AVS fiziks. Institute for NET/JRF, GATE, IIT-JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES

Similar documents
matschek (ccm2548) Ch17-h3 chiu (57890) 1

Physics 218, Spring March 2004

not to be republished NCERT ELECTROMAGNETIC WAVES Chapter Eight MCQ I

Laplace Potential Distribution and Earnshaw s Theorem

8.022 (E&M) Lecture 13. What we learned about magnetism so far

In electrostatics, the electric field E and its sources (charges) are related by Gauss s law: Surface

1 Fundamental Solutions to the Wave Equation

Electromagnetism. Christopher R Prior. ASTeC Intense Beams Group Rutherford Appleton Laboratory

1 Fundamental Solutions to the Wave Equation

Experiment 1 Electric field and electric potential

PHYS 110B - HW #7 Fall 2005, Solutions by David Pace Equations referenced as Eq. # are from Griffiths Problem statements are paraphrased

(conservation of momentum)

11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below.

Answers to Coursebook questions Chapter 2.11

E(r,t) = e 3. r 3. (b) Show that the transverse current, J t,is 3n(n e 3 ) e 3

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other

3/19/2018. PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105

[Griffiths Ch.1-3] 2008/11/18, 10:10am 12:00am, 1. (6%, 7%, 7%) Suppose the potential at the surface of a hollow hemisphere is specified, as shown

EM-2. 1 Coulomb s law, electric field, potential field, superposition q. Electric field of a point charge (1)

Extra Examples for Chapter 1

2. Electrostatics. 2.1 What is electrostatics and electrostatic induction? 2.2 Explain coulomb s law of electrostatics

06 - ROTATIONAL MOTION Page 1 ( Answers at the end of all questions )

Classical Approach to the Theory of Elementary Particles

Ion-sound waves (electrostatic low frequency waves)

Flux. Area Vector. Flux of Electric Field. Gauss s Law

Red Shift and Blue Shift: A realistic approach

Chapter 22: Electric Fields. 22-1: What is physics? General physics II (22102) Dr. Iyad SAADEDDIN. 22-2: The Electric Field (E)

Mass Transfer (Stoffaustausch)

SAMPLE LABORATORY SESSION FOR JAVA MODULE B. Calculations for Sample Cross-Section 2

Electric Anisotropy, Magnetic Anisotropy, Uniaxial and Biaxial Materials, Bianisotropic Media (Definitions)

INFN School on Electron Accelerators. Beam Acceleration Cavity Field and Concepts

Module 05: Gauss s s Law a

Electrostatics (Electric Charges and Field) #2 2010

Physics 2A Chapter 10 - Moment of Inertia Fall 2018

arxiv: v4 [physics.class-ph] 14 Jul 2018

MAGNETIC FIELD INTRODUCTION

ELECTROSTATICS::BHSEC MCQ 1. A. B. C. D.

Solutions. V in = ρ 0. r 2 + a r 2 + b, where a and b are constants. The potential at the center of the atom has to be finite, so a = 0. r 2 + b.

PHYS 2135 Exam I February 13, 2018

University of Illinois at Chicago Department of Physics. Electricity & Magnetism Qualifying Examination

POISSON S EQUATION 2 V 0

Correspondence Analysis & Related Methods

A moving charged particle creates a magnetic field vector at every point in space except at its position.

$ i. !((( dv vol. Physics 8.02 Quiz One Equations Fall q 1 q 2 r 2 C = 2 C! V 2 = Q 2 2C F = 4!" or. r ˆ = points from source q to observer

Fields and Waves I Spring 2005 Homework 8. Due: 3 May 2005

Electromagnetism Physics 15b

Magnetic Field. Conference 6. Physics 102 General Physics II

Welcome to Physics 272

Phys102 Second Major-182 Zero Version Monday, March 25, 2019 Page: 1

Objects usually are charged up through the transfer of electrons from one object to the other.

Waves and Polarization in General

Magnetic field due to a current loop.

16.1 Permanent magnets

COLLISIONLESS PLASMA PHYSICS TAKE-HOME EXAM

Investigation of Magnitude and Phase Errors in Waveguide Samples for the Nicolson-Ross-Weir Permittivity Technique

Today s Plan. Electric Dipoles. More on Gauss Law. Comment on PDF copies of Lectures. Final iclicker roll-call

Gauss Law. Physics 231 Lecture 2-1

CHAPTER 25 ELECTRIC POTENTIAL

ANTENNAS. Vector and Scalar Potentials. Maxwell's Equations. D = εe. For a linear, homogeneous, isotropic medium µ and ε are contant.

Photographing a time interval

3.6 Applied Optimization

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

A near-perfect invisibility cloak constructed with homogeneous materials

IMPLEMENTATION OF MUR S ABSORBING BOUNDARIES WITH PERIODIC STRUCTURES TO SPEED UP THE DESIGN PROCESS USING FINITE-DIFFERENCE TIME-DOMAIN METHOD

Black Body Radiation and Radiometric Parameters:

Lecture 04: HFK Propagation Physical Optics II (Optical Sciences 330) (Updated: Friday, April 29, 2005, 8:05 PM) W.J. Dallas

1 Spherical multipole moments

Gauss s Law Simulation Activities

SEE LAST PAGE FOR SOME POTENTIALLY USEFUL FORMULAE AND CONSTANTS

Reflectance spectra for Si

PHYS 1444 Lecture #5

( ) ( )( ) ˆ. Homework #8. Chapter 27 Magnetic Fields II.

7.2.1 Basic relations for Torsion of Circular Members

TUTORIAL 9. Static magnetic field

( ) Make-up Tests. From Last Time. Electric Field Flux. o The Electric Field Flux through a bit of area is

2 Parallel-Plate Transmission Line (Geometric Model) = c Assume it s a plane wave propagate in the z with polarization in y direction. d dz ~ ˆ.

Physics 181. Assignment 4

Circular Motion & Torque Test Review. The period is the amount of time it takes for an object to travel around a circular path once.

Physics C Rotational Motion Name: ANSWER KEY_ AP Review Packet

The geometric construction of Ewald sphere and Bragg condition:

Physics Spring 2012 Announcements: Mar 07, 2012

Qualifying Examination Electricity and Magnetism Solutions January 12, 2006

Fundamentals of Modern Optics Winter Term 2012/2013 Prof. Thomas Pertsch Abbe School of Photonics Friedrich-Schiller-Universität Jena

Photon, Charged Particle and Anti-charged Particle

Objectives: After finishing this unit you should be able to:

Physics 2212 GH Quiz #2 Solutions Spring 2016

Chapter 13 Gravitation

Circular Motion Problem Solving


Class XII - Physics Wave Optics Chapter-wise Problems. Chapter 10

DOING PHYSICS WITH MATLAB COMPUTATIONAL OPTICS

4. Electrodynamic fields

FARADAY'S LAW. dates : No. of lectures allocated. Actual No. of lectures 3 9/5/09-14 /5/09

Quiz 6--Work, Gravitation, Circular Motion, Torque. (60 pts available, 50 points possible)

F = net force on the system (newton) F,F and F. = different forces working. E = Electric field strength (volt / meter)

Math Section 4.2 Radians, Arc Length, and Area of a Sector

(Sample 3) Exam 1 - Physics Patel SPRING 1998 FORM CODE - A (solution key at end of exam)

University Physics (PHY 2326)

PHYS 1444 Section 501 Lecture #7

Review for Midterm-1

Transcription:

ELECTROMAGNETIC THEORY SOLUTIONS GATE- Q. An insulating sphee of adius a aies a hage density a os ; a. The leading ode tem fo the eleti field at a distane d, fa away fom the hage distibution, is popotional to (A) d - (B) d - (C) d - (D) d -4 Ans: (b) V d osd V, a zeo V E I st tem, d a os sinddd. Q. Two magneti dipoles of magnitude m eah ae plaed in a plane as shown The enegy of inteation is given by m (A) Zeo (B) 4d m (C) d Ans: (d) U 4 m m m m Sine m m m m, m (D) 8d U mos 45 mos 45 m U. 8 d 4d m o 45 d o 45 m fiziks, H.No., G.F, Jia Saai, Nea IIT, Hauz Khas, New Delhi-6 Phone: -6865455/+9-98745498 8-B/6, Jia Saai, Nea IIT Hauz Khas, New Delhi-6 Email: fiziks.physis@gmail.om

Statement fo Linked Answe Questions and 4: Conside the popagation of eletomagneti waves in a linea, homogenous and isotopi mateial medium with eleti pemittivity ε and magneti pemeability μ. Q. Fo a plane wave of angula fequeny ω and popagation veto k popagating in the medium Mawell s equations edue to (A) (B) (C) (D) k E ; k H ; k E H; k H E k E ; k H ; k E H; k H E k E ; k H ; k E H; k H E k E ; k H ; k E H; k H E Ans: (d) Q4. If ε and μ assume negative values in a etain fequeny ange, then the dietions of the popagation veto k and the Poynting veto S in that fequeny ange ae elated as (A) k and S ae paallel (B) k and S ae anti-paallel (C) k and S ae pependiula to eah othe (D) k and S makes an angle that depends on the magnitude of ε and μ fiziks, H.No., G.F, Jia Saai, Nea IIT, Hauz Khas, New Delhi-6 Phone: -6865455/+9-98745498 8-B/6, Jia Saai, Nea IIT Hauz Khas, New Delhi-6 Email: fiziks.physis@gmail.om

Q5. Conside a onduting loop of adius a and total loop esistane R plaed in a egion with a magneti field B theeby enlosing a flu. The loop is onneted to an eletoni iuit as shown, the apaito being initially unhaged C V out If the loop is pulled out of the egion of the magneti field at a onstant speed u, the final output voltage V out is independent of (A) (B) u (C) R (D) C fiziks, H.No., G.F, Jia Saai, Nea IIT, Hauz Khas, New Delhi-6 Phone: -6865455/+9-98745498 8-B/6, Jia Saai, Nea IIT Hauz Khas, New Delhi-6 Email: fiziks.physis@gmail.om

GATE- Q6. If a foe F is deivable fom a potential funtion V(), whee is the distane fom the oigin of the oodinate system, it follows that (A) F (B) F (C) V (D) V Q7. Tow hages q and q ae plaed along the -ais in font of a gounded, infinite onduting plane, as shown in the figue. They ae loated espetively at a distane of.5 m and.5 m fom the plane. The foe ating on the hage q is (A) 4 7q (B) 4 q.5m q q.5m (C) q 4 (D) 4 q Using method of Images we an daw equivalent figue as shown below: q q.5m.5m.5m q q.5m q q q q q 7q 7q F 4 8 4 Q8. A unifom sufae uent is flowing in the positive y-dietion ove an infinite sheet lying in -y plane. The dietion of the magneti field is (A) along î fo z > and along (B) along k fo z > and along (C) along (D) along î fo z < k fo z < î fo z > and along î fo z < k fo z > and along k fo z < fiziks, H.No., G.F, Jia Saai, Nea IIT, Hauz Khas, New Delhi-6 Phone: -6865455/+9-98745498 8-B/6, Jia Saai, Nea IIT Hauz Khas, New Delhi-6 Email: fiziks.physis@gmail.om 4

Q9. A magneti dipole of dipole moment m is plaed in a non-unifom magneti field B. If the position veto of the dipole is, the toque ating on the dipole about the oigin is (A) m B (B) m B (C) m B (D) m B m B Ans: () Q. A spheial onduto of adius a is plaed in a unifom eleti field E E k. The potential at a point P(, θ) fo > a, is given by Ea Φ(, θ) = onstant E os os whee is the distane of P fom the ente O of the sphee and θ is the angle OP makes with the z-ais P The hage density on the sphee at θ = o is (A) / (B) / E E (C) / (D)) / E E O k V a E Ea os os a. E os E os E os E os E Q. Whih of the following epessions fo a veto potential A DOES NOT epesent a unifom magneti field of magnitude B along the z-dietion? (A) A, B, (B) A B y,, B B y B (C) A,, (D) y B A,, Ans: () B A fiziks, H.No., G.F, Jia Saai, Nea IIT, Hauz Khas, New Delhi-6 Phone: -6865455/+9-98745498 8-B/6, Jia Saai, Nea IIT Hauz Khas, New Delhi-6 Email: fiziks.physis@gmail.om 5

Statement fo Linked Questions and : A plane eletomagneti wave has the magneti field given by whee k is the wave numbe and dietions espetively. B k, y, z, t B sin y t k i, j and k ae the Catesian unit vetos in, y and z Q. The eleti field E y, z, t, oesponding to the above wave is given by k (A) i j k B sin y t (B) i j B sin y t k (C) B sin y t i (D) B sin y t j E k k y y k B B sin E B sin y k k t y k tz k Q. The aveage Poynting veto is given by B i j (A) Ans: (d) B i j B i j (B) (C) B B y B S k y B i j (D) fiziks, H.No., G.F, Jia Saai, Nea IIT, Hauz Khas, New Delhi-6 Phone: -6865455/+9-98745498 8-B/6, Jia Saai, Nea IIT Hauz Khas, New Delhi-6 Email: fiziks.physis@gmail.om 6

GATE- Q4. The spae-time dependene of the eleti field of a linealy polaized light in fee spae is given by E os t kz whee E, ω and k ae the amplitude, the angula fequeny and the waveveto, espetively. The time aveage enegy density assoiated with the eleti field is (a) E (b) E () 4 E (d) E u E E E os 4 wt kz u E E Q5. A plane eletomagneti wave taveling in fee spae is inident nomally on a glass plate of efative inde /. If thee is no absoption by the glass, its efletivity is (a) 4% (b) 6% () % (d) 5% n n R n n / / 4 4 5.4 o 4% Q6. The eleti and the magneti field E z, t and B z, t, espetively oesponding to the sala potential z, t and veto potential Az, t i tz ae (a) E iz and B -ĵt (b) E iz and B ĵt () E iz and B -ĵt (d) E iz and B -ĵt Ans: (d) A A E iz, t t B A j t. fiziks, H.No., G.F, Jia Saai, Nea IIT, Hauz Khas, New Delhi-6 Phone: -6865455/+9-98745498 8-B/6, Jia Saai, Nea IIT Hauz Khas, New Delhi-6 Email: fiziks.physis@gmail.om 7

Q7. A plane polaized eletomagneti wave in fee spae at time t= is given E, y ep j i 6 8z B, z, t is given by by. The magneti field (a) B, z, t 6k 8 i ep i6 8z t (b) B, z, t 6k 8 i ep i6 8z t () B, z, t 6k 8 i ep i6 8z t (d) B, z, t 6k 8 i ep i6 8z t B B k i k k E E 8 6 ep j i k. t k 6k 8 i ep i6 8z t,. Q8. Two infinitely etended homogeneous isotopi dieleti media (medium-and medium- with dieleti onstant and 5, espetively) meet at the z = plane as shown in the figue. A unifom eleti field eists eveywhee. Fo z, the eleti field is given by E i j 5k. The intefae sepaating the two media is hage fee. The eleti displaement veto in the medium- is given by (a) D i j k 5 (b) D i j k 5 () D i j k 4 6 (d) D i j k 4 6 medium - medium - z = fiziks, H.No., G.F, Jia Saai, Nea IIT, Hauz Khas, New Delhi-6 Phone: -6865455/+9-98745498 8-B/6, Jia Saai, Nea IIT Hauz Khas, New Delhi-6 Email: fiziks.physis@gmail.om 8

Ans: (b) E E E i j 5 and f D D E E k k E 5 D 5 E i j k. i j k fiziks, H.No., G.F, Jia Saai, Nea IIT, Hauz Khas, New Delhi-6 Phone: -6865455/+9-98745498 8-B/6, Jia Saai, Nea IIT Hauz Khas, New Delhi-6 Email: fiziks.physis@gmail.om 9

GATE- Q9. At a sufae uent, whih one of the magnetostati bounday ondition is NOT CORRECT? (a) Nomal omponent of the magneti field is ontinuous. (b) Nomal omponent of the magneti veto potential is ontinuous. () Tangential omponent of the magneti veto potential is ontinuous. (d) Tangential omponent of the magneti veto potential is not ontinuous. Ans: (d) Q. Intefeene finges ae seen at an obsevation plane z, by the supeposition of two plane waves A i k ep t and A i k ep t, whee A and A ae eal amplitudes. The ondition fo intefeene maimum is (a) k k m (b) k k m () k k m (d) k k m Ans: (b) Q. Fo a sala funtion satisfying the Laplae equation, has (a) zeo ul and non-zeo divegene (b) non-zeo ul and zeo divegene () zeo ul and zeo divegene (d) non-zeo ul and non-zeo divegene Ans: (). and. fiziks, H.No., G.F, Jia Saai, Nea IIT, Hauz Khas, New Delhi-6 Phone: -6865455/+9-98745498 8-B/6, Jia Saai, Nea IIT Hauz Khas, New Delhi-6 Email: fiziks.physis@gmail.om

Q. A iulaly polaized monohomati plane wave is inident on a dieleti intefae at Bewaste angle. Whih one of the following statements is oet? (a) The efleted light is plane polaized in the plane of inidene and the tansmitted light is iulaly polaized. (b) The efleted light is plane polaized pependiula to the plane of inidene and the tansmitted light is plane polaized in the plane of inidene. () The efleted light is plane polaized pependiula to the plane of inidene and the tansmitted light is elliptially polaized. (d) Thee will be no efleted light and the tansmitted light is iulaly polaized. Ans: () Q. A hage distibution has the hage density given by Q Fo this hage distibution the eleti field at,, Q (a) 9 Q (b) 4 Q () 4 Ans: ' ' ' a a a Potential V d d d... 4 a a a Fist tem, total hage Q T d Q d Q d Q Q Seond tem, dipole moment p. Q (d) 6 d Q d Q d Q Q Q Q V 4 V E 4Q 4 4Q 4 Q 8 fiziks, H.No., G.F, Jia Saai, Nea IIT, Hauz Khas, New Delhi-6 Phone: -6865455/+9-98745498 8-B/6, Jia Saai, Nea IIT Hauz Khas, New Delhi-6 Email: fiziks.physis@gmail.om

Q4. A monohomati plane wave at oblique inidene undegoes efletion at a dieleti intefae. If k, k and n ae the unit vetos in the dietions of inident wave, i efleted wave and the nomal to the sufae espetively, whih one of the following epessions is oet? (a) k i k n (b) k i k n () k n k (d) k n k i Ans: () i Q5. In a onstant magneti field of.6 Tesla along the z dietion, find the value of the path integal A dl in the units of (Tesla m ) on a squae loop of side length / metes. The nomal to the loop makes an angle of figue. The answe should be up to two deimal plaes. 6 to the z-ais, as shown in the o 6 ẑ Ans: A dl S A. da B. da BA os 6.6.5T. m S fiziks, H.No., G.F, Jia Saai, Nea IIT, Hauz Khas, New Delhi-6 Phone: -6865455/+9-98745498 8-B/6, Jia Saai, Nea IIT Hauz Khas, New Delhi-6 Email: fiziks.physis@gmail.om