žโ€ฒ

๐ฟ

โˆด โ„Žโ€ฒ

โ„Ž=

๐ฟ

๐‘“0โ€ฆโ€ฆ . . (ii)

From (i) and (ii) we have

๐‘š0 =๐ฟ

๐‘“0โ€ฆโ€ฆ(๐‘–๐‘–๐‘–)

Where hโ€™ is the size of the first image, the object size being h and ๐‘“0 being the focal length of the objective and L be the distance between the second focal point of the objective and first focal point of the eye piece (focal length ๐‘“๐‘’) is called the tube length of compound microscope.

When the final image is formed at the near point, then the angular magnification (๐‘š๐‘’) of the eye piece is

๐‘š๐‘’ = (1 +๐‘‘

๐‘“๐‘’)โ€ฆโ€ฆ . (๐‘–๐‘ฃ)

โˆด Total magnification of compound microscope is

๐‘š๐‘’ = ๐‘š0. ๐‘š๐‘’

๐‘š =1

๐‘“0+ (1 +

๐ท

๐‘“๐‘’)

OR

(a) State Huygensโ€™s principle. Using this principle draw a diagram to show how a

plane wave front incident at the interface of the two media gets refracted when it propagates from a rarer to a denser medium. Hence verify Snellโ€™s law of

refraction. (b) When monochromatic light travels from a rarer to a denser medium, explain the following, giving reasons: (i) Is the frequency of reflected and reflected light same as the frequency of incident light? (ii) Does the decrease in speed imply a reduction in the energy carried by light wave?

Ans.(a) Huygensโ€™s Principle: It is based on the assumptions:

(i) Each point on the primary wave front acts as a source of secondary wavelets, sending out disturbance in all directions in a similar manner as the original source of light does.

(ii) The new position of the wave front at any instant is the envelope of the secondary wavelets at that instant

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Refraction on the basis of wave theory:

(i) Consider any point Q on the incident wave front. (ii) Suppose when disturbance from point P on incident wave front reaches point

pโ€™ on the refracting surface XY. (iii) Since, Pโ€™Aโ€™ represents the refracted wave front, the time taken by light to

travel from a point on incident wave front to the corresponding point on refracted wave front should always be the same. Now, time taken by light to go from Q to Qโ€™ will be

๐‘ก =๐‘„๐พ

๐‘+

๐พ๐‘„โ€ฒ

๐‘ฃ โ€ฆ . . (๐‘–)

In right angled โˆ†๐ด๐‘„๐พ,< ๐‘„๐ด๐พ = ๐‘–

โˆด ๐‘„๐พ = ๐ด๐พ sin ๐‘– ---(ii)

in right- =angled โˆ†๐‘ƒโ€ฒ๐‘„โ€ฒ๐พ,< ๐‘„โ€ฒ๐‘ƒโ€ฒ๐พ = ๐‘Ÿ ๐‘Ž๐‘›๐‘‘ ๐พ๐‘„โ€ฒ = ๐พ๐‘ƒโ€ฒ sin ๐‘Ÿ. ---(iii)

Substituting (ii) and (iii) in equation (i)

We get

๐‘ก =๐ด๐พ sin ๐‘–

๐‘+

๐พ๐‘ƒโ€ฒ sin ๐‘Ÿ

๐‘ฃ

or,

๐‘ก =๐ด๐พ sin ๐‘–

๐‘+

(๐ด๐‘ƒโ€ฒ โˆ’ ๐ด๐พ) sin ๐‘Ÿ

๐‘ฃ(KPโ€™ = APโ€™ โˆ’ AK)

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or,

๐‘ก =๐ด๐‘ƒโ€ฒ

๐‘sin ๐‘Ÿ + ๐ด๐พ (

sin ๐‘–

๐‘โˆ’

sin ๐‘Ÿ

๐‘ฃ)โ€ฆ . (๐‘–๐‘ฃ)

The rays from different point on the incident wave front will take the same time to reach the corresponding points on the refracted wave from i.e., t given by equation

(iv) is independent of AK. It will happen so,

If

sin ๐‘–

๐‘โˆ’

sin ๐‘Ÿ

๐‘ฃ= 0

sin ๐‘–

sin ๐‘Ÿ=

๐‘

๐‘ฃ= ๐œ‡ =

sin ๐‘–

sin ๐‘Ÿ

This is the Snellโ€™s law for refraction of light.

(b)(i). The frequency of refracted light remains same as the frequency of incident light frequency only depends on the source of light.

(ii) Since, the frequency remains same, hence there is no reduction in energy.

Q.19. State the law of radioactive decay. Plot a graph showing the number (N) of undecided nuclei as a function of time (t) for a given radioactive sample having half life ๐‘ปยฝ. Depict in the plot the number of undecided nuclei at (i) t = 3 ๐‘ปยฝ and (ii) t = 5 ๐‘ปยฝ. 3 mark Ans. Radioactive decay Law: The number of atoms disintegrated per second at any instant is directly Proportional to the number of radioactive atoms actually present at that time. The following graph showing the number (N) of Undecided nuclei as a function of time (t) for a given radioactive sample having half-life. And undecided nuclei at (i) t = 2 ๐‘‡1/2 (ii) t = 4 ๐‘‡1/2 included also,

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Q.20. Three light rays red (R), green (G) and blue (B) are incident on a right angled prism 'abc' at face 'ab'. The refractive indices of the material of the prism for red, green and blue wavelengths are 1.39, 1.44 and 1.47 respectively. Out of the three which color ray will emerge out of face 'ac' ? Justify your answer. Trace the path of these rays after passing through face 'ab'. 3 marks

Ans. The red light ray (R) will emerge out of face ac. The path of green (G) and blue (B) light rays will be as,

Q.21. (a) Why photoelectric effect cannot be explained on the basis of wave nature of light? Give reasons.

(b) write the basis features of photon picture of electromagnetic radiation on which Einsteinโ€™s photoelectric equation is based. 3 marks

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Ans. (a) Wave nature of radiation cannot explain the following:

(i) The instantaneous ejection of photoelectrons. (ii) The existence of threshold frequency for a metal surface (iii) The fact that kinetic energy of the emitted electrons is independent of the intensity of

light and depends upon its frequency. Thus, the photoelectric effect cannot be explained on the basis of wave

nature of light.

(b) Photon picture of electromagnetic radiation on which Einsteinโ€™s photoelectric equation is based on particle nature of light. Its basic features are:

(i) In interaction with matter, radiation behaves as if it is made up of particles called photons.

(ii) Each photon has energy E = hv and momentum ๐‘ =โ„Ž๐‘ฃ

๐‘ and speed C, the speed of

light. (iii) All photons of light a particular frequency v, or wavelength ๐œ† have the same energy

๐ธ = โ„Ž๐‘ฃ =โ„Ž๐‘ฃ

๐‘ and momentum ๐‘ =

โ„Ž๐‘ฃ

๐‘=

โ„Ž

๐œ†whatever the intensity of radiation may be.

(iv) By increasing the intensity of light of given wavelength, there is only an increase in the number of photons per second crossing a given area, with each photon having the same energy. Thus photon energy is independent of intensity of radiation.

Photons are electrically neutral and are not deflected by electric and magnetic fields.

Q.22. You are given three lenses ๐‘ณ๐Ÿ, ๐‘ณ๐Ÿ and ๐‘ณ๐Ÿ‘each of focal length 20 cm. An object is kept at 40 cm in front of ๐‘ณ๐Ÿ, as shown. The final real image is formed at the focus โ€˜Iโ€™ of ๐‘ณ๐Ÿ‘. Find the separations between ๐‘ณ๐Ÿ, ๐‘ณ๐Ÿ ๐’‚๐’๐’… ๐‘ณ๐Ÿ‘. 3 marks

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Ans.

1

๐‘ฃ1โˆ’

1

๐‘ข=

1

๐‘“1

1

๐‘ฃ1=

1

๐‘“1+

1

๐‘ข1

1

20+

1

โˆ’40=

1 โˆ’ 2 โˆ’ 7

โˆ’40

1

40

๐‘ฃ1 = 40๐‘๐‘š.

Here, image by ๐ฟ3 is formed at focus. So the object should lie at infinity for ๐ฟ3. Hence. ๐ฟ2 will produce image at infinity. So we can conclude that object for ๐ฟ2 should be at its focus.

But, we have seen above that image by ๐ฟ1 is formed at 40 right of ๐ฟ1which is at 20 cm left of ๐ฟ2 focus of ๐ฟ2.

So ๐‘‹1= distance between ๐ฟ1 and ๐ฟ2 = (40 + 20) cm = 60 cm

Again distance between ๐ฟ2 and ๐ฟ3 does not matter as the image by ๐ฟ2 is formed at infinity so ๐‘‹2 can take any value.

SECTION - D

Q.23. With the help of a suitable ray diagram, derive the mirror formula for a concave mirror. 4 marks

Ans. Mirror Formula for Concave Mirror:

Let, AB be the length of an object placed beyond C in front of a concave mirror. The image Aโ€™Bโ€™ is real, inverted and between C and F.

Applying sign conventions, we have

Object distance PB = โˆ’๐‘ข image distance PBโ€™ = โˆ’๐‘ฃ focal length PF = โˆ’๐‘“ and radius of curvature PC = โˆ’2๐‘“

In similar โˆ†s ABC and Aโ€ฒBโ€ฒF

๐ด๐ต

๐ดโ€ฒ๐ตโ€ฒ=

๐ต๐ถ

๐ตโ€ฒ๐ถ โ€ฆ (๐‘–)

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and similar โˆ†s RSF and Aโ€ฒBโ€ฒF

๐‘…๐‘†

๐ดโ€ฒ๐ตโ€ฒ=

๐‘†๐น

๐ตโ€ฒ๐น

โˆต ๐‘…๐‘† = ๐ด๐ต

๐ด๐ต

๐ดโ€ฒ๐ตโ€ฒ=

๐‘†๐น

๐ตโ€ฒ๐น โ€ฆ (๐‘–๐‘–)

From eq. (i) and (ii), we have

๐ต๐ถ

๐ตโ€ฒ๐ถ=

๐‘†๐น

๐ตโ€ฒ๐น

Since, the aperture of the concave mirror is small so the point S and P coincides.

โˆด๐ต๐ถ

๐ตโ€ฒ๐ถ=

๐‘ƒ๐น

๐ตโ€ฒ๐น

๐‘ƒ๐ต โˆ’ ๐‘ƒ๐ถ

๐‘ƒ๐ถ โˆ’ ๐‘ƒ๐ตโ€ฒ=

๐‘ƒ๐น

๐‘ƒ๐ตโ€ฒ โˆ’ ๐‘ƒ๐น

โˆ’๐‘ข + 2๐‘“

โˆ’2๐‘“ + ๐‘ฃ=

โˆ’๐‘“

โˆ’๐‘ฃ + ๐‘“

๐‘ข๐‘ฃ โˆ’ ๐‘ข๐‘“ โˆ’ 2๐‘ฃ๐‘“ + 2๐‘“2 = 2๐‘“2 โˆ’ ๐‘“๐‘ฃ

โ‡’ ๐‘ข๐‘ฃ = ๐‘ข๐‘“ + ๐‘ฃ๐‘“

Dividing both side by ๐‘ข๐‘ฃ๐‘“, we get

๐‘ข๐‘ฃ

๐‘ข๐‘ฃ๐‘“=

๐‘ข๐‘“

๐‘ข๐‘ฃ๐‘“+

๐‘ฃ๐‘“

๐‘ข๐‘ฃ๐‘“

โˆด1

๐‘“=

1

๐‘ฃ+

1

๐‘ข

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SECTION โ€“ E

Q.24. (a) for a ray of light travelling from a denser medium of refractive index ๐’๐Ÿto a rarer medium of refractive index ๐’๐Ÿ, prove that

๐’๐Ÿ

๐’๐Ÿ= sin ๐’Š๐’„ ,

where ๐’Š๐’„is the critical angle of incidence for the media.

(b) Explain with the help of a diagram. how the above principle is used for transmission of video signals using optical fibers? 5 marks

Ans.(a) Relation between refractive index and critical angle: Let O be a point object in the denser medium of refractive index (๐‘›1). A ray incident along OA1 deviates away from normal and is refracted along A1 B1in the rarer medium of refractive index (๐‘›2). It increases with increase in the angle of incidence: For particular value of i = C, the critical angle, the incident ray OA2 is refracted at < r = 90ยฐ and goes along A2 B2.

Applying Snellโ€™s Law at A2

n1 ๐‘ ๐‘–๐‘› ic = n2 sin 900 โ‡’n1 ๐‘ ๐‘–๐‘› ic = n2ร—1

โˆด ๐‘ ๐‘–๐‘› ic =n2

n1 ๐‘œ๐‘Ÿ

n2

n1= ๐‘ ๐‘–๐‘› ic

(b) Optical Fiber: Optical fiber make use the phenomenon of total internal reflection. Optical fibers consist of many long high quality composite glass or quartz fibers. Each fiber consists of a core and cladding. The refractive index of the material of the core is higher than that of the cladding.

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Propagation of light through an optical fiber: When light is incident at one end of the fiber at a small angle, it suffers several total internal reflection at the glass boundary because the angle of incidence is greater than the critical angle. The intensity of the out coming beam is almost equal to that of the incident beam.

OR

(a) What is plane polarized light? Two polaroidโ€™s are placed at ๐Ÿ—๐ŸŽ๐ŸŽ to each other

and the transmitted intensity is zero. What happens when one more polaroid is placed between these two bisecting the angle between them? how will the intensity of transmitted light vary on further rotting the polaroid?

(b) If a light beam shows no intensity variation when transmitted. Through a polaroid which is rotated, does it mean that the light is un โ€“ polarized? explain briefly.

Ans.(a) Plane polarized light: When polarized, light is passed through a tourmaline crystal cut with its face parallel to its crystallographic axis AB. Only those vibrations of light pass through the crystal, which are parallel to AB, all other vibrations are absorbed. The emerged light from the Crystal is said to be plane polarized light. If E is the amplitude of electric field component emanating-from 1st polaroid, then from 2nd polaroid at 45ยฐ.The amplitude of

electric field component is E1 = E cos 45ยฐ = E ร—1

โˆš2ร—

E

โˆš2

Again amplitude of electric field component coming from 3rd polaroid at 45ยฐ to 2nd polaroid would be

E2 = E1 cos 45ยฐ =

E

โˆš2.1

โˆš2=

E

2

= Half of E

As Intensity ๐›ผE2

โˆด Intensity transmitted from three polaroidโ€™s will be 1

4th of the intensity

transmitted from the first polaroid. (b) No, The light which is made up of electric field components Ex, Ey with 90ยฐ phase difference but equal amplitudes. The tip of electric vector executes uniform circular motion at the frequency of the light itself.

When such light is passed through a polaroid, which is rotated, the transmitted average intensity remains constant.

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Q.25. An a.c. source generating a voltage ๐’— = ๐’—๐’Ž ๐ฌ๐ข๐ง๐Ž๐’• is connected capacitor of capacitance C. find the expression for the current, i , through it. Plot a graph of v and i versus t to show that the current is ๐…/๐Ÿ ahead of the voltage. A resistor of 200 ๐›€ and a capacitor of ๐Ÿ๐Ÿ“. ๐ŸŽ ๐๐‘ญ Fare connected in series to a 220 V, 50 Hz a.c. source. Calculate the current in the circuit and the rms voltage across the resistor and the capacitor. Is the algebraic sum of these voltages more than the source voltage? if yes, resolve the paradox. 5 marks

Ans. A.C source containing capacitor: Let a source of alternating ๐‘’๐‘š๐‘“. ๐‘‰ = ๐‘‰๐‘š sin๐œ”๐‘ก be connected to a capacitor of capacitance C only

๐‘‰ = ๐‘‰๐‘š sin๐œ”๐‘ก โ€ฆ (๐‘–)

At every instant, the potential V is given by

๐‘‰ =๐‘ž

๐ถ โ‡’ ๐‘‰๐‘š

sin๐œ”๐‘ก =๐‘ž

๐‘ โˆด ๐‘ž = ๐ถ ๐‘‰๐‘š sin๐œ”๐‘ก.

If I is instantaneous value of current in the circuit at instant t, then

๐‘– =๐‘‘๐‘ž

๐‘‘๐‘ก=

๐‘‘

๐‘‘๐‘ก (๐ถ ๐‘‰๐‘š sin๐œ”๐‘ก)

๐‘– = ๐‘ ๐‘‰๐‘š(cos๐œ”๐‘ก). ๐œ” =

1๐‘š1๐œ”๐‘

sin (๐œ”๐‘ก +๐œ‹

2)

The current will be maximum. When (sin๐œ”๐‘ก +๐œ‹

2) = 1

โˆด ๐‘–๐‘š =๐‘‰๐‘š1

๐œ”๐‘

ร— 1 = ๐‘‰๐‘š1

๐œ”๐‘

๐‘– = ๐‘–๐‘š sin (๐œ”๐‘ก +๐œ‹

2)

Therefore, alternating current I lead the alternating voltage by a phase angle of ๐œ‹

2.

Numerical: Here R = 200 ฮฉ

๐ถ = 15.0 ๐œ‡๐น = 15 ร— 10โˆ’6๐น, ๐‘‰๐‘Ÿ๐‘š๐‘  = 220 ๐‘‰,

๐œ = 50 ๐ป๐‘ง

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๐ผ๐‘Ÿ๐‘š๐‘  =?

๐‘‹๐‘ =1

๐œ”๐‘=

1

2๐œ‹๐œ๐‘

=1

2 ร—227

ร— 50 ร— 15 ร— 10โˆ’6

=7 ร— 106

33000

= 212.12 โ‰ˆ 212 ฮฉ

โˆด ๐‘ = โˆš๐‘…2 + โˆš๐‘‹๐‘2 = โˆš(200)2 + (212)2

= โˆš40000 + 44944

= โˆš84944

= 291.45 ฮฉ

โˆด ๐ผ๐‘Ÿ๐‘š๐‘  =๐‘‰๐‘Ÿ๐‘š๐‘ 

๐‘=

220

291.45

= 0.75 ๐ด

โˆด ๐‘‰๐‘… = ๐‘‰๐‘Ÿ๐‘š๐‘  ๐‘… = 0.75ร—200

= 125 ๐‘‰

๐‘‰๐‘ = ๐ผ๐‘Ÿ๐‘š๐‘ . ๐‘‹๐‘

= 0.75 ร— 212 = 159 ๐‘‰

โˆด ๐‘‰๐‘… + ๐‘‰๐ถ = 150 + 159 = 309

โˆด ๐‘‰๐‘… + ๐‘‰๐ถ > ๐‘‰

This is because these voltages are not in same phase and they cannot be added like ordinary numbers.

โˆด ๐‘‰ = โˆš๐‘‰๐‘…2 + ๐‘‰๐ถ

2

= โˆš(150)2 + (159)2

= โˆš47781

= 218.18 ๐‘‰.

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Q.26. State Faradayโ€™s law of electromagnetic induction. Figure shows a rectangular conductor PORS in which the conductor PQ is free to move in a uniform magnetic field B perpendicular to the plane of the paper. The field extends from x=0 to x=b and is zero for x>b. Assume that only the arm PQ possesses resistance r, when the arm PQ is pulled outward from x=0 with constant speed v, absinthe expressions for the flux and the induced emf. Sketch the variations of these quantities with distance 0 x 2b. 5 marks

Ans. Part I: Faradayโ€™s law of induction: It states that the emf induced in a coil of N turns is directly related to the rate of change of flux through it.

โˆด ๐œ€ = โˆ’๐‘๐‘‘โˆ…๐ต

๐‘‘๐‘ก

Where โˆ…๐ต is the flux linked with one turn of the coil? If the circuit is closed, a

current I =๐œ€

๐‘… is set up in it.

Part II: refer to following fig (a). the arm PQ of the rectangular conductor is moved from x = 0, outwards. The uniform magnetic field is perpendicular to the plane and extends from x = 0 to x = b and zero the situation when the arm PQ possesses substantial resistance r. Consider the situation when the arm PQ is pulled outwards from x = 0 to x = 2b, and is then moved back to x = 0 with constant speed v. obtain expressions for the flux, the induced emf, the force necessary to pull the arm and the power dissipated as joule heat. Sketch the variation of these quantities with distance.

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Let us first consider the forward motion from ๐‘ฅ = 0 to x = 2b the flux โˆ…๐‘ linked with the circuit SPQR is

โˆ…๐‘ = ๐ต๐‘™๐‘ฅ 0 โ‰ค ๐‘ฅ < ๐‘

= Blb b โ‰ค ๐‘ฅ < 2๐‘

The induced emf is,

๐œ€ = โˆ’๐‘‘โˆ…๐‘

๐‘‘๐‘ก= โˆ’๐ต๐‘™๐‘ฃ ; 0 โ‰ค ๐‘ฅ < ๐‘ = 0 ; ๐‘ โ‰ค< 2๐‘

When the induced emf is non-zero, the current I is (in magnitude)

I =๐ต๐‘™๐‘ฃ

๐‘Ÿ

The force required to keep the arm PQ in constant motion is IlB. Its direction is to the left. In magnitude

F =๐ต2๐‘™2๐‘ฃ

๐‘Ÿ= 0 ; 0 โ‰ค ๐‘ฅ < ๐‘ = 0 ; ๐‘ โ‰ค ๐‘ฅ < 2๐‘

The joule heating loss is

๐‘๐‘— = I2๐‘Ÿ

=๐ต2๐‘™2๐‘ฃ2

๐‘Ÿ 0 โ‰ค ๐‘ฅ < ๐‘

= 0 b โ‰ค ๐‘ฅ < 2

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OR

Draw a schematic diagram of a step-up transformer. Explain its working principle. Deduce the expression for the secondary to primary voltage in terms of the number of turns in the two coils. In an ideal transformer, how is this ratio related to the currents in the two coils?

How is the transformer used in large scale transmission and distribution of electrical energy over long distances?

Ans. Step up transformer: principle: It is a device which converts low voltage. A.C. into high voltage A. C. It is based upon the principle of mutual induction. When alternating current passed through a coil, an induced e. m. f. is set up in the neighboring coil.

Construction: A transformer consists of two coils of many turns of insulated copper wire wound on a closed laminated iron core. One of the coils known as primary (p) is connected to A.C. supply. The other coil known as secondary (s) is connected to the load.

Working: When an alternating current is passed through the primary, the magnetic flux through the iron core changes which does two things. It produces e. m. f in the primary and an induced e. m. f is also set up in the secondary, if we assume that the resistance of primary is negligible, the back e. m. f will be equal to the voltage applied to the primary.

โˆด ๐‘‰๐‘ = โˆ’๐‘๐‘

๐‘‘โˆ…

๐‘‘๐‘ก

and ๐‘‰๐‘  = โˆ’๐‘๐‘ 

๐‘‘โˆ…

๐‘‘๐‘ก

Where ๐‘๐‘and ๐‘๐‘  are number of terms in the primary and secondary respectively. V๐‘

and V๐‘  are their respective voltages.

๐‘‰๐‘ ๐‘‰๐‘

=N๐‘ 

N๐‘

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This ratio N๐‘ 

N๐‘ called the turms ratio.

In a step โˆ’ up transformer: N๐‘  > N๐‘

So ๐‘‰s > V๐‘

In a step โˆ’ down transformer: N๐‘  < N๐‘

So, V๐‘  > V๐‘

Large scale transmission: The large scale transmission and distribution of electrical energy over long distances is done with the use of transformers. The voltage output of the generator is stepped-upโ€”so that reduced and power loss I2R is cut down. It is then transmitted over long distances to an area sub- station near the consumers. There the voltage is stepped down. It is further stepped down. It is further stepped down at distributing sub-stations and utility poles before a power supply of 240 V reaches our homes.

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