TEST-03 TOPIC: MAGNETISM AND MAGNETIC EFFECT OF CURRENT Q.1 Find the magnetic field intensity due to a thin wire carrying current I in the Fig.

Similar documents
Synopsis : 8. ELECTROMAGNETISM

24-2: Electric Potential Energy. 24-1: What is physics

ALL QUESTIONS ARE WORTH 20 POINTS. WORK OUT FIVE PROBLEMS.

Physics Exam II Chapters 25-29

Rotational Kinematics. Rigid Object about a Fixed Axis Western HS AP Physics 1

Dynamics of Rigid Bodies

COLLEGE OF FOUNDATION AND GENERAL STUDIES PUTRAJAYA CAMPUS FINAL EXAMINATION TRIMESTER /2017

Physics 11b Lecture #2. Electric Field Electric Flux Gauss s Law

Chapter 13 - Universal Gravitation

MAGNETIC FIELD INTRODUCTION

CSJM University Class: B.Sc.-II Sub:Physics Paper-II Title: Electromagnetics Unit-1: Electrostatics Lecture: 1 to 4

Physics 1501 Lecture 19

Physics Exam 3

PHYS Week 5. Reading Journals today from tables. WebAssign due Wed nite

Physics 207 Lecture 16

3.1 Electrostatic Potential Energy and Potential Difference

Description Linear Angular position x displacement x rate of change of position v x x v average rate of change of position

Physics NYB problem set 5 solution


Chapter 5 Circular Motion

21 MAGNETIC FORCES AND MAGNETIC FIELDS

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism

Rigid Bodies: Equivalent Systems of Forces

Physics 202, Lecture 2. Announcements

Physics 1: Mechanics

Engineering Mechanics. Force resultants, Torques, Scalar Products, Equivalent Force systems

Objectives. Chapter 6. Learning Outcome. Newton's Laws in Action. Reflection: Reflection: 6.2 Gravitational Field

Chapter 12 Equilibrium and Elasticity

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

PHY126 Summer Session I, 2008

iclicker Quiz a) True b) False Theoretical physics: the eternal quest for a missing minus sign and/or a factor of two. Which will be an issue today?

VEKTORANALYS FLUX INTEGRAL LINE INTEGRAL. and. Kursvecka 2. Kapitel 4 5. Sidor 29 50

Remember: When an object falls due to gravity its potential energy decreases.

Chapter 23: Electric Potential

PY208 Matter & Interactions Final Exam S2005

10/15/2013. PHY 113 C General Physics I 11 AM-12:15 PM MWF Olin 101

Physics Spring 2012 Announcements: Mar 07, 2012

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

Calculate the electric potential at B d2=4 m Calculate the electric potential at A d1=3 m 3 m 3 m

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

anubhavclasses.wordpress.com CBSE Solved Test Papers PHYSICS Class XII Chapter : Electrostatics

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

Module 18: Outline. Magnetic Dipoles Magnetic Torques

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

JURONG JUNIOR COLLEGE Physics Department Tutorial: Electric Fields (solutions)

Unit 6 Practice Test. Which vector diagram correctly shows the change in velocity Δv of the mass during this time? (1) (1) A. Energy KE.

Chapter Fifiteen. Surfaces Revisited

20-9 ELECTRIC FIELD LINES 20-9 ELECTRIC POTENTIAL. Answers to the Conceptual Questions. Chapter 20 Electricity 241

7/1/2008. Adhi Harmoko S. a c = v 2 /r. F c = m x a c = m x v 2 /r. Ontang Anting Moment of Inertia. Energy

Magnetic fields (origins) CHAPTER 27 SOURCES OF MAGNETIC FIELD. Permanent magnets. Electric currents. Magnetic field due to a moving charge.

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer.

ev dm e evd 2 m e 1 2 ev2 B) e 2 0 dm e D) m e

Electrostatics. 1. Show does the force between two point charges change if the dielectric constant of the medium in which they are kept increase?

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

Electrostatics. 3) positive object: lack of electrons negative object: excess of electrons

PHY 213. General Physics II Test 2.

16.1 Permanent magnets

One-dimensional kinematics

The Law of Biot-Savart & RHR P θ

Scalars and Vectors Scalar

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

6. CURRENT ELECTRICITY

Exam 3, vers Physics Spring, 2003

Electrostatics (Electric Charges and Field) #2 2010

Ch 30 - Sources of Magnetic Field! The Biot-Savart Law! = k m. r 2. Example 1! Example 2!

AP Physics Electric Potential Energy

Uniform Circular Motion

( )( )( ) ( ) + ( ) ( ) ( )

Capítulo. Three Dimensions

Unit 6 Practice Test. Which vector diagram correctly shows the change in velocity Δv of the mass during this time? (1) (1) A. Energy KE.

Field due to a collection of N discrete point charges: r is in the direction from

2/26/2014. Magnetism. Chapter 20 Topics. Magnets and Magnetic Fields. Magnets and Magnetic Fields. Magnets and Magnetic Fields

1. A body will remain in a state of rest, or of uniform motion in a straight line unless it

Chapter 4. Newton s Laws of Motion

a v2 r a' (4v) 2 16 v2 mg mg (2.4kg)(9.8m / s 2 ) 23.52N 23.52N N

Test 1 phy What mass of a material with density ρ is required to make a hollow spherical shell having inner radius r i and outer radius r o?

Electricity Revision ELECTRICITY REVISION KEY CONCEPTS TERMINOLOGY & DEFINITION. Physical Sciences X-Sheets

2/24/2014. The point mass. Impulse for a single collision The impulse of a force is a vector. The Center of Mass. System of particles

Chapter 23: GAUSS LAW 343

Algebra-based Physics II

(a) Calculate the apparent weight of the student in the first part of the journey while accelerating downwards at 2.35 m s 2.

MTE2 Wed 26, at 5:30-7:00 pm Ch2103 and SH 180. Contents of MTE2. Study chapters (no 32.6, 32.10, no 32.8 forces between wires)

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

THE MAGNETIC FIELD. This handout covers: The magnetic force between two moving charges. The magnetic field, B, and magnetic field lines

AP Physics 1 - Circular Motion and Gravitation Practice Test (Multiple Choice Section) Answer Section

Integral Vector Operations and Related Theorems Applications in Mechanics and E&M

Chapter 28: Magnetic Field and Magnetic Force. Chapter 28: Magnetic Field and Magnetic Force. Chapter 28: Magnetic fields. Chapter 28: Magnetic fields

Physics 111 Lecture 11

Chapter 10 and elements of 11, 12 Rotation of Rigid Bodies

? this lecture. ? next lecture. What we have learned so far. a Q E F = q E a. F = q v B a. a Q in motion B. db/dt E. de/dt B.

DYNAMICS VECTOR MECHANICS FOR ENGINEERS: Kinematics of Rigid Bodies in Three Dimensions. Seventh Edition CHAPTER

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

Consider two masses m 1 at x = x 1 and m 2 at x 2.

Physics 2A Chapter 11 - Universal Gravitation Fall 2017

Lesson 8: Work, Energy, Power (Sections ) Chapter 6 Conservation of Energy

Chapter 8. Linear Momentum, Impulse, and Collisions

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


How Electric Currents Interact with Magnetic Fields

CSU ATS601 Fall Other reading: Vallis 2.1, 2.2; Marshall and Plumb Ch. 6; Holton Ch. 2; Schubert Ch r or v i = v r + r (3.

Transcription:

TEST-03 TPC: MAGNETSM AND MAGNETC EFFECT F CURRENT Q. Fnd the magnetc feld ntensty due to a thn we cayng cuent n the Fg. - R 0 ( + tan) R () 0 ( ) R 0 ( + ) R 0 ( + tan ) R Q. Electons emtted wth neglgble speed fom an electon gun ae acceleated though a potental dffeence V along the -as. These electons emege fom a naow hole nto a unfom magnetc feld of stength dected along -as. Some electons emegng at slghtly degent angles as shown n the Fg. These paaal electons ae efocused on the -as at a dstance - 8 4 e e mv mv F 0 () -as mv e e mv Q.3 A squae loop ACD, cayng a cuent, s placed nea and coplana wth a long staght conducto cayng cuent - A L/ L Thee s no net foce on the loop () The loop wll be attacted by the conducto only f the cuent n the loop flows clockwse The loop wll be attacted by the conducto only f the cuent n the loop flows antclockwse The loop wll always be attacted by the conducto Q.4 A coppe we of damete.6 mm caes a cuent. The mamum magnetc feld due to ths we s 5 0 3 T. The alue of s - 40 A 0 A C D L () 5 A A Q.5 A chage q moes wth a elocty m/s along - as n a unfom magnetc feld ( î + ĵ + 3 kˆ ) tesla - Chage wll epeence a foce n z-y plane () Chage wll epeence a foce along y as Chage wll epeence a foce along + z as Chage wll epeence a foce along z as Q.6 An electon s pojected wth elocty î n unfom magnetc feld 0 kˆ. The nstantaneous foce on ts s - e 0 ĵ () e 0 ĵ e 0 î e 0 kˆ Q.7 Rato of magnetc feld at the cente of a cuent cayng col of adus R and at a dstance of 3R on ts as s - 0 0 () 0 0 0 0 WWW.PHSCSKNWLEDGE.CM Page of 6

Q.8 An electon s mong along poste -as. A unfom electc feld ests towads negate y-as. What should be the decton of magnetc feld of sutable magntude so that net foce on electon s zeo-? poste z-as () negate z-as poste y-as negate y-as Q.9 The magnetc feld at the cente of an equlateal 3 () 3 6 4 Q.3 A conductng od of length and mass m s mong down a smooth nclned plane of nclnaton wth constant elocty. A cuent s flowng n the conducto n a decton pependcula to pape nwad. A etcally upwad magnetc feld ests n space. Then, magntude of magnetc feld s tangula loop of sde L and cayng a cuent s - Sde ew 9 0 4L () 3 0 3 4L 0 3 L 3 0 4L Q.0 A unfom magnetc feld ests n egon whch fom an equlateal tangle of sde a. The magnetc feld s pependcula to the plane of the tangle. A chage q entes nto ths magnetc feld pependculaly wth speed along pependcula bsecto of one sde and comes out along pependcula bsecto of othe sde. The magnetc nducton n the tangle s - m qa () m qa m qa m 4qa Q. A ccula col of adus. Cayng cuent s placed n unfom magnetc feld whch s pependcula to the plane of col, toque actng on the loop s - () 4 zeo Q. n adjacent fgue, all the wes ae long and paallel, f net foce/length on we s zeo, then d d wll be - 3 sn () tan cos sn Q.4 A cuent s unfomly dstbuted oe the coss secton of a long hollow cylndcal we of nne adus R and oute adus R. Magnetc feld aes wth dstance fom the as of cylnde as - () Q.5 Two nfntely long conductng we cay cuents, as shown n fgue. f the hozontal we cayng cuent poduces a magnetc feld at the pont P( d, d, 0), then the esultant magnetc feld at ths pont s A C d d WWW.PHSCSKNWLEDGE.CM Page of 6

d P d j 4A A k () k zeo k Q.6 An electon taellng wth a speed u along the poste -as entes nto a egon of magnetc feld whee = kˆ( 0). t comes out of 0 the egon wth speed then e y u = u at y > 0 () = u at y < 0 > u at y > 0 > u at y < 0 Q.7 An electon moes n a ccula obt wth a unfom speed. t poduces a magnetc feld at the cente of the ccle. The adus of the ccle s popotonal to - () Q.8 A we of length L mete cayng a cuent ampee s bent n the fom of a ccle. ts magntude of magnetc moment wll be - L L L L () 4 4 4 8 Q.9 A long we caes a steady cuent. t s bent nto a ccle of one tun and the magnetc feld at the cente of the col s. t s then bent nto a ccula loop of n tuns. The magnetc feld at the cente of the col wll be - n () n n n Q.0 A mong col galanomete has 50 equal dsons. ts cuent senstty s 0-dsons pe mllampee and oltage senstty s dsons pe mllolt. n ode that each dson eads olt, the esstance n ohms needed to be connected n sees wth the col wll be - 0 5 () 0 3 9995 99995 Q. Total magnetc nducton ( ) at s : F 0 ( ) kˆ C D E () 0 ( + + tan ) ( kˆ ) 0 ( + tan ) ( kˆ ) 0 ( tan ) kˆ Q. Dagam shows a thck walled hollow ppe wth cuent flowng n the shaded poton between a and b. Magnetc feld n the egon between a and b at a dstance fom cente wll be zeo a 0 a b a b () 0 0 b b a Q.3 f magnetc feld s along +e z-as and a potental dffeence s appled acoss an onzed gas chambe placed n the -y plane then : e e + + fee electons (kˆ) (+ e -decton) + e ons V () Magnetc foce on +e ons wll act along +y as () Magnetc foce on electons wll act along + y as oth () and () ae coect () oth () and () ae wong WWW.PHSCSKNWLEDGE.CM Page 3 of 6

nly () s coect nly () s coect Q.4 f the etenson n both the spngs nceases fom to 0 on flowng cuent n the od fom to A then, the alue of magnetc feld wll be - spng constant "K" A = length of od 0 mass of od = m () (0 ) Q.5 A chage patcle hang mass of.6 0 6 kg comes out of acceleato tube wth knetc enegy 0 3 ev. Calculate the smallest magntude of magntc feld that should be appled n etcally downwads decton to just peent the chage patcle fom colldng the plate (Assume chage on patcle = chage of poton) K.Enegy = 0 3 ev Acceleato tuble Plate 0 (mete) Tesla () 4 Tesla 0.0 Tesla 0.04 Tesla Q.6 Two paallel wes cayng cuent and n the same decton, hae magnetc feld at the md pont between them. f cuent s swtched off then magnetc feld at the mdpont wll be - () / 4 /4 Q.7 n the dagam, A s a ccula col of we cayng an antclockwse cuent. C s an nfnte long staght we cayng a cuent pependcula nto the plane of pape though the cente of the col. Foce on C due to A s (R = Radus of col) - 0 C 0 0 () 0 Zeo R Q.8 A solenod of.5 mete length and 4.0 cm damete possesses 0 tuns pe cm. A cuent of 5 ampee s flowng though t. The magnetc nducton at as nsde the solenod s - 0 3 T A () 0 5 T 0 gauss 0 5 gauss Q.9 A poton and an alpha-patcle ente a unfom magnetc feld wth the same elocty. The peod of otaton of the alpha patcle wll be - fou tmes that of the poton () two tmes that of the poton thee tmes that of the poton same as that of the poton Q.30 A squae conductng loop of sde length L caes a cuent. The magnetc feld at the cente of the loop s- ndependent of L () popotonal to L nesely popotonal to L lnealy popotonal to L Q.3 A steam of electons s pojected hozontally to the ght. A staght conducto cayng a cuent s suppoted paallel to the electon steam and aboe t. f the cuent n the conducto s fom left to ght,what wll be the effect on the electon steam - The electon steam wll be pulled upwads () The electon steam wll be pulled downwads The electon steam wll be etaded The electon steam wll be speeded up towads the ght Q.3 A ccula col of we caes a cuent. PQ s a pat of a ey long we cayng a cuent and passng close to the ccula col. f the dectons of cuents ae those shown n fgue, what s the decton of foce actng on PQ? WWW.PHSCSKNWLEDGE.CM Page 4 of 6

Q Paallel to PQ, towads P () Paallel to PQ, towads Q At ght angles to PQ, to ght At ght angles to PQ, to the left Q.33 Two staght long conductos A and CD ae pependcula to each othe and cay cuents and. The magntude of the magnetc nducton at a pont P at a dstance d fom the pont n a decton pependcula to the plane ACD s - 0 ( + ) () d 0 d P ( ) 0 d 0 ( ) 4d Q.34 Two patcles and hang equal chages, afte beng acceleated though the same potental dffeence, ente a egon of unfom magnetc feld and descbe ccula paths of ad R and R espectely. The ato of masses of and s - (R /R ) / () (R /R ) (R /R ) (R /R ) Q.35 The feld nomal to the plane of a we of n tuns and adus whch caes a cuent s measued of the col at a small dstance h fom the cente of the col. Ths s smalle than the feld at the cente by the facton - 3 h h 3 () 3 h 3 h Q.36 n a coaal staght cable, the nne conducto and the oute conducto hae equal cuents n opposte dectons. The magnetc nducton s zeo - nsde the nne conducto () nsde the oute conducto n between the two conductos outsde the oute conducto Q.37 Two patcles and hang equal chages, afte beng acceleated though the same potental dffeence, ente a egon of unfom magnetc feld and descbe ccula paths of ad R and R espectely. The ato of mass of to that of s (R /R ) / () R /R (R /R ) R /R Q.38 Two wes PQ and QR, cay equal cuents as shown n Fg. ne end of both the wes etends to nfnty. PQR =. The magntude of the magnetc feld at on the bsecto angle of these two wes at a dstance fom pont Q s Q P 0 sn 4 0 tan 4 () R 0 cot( / ) 4 0 ( cos/ ) (sn / ) Q.39 Fo c = a and a < b < c, the magnetc feld at pont P wll be zeo when - a = b c a P b () a = 5 3 b a = 3 5 b a = 3 b Q.40 Two ccula cols and hang equal numbe of tuns and cay equal cuents n the same sense and subtend same sold angle at pont. f the smalle col s mdway between and, then f we epesent the magnetc nducton due to bgge col at as and due to smalle col at as then WWW.PHSCSKNWLEDGE.CM Page 5 of 6

d.. d/ /T /T = () = = = 4 Q.4 The col n a tangent galanomete s 6 cm n adus. f a cuent of 0 ma s to poduce a deflecton of 45º, then the numbe of tuns wound on t s (take hozontal component of eath's magnetc feld = 0.36 0 4 T and 0 = 4 0 7 Wb A m ) 9 () 458 689 96 Q.4 A cuent cayng loop s placed n a unfom magnetc feld n fou dffeent oentatons,,, and V. f we aange them n deceasng ode of potental enegy, then Q.44 Unts of pole stength of a magnet ae - A m () A m A m A m Q.45 Wok done n tunng a magnet of magnetc moment M by an angle of 90 fom the magnetc medan s n tmes the coespondng wok done to tun though an angle of 60, whee n s - / () /4... > > > V > V > > V. () > > > V > V > > Q.43 The coect cue between and paamagnetc magnetc s - T fo () /T /T WWW.PHSCSKNWLEDGE.CM Page 6 of 6