ENGI 7811/9816 Winter 2017 FEKO Simulation Assignment 3 Due: Monday, Mar 27, 2017

Size: px
Start display at page:

Download "ENGI 7811/9816 Winter 2017 FEKO Simulation Assignment 3 Due: Monday, Mar 27, 2017"

Transcription

1 ENGI 7811/9816 Winter 2017 FEKO Simulation Assignment 3 Due: Monday, Mar 27, STANDING WAVE ANTENNA (DIPOLE) 1. Using FEKO, provide plots for the current distribution and the 3-D far-eld electric-eld pattern of a dipole antenna with length l = 7λ/2. In your simulation, consider frequency=300 MHz, wire radius=0.001λ. Comment on the result (see slide 100 of Unit 3). Figure 1: Current distribution for antenna in 1-1.

2 Figure 2: 3-D far-eld electric eld pattern for antenna in TRAVELING WAVE ANTENNA (YAGI-UDA ANTENNA) 1. Read section 7.3 of our FEKO reference book. 2. Using FEKO, simulate a simple three-element Yagi-Uda dipole array consisting of one driven element and two parasitic elements. The dipoles are spaced at a distance of 0.04λ apart and all have a wire radius of 0.001λ. The driven element has a length of λ. The reector and director elements have a length of 0.49λ and 0.45λ, respectively. Consider a frequency of 300 MHz. Provide plots for the current distribution and the 3-D far-eld electric-eld pattern. Comment on the result and compare it with the results pertaining to the standing wave antenna in Problem 1-1.

3 Figure 3: Current distribution of 2-2.

4 Figure 4: 3-D eld pattern of problem LINEAR AND PLANAR ARRAYS 1. Review Chapter 11 of our FEKO reference book. 2. Two-Element Uniform Half-Wave Dipole Array Placed Along the X-Axis: Using FEKO, verify the broad-side and end-re modes of a two-element half-wave dipole array as discussed in Unit 3 of the class notes (see Figure 5). Use a frequency of 300 MHz, wire radius= 0.001λ, and consider array spacing of d = λ/2, d = 0.7λ, and d = λ. For all cases, provide plots for the 3-D far-eld electric-eld pattern, phi cuts at phi =0 and phi = 180 degrees and a theta cut at theta = 90 degrees (i.e., superimpose the three cuts on a single plot). Compare the cuts obtained with the corresponding resultant patterns in slides 46/47 and 49/50 of Unit 3, and comment on the eect of increasing the array spacing.

5 Figure 5: Two-element dipole array of Problem 3-2.

6 (a) 3-D far-eld pattern of 3-2. (b) Phi and theta cuts superimposed (for 3-2). Figure 6: β = 0 (broad-side mode), and d = 0.5λ [Problem 3-2].

7 (a) 3-D far-eld pattern. (b) Phi and theta cuts superimposed. Figure 7: β = 180 (end-re mode), and d = 0.5λ [Problem 3-2].

8 (a) 3-D far-eld pattern. (b) Phi and theta cuts superimposed. Figure 8: 0 (broad-side mode), and d = 0.7λ [Problem 3-2].

9 (a) 3-D far-eld pattern. (b) Phi and theta cuts superimposed. Figure 9: 180 (end-re mode), and d = 0.7λ [Problem 3-2].

10 (a) 3-D far-eld pattern. (b) Phi and theta cuts superimposed. Figure 10: 0 (broad-side mode), and d = λ [Problem 3-2].

11 (a) 3-D far-eld pattern. (b) Phi and theta cuts superimposed. Figure 11: 180 (end-re mode), and d = λ [Problem 3-2]. 3. Five-Element Uniform Dipole Array Placed along the X-Axis (slide 61 of Unit 3): Using FEKO, simulate the broad-side and end-re modes of a 5-element uniform linear half-wave dipole array placed as shown in Figure 12. Use a frequency of 300 MHz, wire radius=0.001λ, and array spacing d = λ/2. Provide plots for the 3-D far-eld electric-eld pattern, and phi and theta cuts similar to Problem 3-2.

12 Figure 12: Five-element dipole array of Problem 3-3.

13 (a) 3-D electric-eld pattern. (b) Phi and theta cuts superimposed. Figure 13: Five-element array (broad-side mode) of Problem 3-3.

14 (a) 3-D electric-eld pattern. (b) Phi and theta cuts superimposed. Figure 14: Five-element array (end-re mode) of Problem Five-Element Binomial Array Placed Along the X-Axis (slide 83 of Unit 3): Using FEKO, simulate a 5-element binomial half-wave dipole array. Use amplitude distribution of 1/6, 4/6, 6/6, 4/6, 1/6, a frequency of 300 MHz, wire radius=0.001λ, and array spacing d = λ/2. Provide plots for the 3-D far-eld electric-eld pattern. Compare the 3-D eld pattern with that obtained for the ve-element uniform dipole array in Problem 3-3 (i.e., broad-side and end-re modes).

15 (a) 3-D electric-eld pattern. (b) Phi and theta cuts superimposed. Figure 15: Five-element binomial array of Problem A 3 by 3 Uniform Planar Dipole Array: Using FEKO, simulate a 3 3 uniform planar half-wave dipole array arranged as shown in Figure 16. Use a frequency of 300 MHz, wire radius=0.001λ, and β = 0. Provide a 3-D far-eld electric-eld pattern plots for the following cases (comment on the result and compare it with the simulations of the linear array considered in Problem 3-3): dx = 0.5λ and dy = 0.5λ,

16 dx = 0.5λ and dy = λ, dx = λ and dy = 0.5λ, and dx = λ and dy = λ. Figure 16: A 3 3 planar dipole array of Problem 3-5. Figure 17: Plot for Problem 3-5 (dx = 0.5λ and dy = 0.5λ).

17 Figure 18: Plot for Problem 3-5 (dx = 0.5λ and dy = λ).

18 Figure 19: Plot for Problem 3-5 (dx = λ and dy = 0.5λ).

19 Figure 20: Plot for Problem 3-5 (dx = λ and dy = λ).

RADIATING ELEMENTS MAY BE: DIPOLES, SLOTS, POLYRODS, LOOPS, HORNS, HELIX, SPIRALS, LOG PERIODIC STRUCTURES AND EVEN DISHES Dipoles simple structures,

RADIATING ELEMENTS MAY BE: DIPOLES, SLOTS, POLYRODS, LOOPS, HORNS, HELIX, SPIRALS, LOG PERIODIC STRUCTURES AND EVEN DISHES Dipoles simple structures, ANTENNA ARRAYS Array - collection of radiating elements An array may be: 1D (linear), 2D (planar), 3D (frequency selective) structure of radiating elements Purpose More directivity, Steereable beams Radiation

More information

Preliminary Exam: Electromagnetism, Thursday January 12, :00-12:00

Preliminary Exam: Electromagnetism, Thursday January 12, :00-12:00 1 Preliminary Exam: Electromagnetism, Thursday January 12, 2017. 9:00-12:00 Answer a total of any THREE out of the four questions. For your answers you can use either the blue books or individual sheets

More information

Engineering Mechanics Prof. U. S. Dixit Department of Mechanical Engineering Indian Institute of Technology, Guwahati Kinematics

Engineering Mechanics Prof. U. S. Dixit Department of Mechanical Engineering Indian Institute of Technology, Guwahati Kinematics Engineering Mechanics Prof. U. S. Dixit Department of Mechanical Engineering Indian Institute of Technology, Guwahati Kinematics Module 10 - Lecture 24 Kinematics of a particle moving on a curve Today,

More information

Progress In Electromagnetics Research C, Vol. 24, , 2011

Progress In Electromagnetics Research C, Vol. 24, , 2011 Progress In Electromagnetics Research C, Vol. 24, 173 183, 2011 STUDY OF THE RADIATED POLARIZATIO OF A ATEA ARRAY WITH CIRCULAR GEOMETRY K. Louertani 1, *, R. Guinvarc h 2,. Ribière-Tharaud 3, and M. Hélier

More information

Unit 1: Introduction to Antennas + Electromagnetics Review

Unit 1: Introduction to Antennas + Electromagnetics Review Unit 1: Introduction to Antennas + Electromagnetics Review Antennas ENGI 7811 Khalid El-Darymli, Ph.D., EIT Dept. of Electrical and Computer Engineering Faculty of Engineering and Applied Science Memorial

More information

Final Practice Problems

Final Practice Problems Final Practice Problems 1. The figure below shows a snapshot graph at t = 0 s of a sinusoidal wave traveling to the right along a string at 50 m/s. (a) Write the equation that describes the displacement

More information

Antennas Prof. Girish Kumar Department of Electrical Engineering Indian Institute of Technology, Bombay. Module 02 Lecture 08 Dipole Antennas-I

Antennas Prof. Girish Kumar Department of Electrical Engineering Indian Institute of Technology, Bombay. Module 02 Lecture 08 Dipole Antennas-I Antennas Prof. Girish Kumar Department of Electrical Engineering Indian Institute of Technology, Bombay Module 02 Lecture 08 Dipole Antennas-I Hello, and welcome to today s lecture. Now in the last lecture

More information

Chapter 29: Maxwell s Equation and EM Waves. Slide 29-1

Chapter 29: Maxwell s Equation and EM Waves. Slide 29-1 Chapter 29: Maxwell s Equation and EM Waves Slide 29-1 Equations of electromagnetism: a review We ve now seen the four fundamental equations of electromagnetism, here listed together for the first time.

More information

PHYS 102 SECOND MAJOR EXAM TERM 011

PHYS 102 SECOND MAJOR EXAM TERM 011 PHYS 102 SECOND MAJOR EXAM TERM 011 * QUESTION NO: 1 An infinite non-conducting sheet has a surface charge density 0.10*10**(-6) C/m**2 on one side. How far apart are equipotential surfaces whose potentials

More information

ELECTROMAGNETIC FIELD OF A HORIZONTAL IN- FINITELY LONG MAGNETIC LINE SOURCE OVER THE EARTH COATED WITH A DIELECTRIC LAYER

ELECTROMAGNETIC FIELD OF A HORIZONTAL IN- FINITELY LONG MAGNETIC LINE SOURCE OVER THE EARTH COATED WITH A DIELECTRIC LAYER Progress In Electromagnetics Research Letters, Vol. 31, 55 64, 2012 ELECTROMAGNETIC FIELD OF A HORIZONTAL IN- FINITELY LONG MAGNETIC LINE SOURCE OVER THE EARTH COATED WITH A DIELECTRIC LAYER Y.-J. Zhi

More information

Self-Standing End-Fed Electrically Quasi-Uniform Linear Arrays: Analysis, Design, Construction, Measurements and FLOSS

Self-Standing End-Fed Electrically Quasi-Uniform Linear Arrays: Analysis, Design, Construction, Measurements and FLOSS TELECOMMUNICATIONS ENGINEERING APPLICATIONS Self-Standing End-Fed Electrically Quasi-Uniform Linear Arrays: Analysis, Design, Construction, Measurements and FLOSS K.Th. Kondylis, N.I. Yannopoulou, P.E.

More information

B 2 = ɛ o. E o B o. B 2 = 1 µ o. E B. Note that the direction of the vector S gives the direction of propagation of the wave.

B 2 = ɛ o. E o B o. B 2 = 1 µ o. E B. Note that the direction of the vector S gives the direction of propagation of the wave. Physics 33 : Chapter 31 Examples : Electromagnetic Waves Maxwell s equations relate electric and magnetic fields in fairly complex ways, involving space and time derivatives of each other. Combining these

More information

CYK\2009\PH102\Tutorial 10

CYK\2009\PH102\Tutorial 10 CYK\2009\PH02\Tutorial 0 Physics II. [G 6.3] Find the force of attraction between two magnetic dipoles, m and m 2, oriented as shown in the Fig., a distance r apart, (a) using F = 2πIRB cos θ, and (b)

More information

Cyclotron, final. The cyclotron s operation is based on the fact that T is independent of the speed of the particles and of the radius of their path

Cyclotron, final. The cyclotron s operation is based on the fact that T is independent of the speed of the particles and of the radius of their path Cyclotron, final The cyclotron s operation is based on the fact that T is independent of the speed of the particles and of the radius of their path K 1 qbr 2 2m 2 = mv = 2 2 2 When the energy of the ions

More information

Magnetic Measurements

Magnetic Measurements Magnetic Measurements Neil Marks, DLS/CCLRC, Daresbury Laboratory, Warrington WA4 4AD, U.K. Tel: (44) (0)1925 603191 Fax: (44) (0)1925 603192 Philosophy To cover the possible methods of measuring flux

More information

Electric Flux. To investigate this, we have to understand electric flux.

Electric Flux. To investigate this, we have to understand electric flux. Problem 21.72 A charge q 1 = +5. nc is placed at the origin of an xy-coordinate system, and a charge q 2 = -2. nc is placed on the positive x-axis at x = 4. cm. (a) If a third charge q 3 = +6. nc is now

More information

Kevin James. MTHSC 206 Section 16.4 Green s Theorem

Kevin James. MTHSC 206 Section 16.4 Green s Theorem MTHSC 206 Section 16.4 Green s Theorem Theorem Let C be a positively oriented, piecewise smooth, simple closed curve in R 2. Let D be the region bounded by C. If P(x, y)( and Q(x, y) have continuous partial

More information

A-level PHYSICS (7408/3BD)

A-level PHYSICS (7408/3BD) SPECIMEN MATERIAL A-level PHYSICS (7408/3BD) Paper 3 Section B (Turning points in Physics) Specimen 2014 Morning Time allowed: 2 hours Materials For this paper you must have: a pencil a ruler a calculator

More information

DEPARTMENT OF PHYSICS. University at Albany State University of New York. Comprehensive Field Examination. Classical. Monday, May 21, 2018

DEPARTMENT OF PHYSICS. University at Albany State University of New York. Comprehensive Field Examination. Classical. Monday, May 21, 2018 DEPARTMENT OF PHYSICS University at Albany State University of New York Comprehensive Field Examination Classical Monday, May 21, 218 1: AM - 1: PM Instruction: Answer any four out of five questions Please

More information

High Speed Communication Circuits and Systems Lecture 4 Generalized Reflection Coefficient, Smith Chart, Integrated Passive Components

High Speed Communication Circuits and Systems Lecture 4 Generalized Reflection Coefficient, Smith Chart, Integrated Passive Components High Speed Communication Circuits and Systems Lecture 4 Generalized Reflection Coefficient, Smith Chart, Integrated Passive Components Michael H. Perrott February 11, 2004 Copyright 2004 by Michael H.

More information

A Robust Method of Calculating the Effective Length of a Conductive Strip on an Ungrounded Dielectric Substrate

A Robust Method of Calculating the Effective Length of a Conductive Strip on an Ungrounded Dielectric Substrate Progress In Electromagnetics Research M, Vol. 35, 57 66, 2014 A Robust Method of Calculating the Effective Length of a Conductive Strip on an Ungrounded Dielectric Substrate Manimaran Kanesan *, David

More information

Q1. Three point charges are arranged as shown in FIGURE 1. Find the magnitude of the net electrostatic force on the point charge at the origin.

Q1. Three point charges are arranged as shown in FIGURE 1. Find the magnitude of the net electrostatic force on the point charge at the origin. Coordinator: Saleem Rao Monday, May 01, 2017 Page: 1 Q1. Three point charges are arranged as shown in FIGURE 1. Find the magnitude of the net electrostatic force on the point charge at the origin. A) 1.38

More information

Magnetic Flux. Conference 8. Physics 102 General Physics II

Magnetic Flux. Conference 8. Physics 102 General Physics II Physics 102 Conference 8 Magnetic Flux Conference 8 Physics 102 General Physics II Monday, March 24th, 2014 8.1 Quiz Problem 8.1 Suppose we want to set up an EMF of 12 Volts in a circular loop of wire

More information

Copyright , Larry Randall, d/b/a The NRE Group All Rights Reserved

Copyright , Larry Randall, d/b/a The NRE Group All Rights Reserved NEAR VERTICAL INCIDENCE SKYWAVE (NVIS) Larry Randall -WA5BEN The NRE Group larry@nregroup.net Revision: 1.6 Issue Date: 06 Nov 2014 Copyright 2007 2015, Larry Randall, d/b/a The NRE Group All Rights Reserved

More information

March 11. Physics 272. Spring Prof. Philip von Doetinchem

March 11. Physics 272. Spring Prof. Philip von Doetinchem Physics 272 March 11 Spring 2014 http://www.phys.hawaii.edu/~philipvd/pvd_14_spring_272_uhm.html Prof. Philip von Doetinchem philipvd@hawaii.edu Phys272 - Spring 14 - von Doetinchem - 32 Summary Magnetic

More information

PHYSICS 218 FINAL EXAM Friday, December 11, 2009

PHYSICS 218 FINAL EXAM Friday, December 11, 2009 PHYSICS 218 FINAL EXAM Friday, December 11, 2009 NAME: SECTION: 525 526 527 528 Note: 525 Recitation Wed 9:10-10:00 526 Recitation Wed 11:30-12:20 527 Recitation Wed 1:50-2:40 528 Recitation Mon 11:30-12:20

More information

Questions Chapter 22 Electric Fields

Questions Chapter 22 Electric Fields Questions Chapter 22 Electric Fields 22-1 What is Physics? 22-2 The Electric Field 22-3 Electric Field Lines 22-4 Electric Field due to a Point Charge 22-5 Electric Field due to an Electric Dipole 22-6

More information

Problem 2: 25 points The space between the conductors of a long coaxial cable used to transmit television signals has an inner radius r 1 =0:15 mm and

Problem 2: 25 points The space between the conductors of a long coaxial cable used to transmit television signals has an inner radius r 1 =0:15 mm and Physics 272. Practice Final Exam On the nal exam there will be 8 problems. The nal exam is Thursday May 12th, 9:45-11:45 a.m. in WAT 112 Problem 1: 25 points A sphere has a volume charge density (r) =

More information

UNIVERSITY OF BOLTON. SCHOOL OF ENGINEERING, SPORTS and SCIENCES BENG (HONS) ELECTRICAL & ELECTRONICS ENGINEERING EXAMINATION SEMESTER /2018

UNIVERSITY OF BOLTON. SCHOOL OF ENGINEERING, SPORTS and SCIENCES BENG (HONS) ELECTRICAL & ELECTRONICS ENGINEERING EXAMINATION SEMESTER /2018 ENG018 SCHOOL OF ENGINEERING, SPORTS and SCIENCES BENG (HONS) ELECTRICAL & ELECTRONICS ENGINEERING MODULE NO: EEE6002 Date: 17 January 2018 Time: 2.00 4.00 INSTRUCTIONS TO CANDIDATES: There are six questions.

More information

(x + y) ds. 2 (1) dt = p Find the work done by the force eld. yzk

(x + y) ds. 2 (1) dt = p Find the work done by the force eld. yzk MATH Final Exam (Version 1) Solutions May 4, 11 S. F. Ellermeyer Name Instructions. Your work on this exam will be graded according to two criteria: mathematical correctness and clarity of presentation.

More information

CQ 1 What is alike when we say "two like charges?" Do they look, feel, or smell alike?

CQ 1 What is alike when we say two like charges? Do they look, feel, or smell alike? Ch20P Page 1 1P22/1P92 Problems (2011) Chapter 20 Electric Fields and Forces Sunday, January 09, 2011 4:50 PM CQ 1 What is alike when we say "two like charges?" Do they look, feel, or smell alike? CQ 3

More information

MATH The Derivative as a Function - Section 3.2. The derivative of f is the function. f x h f x. f x lim

MATH The Derivative as a Function - Section 3.2. The derivative of f is the function. f x h f x. f x lim MATH 90 - The Derivative as a Function - Section 3.2 The derivative of f is the function f x lim h 0 f x h f x h for all x for which the limit exists. The notation f x is read "f prime of x". Note that

More information

Outline. Recall... Limits. Problem Solving Sessions. MA211 Lecture 4: Limits and Derivatives Wednesday 17 September Definition (Limit)

Outline. Recall... Limits. Problem Solving Sessions. MA211 Lecture 4: Limits and Derivatives Wednesday 17 September Definition (Limit) Outline MA211 Lecture 4: Limits and Wednesday 17 September 2008 1 0.2 0.15 0.1 2 ) x) 0.05 0 0.05 0.1 3 ) t) 0.15 0.2 0.4 0.3 0.2 0.1 0 0.1 0.2 0.3 0.4 4 Extra: Binomial Expansions MA211 Lecture 4: Limits

More information

Shaping the Beam of Light in Nanometer Scales: A Yagi-Uda Nanoantenna in Optical Domain

Shaping the Beam of Light in Nanometer Scales: A Yagi-Uda Nanoantenna in Optical Domain Shaping the Beam of Light in Nanometer Scales: A Yagi-Uda Nanoantenna in Optical Domain Jingjing Li, Alessandro Salandrino, and Nader Engheta* University of Pennsylvania Department of Electrical and Systems

More information

4. Theunitsoftheelectric eldare: A. N C 2 B. C/N C. N D. N/C E. C=m 2 ans: D Section: 22{2; Di±culty: E. Chapter 22: ELECTRIC FIELDS 377

4. Theunitsoftheelectric eldare: A. N C 2 B. C/N C. N D. N/C E. C=m 2 ans: D Section: 22{2; Di±culty: E. Chapter 22: ELECTRIC FIELDS 377 Chapter 22: ELECTRIC FIELDS 1 An electric eld is most directly related to: A the momentum of a test charge B the kinetic energy of a test charge C the potential energy of a test charge D the force acting

More information

Electric Fields and Forces. Key Concepts

Electric Fields and Forces. Key Concepts Ch20Lectures Page 1 Ch20Lectures Monday, January 25, 2010 7:33 AM Chapter 20 Electric Fields and Forces Key Concepts electric charge principle of conservation of charge charge polarization, both permanent

More information

PHYS 102 Exams. PHYS 102 Exam 3 PRINT (A)

PHYS 102 Exams. PHYS 102 Exam 3 PRINT (A) PHYS 102 Exams PHYS 102 Exam 3 PRINT (A) The next two questions pertain to the situation described below. A metal ring, in the page, is in a region of uniform magnetic field pointing out of the page as

More information

Lagrangian Dynamics: Generalized Coordinates and Forces

Lagrangian Dynamics: Generalized Coordinates and Forces Lecture Outline 1 2.003J/1.053J Dynamics and Control I, Spring 2007 Professor Sanjay Sarma 4/2/2007 Lecture 13 Lagrangian Dynamics: Generalized Coordinates and Forces Lecture Outline Solve one problem

More information

Coulomb Balance. Figure 1: The Coulomb Balance apparatus.

Coulomb Balance. Figure 1: The Coulomb Balance apparatus. Coulomb Balance Name Partner Date Introduction In this experiment we will use the Coulomb Balance shown in Figure 1 to determine how the force between two charges depends upon the distance of separation

More information

Absorption efficiency and physical bounds on antennas

Absorption efficiency and physical bounds on antennas Absorption efficiency and physical bounds on antennas Gustafsson, Mats; Cismasu, Marius; Nordebo, Sven 21 Link to publication Citation for published version (APA): Gustafsson, M., Cismasu, M., & Nordebo,

More information

Lecture 34: MON 13 APR Ch ,5

Lecture 34: MON 13 APR Ch ,5 Physics 2102 Jonathan Dowling James Clerk Maxwell (1831-1879) Lecture 34: MON 13 APR Ch.33.1 3,5 3,5 7: E&M Waves MT03 Avg: 65/100 Q1/P3 K. Schafer Office hours: MW 1:30-2:30 pm 222B Nicholson P1/Q2 J.

More information

Electrostatics. 4πε 2) + Q / 2 4) 4 Q

Electrostatics. 4πε 2) + Q / 2 4) 4 Q Two spheres A and B of radius a and b respectively are at the same potential The ratio of the surface charge density of A to B is: ) a / b ) b / a a / b b / a Two free protons are separated by a distance

More information

Math 241: Multivariable calculus

Math 241: Multivariable calculus Math 241: Multivariable calculus Professor Leininger Fall 2014 Calculus of 1 variable In Calculus I and II you study real valued functions of a single real variable. Examples: f (x) = x 2, r(x) = 2x2 +x

More information

and Ee = E ; 0 they are separated by a dielectric material having u = io-s S/m, µ, = µ, 0

and Ee = E ; 0 they are separated by a dielectric material having u = io-s S/m, µ, = µ, 0 602 CHAPTER 11 TRANSMISSION LINES 11.10 Two identical pulses each of magnitude 12 V and width 2 µs are incident at t = 0 on a lossless transmission line of length 400 m terminated with a load. If the two

More information

Tuesday, September 29, Page 453. Problem 5

Tuesday, September 29, Page 453. Problem 5 Tuesday, September 9, 15 Page 5 Problem 5 Problem. Set up and evaluate the integral that gives the volume of the solid formed by revolving the region bounded by y = x, y = x 5 about the x-axis. Solution.

More information

A) 4 B) 3 C) 2 D) 5 E) 6

A) 4 B) 3 C) 2 D) 5 E) 6 Coordinator: Saleem Rao Monday, January 01, 2018 Page: 1 Q1. A standing wave having three nodes is set up in a string fixed at both ends. If the frequency of the wave is doubled, how many antinodes will

More information

ELECTROSTATICS (Important formulae and Concepts) I Electric charges and Coulomb s law

ELECTROSTATICS (Important formulae and Concepts) I Electric charges and Coulomb s law ELECTROSTATICS (Important formulae and Concepts) I Electric charges and Coulomb s law II Electric Field and Electric Dipole www.nrpschool.com www.nrpschool.com III ELECTRIC POTENTIAL www.nrpschool.com

More information

Cylindrical Antennas and Arrays Revised and enlarged 2nd edition of Arrays of Cylindrical Dipoles

Cylindrical Antennas and Arrays Revised and enlarged 2nd edition of Arrays of Cylindrical Dipoles Cylindrical Antennas and Arrays Revised and enlarged 2nd edition of Arrays of Cylindrical Dipoles Ronold W. P. King Gordon McKay Professor of Applied Physics, Emeritus, Harvard University George J. Fikioris

More information

Completion Date: Monday February 11, 2008

Completion Date: Monday February 11, 2008 MATH 4 (R) Winter 8 Intermediate Calculus I Solutions to Problem Set #4 Completion Date: Monday February, 8 Department of Mathematical and Statistical Sciences University of Alberta Question. [Sec..9,

More information

Columbia University Department of Physics QUALIFYING EXAMINATION

Columbia University Department of Physics QUALIFYING EXAMINATION Columbia University Department of Physics QUALIFYING EXAMINATION Monday, January 14, 2013 3:10PM to 5:10PM Classical Physics Section 2. Electricity, Magnetism & Electrodynamics Two hours are permitted

More information

Charge and current elements

Charge and current elements Charge and current elements for 1-, 2- and 3-dimensional integration Frits F.M. de Mul Presentations: Electromagnetism: History Electromagnetism: Electr. topics Electromagnetism: Magn. topics Electromagnetism:

More information

Engineering Physics 1 Dr. B. K. Patra Department of Physics Indian Institute of Technology-Roorkee

Engineering Physics 1 Dr. B. K. Patra Department of Physics Indian Institute of Technology-Roorkee Engineering Physics 1 Dr. B. K. Patra Department of Physics Indian Institute of Technology-Roorkee Module-05 Lecture-04 Maxwellian Distribution Law of Velocity Part 02 So, we have already told to experiment

More information

Mathematics B Monday 2 November 2015 Paper One Question book

Mathematics B Monday 2 November 2015 Paper One Question book 2015 Senior External Examination Mathematics B Monday 2 November 2015 Paper One Question book 9 am to 12:10 pm Time allowed Perusal time: 10 minutes Working time: 3 hours Examination materials provided

More information

In this lecture we calculate moments and products of inertia of some simple geometric figures. (Refer Slide Time: 0:22)

In this lecture we calculate moments and products of inertia of some simple geometric figures. (Refer Slide Time: 0:22) Engineering Mechanics Professor Manoj K Harbola Department of Physics Indian Institute of Technology Kanpur Module 4 Lecture No 37 Properties of plane surfaces VIII: second moment and product of an area,

More information

Maxwell's Eqns & Related Formulae Scalar & Vector Potentials Radiation Mechanism Ackgt. Antennas ENGI Winter 2017

Maxwell's Eqns & Related Formulae Scalar & Vector Potentials Radiation Mechanism Ackgt. Antennas ENGI Winter 2017 Unit 1: to Antennas + Electromagnetics Review Antennas ENGI 7811 Khalid El-Darymli, Ph.D., EIT Dept. of Electrical and Computer Engineering Faculty of Engineering and Applied Science Memorial University

More information

Analysis of log-periodic dipole arrays with boundary elements

Analysis of log-periodic dipole arrays with boundary elements Boundary Elements and Other Mesh Reduction Methods XXX 75 Analysis of log-periodic dipole arrays with boundary elements D. Poljak 1, V. Doric 1, M. Birkic 2 & D. Kosor 3 1 Department of Electronics, University

More information

Physics P201 D. Baxter/R. Heinz. FINAL EXAM December 10, :00 10:00 AM INSTRUCTIONS

Physics P201 D. Baxter/R. Heinz. FINAL EXAM December 10, :00 10:00 AM INSTRUCTIONS Seat # Physics P201 D. Baxter/R. Heinz FINAL EXAM December 10, 2001 8:00 10:00 AM INSTRUCTIONS 1. Sit in SEAT # given above. 2. DO NOT OPEN THE EXAM UNTIL YOU ARE TOLD TO DO SO. 3. Print your name (last

More information

Arrays. Ranga Rodrigo. August 19, 2010

Arrays. Ranga Rodrigo. August 19, 2010 Arrays Ranga Rodrigo August 9, 00 Lecture notes are fully based on Balanis [?. Some diagrams and text are directly from the books. Contents Two-Element Array -Element Linear Array: Uniform Amplitude and

More information

ENGI 4430 Line Integrals; Green s Theorem Page 8.01

ENGI 4430 Line Integrals; Green s Theorem Page 8.01 ENGI 4430 Line Integrals; Green s Theorem Page 8.01 8. Line Integrals Two applications of line integrals are treated here: the evaluation of work done on a particle as it travels along a curve in the presence

More information

University of Houston Mathematics Contest: Physics Exam 2017

University of Houston Mathematics Contest: Physics Exam 2017 Unless otherwise specified, please use g as the acceleration due to gravity at the surface of the earth. Vectors x, y, and z are unit vectors along x, y, and z, respectively. Let G be the universal gravitational

More information

Physics 240 Fall 2003: Exam #1. Please print your name: Please list your discussion section number: Please list your discussion instructor:

Physics 240 Fall 2003: Exam #1. Please print your name: Please list your discussion section number: Please list your discussion instructor: Physics 4 Fall 3: Exam #1 Please print your name: Please list your discussion section number: Please list your discussion instructor: Form #1 Instructions 1. Fill in your name above. This will be a 1.5

More information

PHY132 Review for Mid-Term Test

PHY132 Review for Mid-Term Test PHY132 Review for Mid-Term Test Examinations are formidable even to the best prepared, for the greatest fool may ask more than the wisest man can answer. Charles Caleb Colton, English writer (1780-1832)

More information

jfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksm+nklth egkjkt

jfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksm+nklth egkjkt Phone : 93 93 7779, 9893 58881 Sount & Waves Page: 9 fo/u fopkjr Hkh# tu] ugha vkjehks dke] foifr ns[k NksM+s rqjar e/;e eu dj ';kea iq#"k flag ladyi dj] lgrs foifr vusd] ^cuk^ u NksM+s /;s; dks] j?kqcj

More information

Physics 2401 Summer 2, 2008 Exam III

Physics 2401 Summer 2, 2008 Exam III Physics 2401 Summer 2, 2008 Exam e = 1.60x10-19 C, m(electron) = 9.11x10-31 kg, ε 0 = 8.845x10-12 C 2 /Nm 2, k e = 9.0x10 9 Nm 2 /C 2, m(proton) = 1.67x10-27 kg. n = nano = 10-9, µ = micro = 10-6, m =

More information

Unit 1 & 2 Maths Methods (CAS) Exam

Unit 1 & 2 Maths Methods (CAS) Exam Name: Teacher: Unit 1 & 2 Maths Methods (CAS) Exam 2 2017 Monday November 20 (1.00pm - 3.15pm) Reading time: 15 Minutes Writing time: 120 Minutes Instruction to candidates: Students are permitted to bring

More information

Family Name: Given Name: Student number:

Family Name: Given Name: Student number: Family Name: Given Name: Student number: Academic Honesty: In accordance with the Academic Honesty Policy (T0.02), academic dishonesty in any form will not be tolerated. Prohibited acts include, but are

More information

Chapter 14. PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman. Lectures by Wayne Anderson

Chapter 14. PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman. Lectures by Wayne Anderson Chapter 14 Periodic Motion PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman Lectures by Wayne Anderson Exam 3 results Class Average - 57 (Approximate grade

More information

PHYSICS B SAMPLE EXAM I Time - 90 minutes 70 Questions

PHYSICS B SAMPLE EXAM I Time - 90 minutes 70 Questions Page 1 of 7 PHYSCS B SAMPLE EXAM Time - 90 minutes 70 Questions Directions:Each of the questions or incomplete statements below is followed by five suggested Solutions or completions. Select the one that

More information

FIFTH MIDTERM -- REVIEW PROBLEMS

FIFTH MIDTERM -- REVIEW PROBLEMS Physics 2210 Fall 2005 Paolo Gondolor FIFTH MIDTERM -- REVIEW PROBLEMS A solution set is available on the course web page in pdf format (no solutions for 27-29). 7 1. Assume that the planet Uranus has

More information

Class 11 : Magnetic materials

Class 11 : Magnetic materials Class 11 : Magnetic materials Magnetic dipoles Magnetization of a medium, and how it modifies magnetic field Magnetic intensity How does an electromagnet work? Boundary conditions for B Recap (1) Electric

More information

Programming with General Relativity. Michael. C. Ryan

Programming with General Relativity. Michael. C. Ryan Programming with General Relativity Michael. C. Ryan August 5, 2009 Introduction This report is intended for its readers to view my progress. My primary focus is General Relativity and its consequences

More information

(12) Patent Application Publication (10) Pub. No.: US 2006/ A1

(12) Patent Application Publication (10) Pub. No.: US 2006/ A1 US 20060070371A1 (19) United States (12) Patent Application Publication (10) Pub. No.: US 2006/0070371 A1 St. Clair (43) Pub. Date: Apr. 6, 2006 (54) ELECTRIC DIPOLE MOMENT PROPULSION (22) Filed: Oct.

More information

PHYSICS 12 NAME: Gravitation

PHYSICS 12 NAME: Gravitation NAME: Gravitation 1. The gravitational force of attraction between the Sun and an asteroid travelling in an orbit of radius 4.14x10 11 m is 4.62 x 10 17 N. What is the mass of the asteroid? 2. A certain

More information

(Refer Slide Time: 3:39)

(Refer Slide Time: 3:39) Course on Momentum Transfer in Process Engineering By Professor Tridib Kumar Goswami Department of Agricultural & Food Engineering Indian Institute of Technology, Kharagpur Lecture 1 Module 1 Mass balance

More information

1. Write the relation for the force acting on a charge carrier q moving with velocity through a magnetic field in vector notation. Using this relation, deduce the conditions under which this force will

More information

This practice exam is intended to help you prepare for the final exam for MTH 142 Calculus II.

This practice exam is intended to help you prepare for the final exam for MTH 142 Calculus II. MTH 142 Practice Exam Chapters 9-11 Calculus II With Analytic Geometry Fall 2011 - University of Rhode Island This practice exam is intended to help you prepare for the final exam for MTH 142 Calculus

More information

Section 24.8 Magnets and Magnetic Materials Pearson Education, Inc.

Section 24.8 Magnets and Magnetic Materials Pearson Education, Inc. Section 24.8 Magnets and Magnetic Materials A Current Loop in a Uniform Field Slide 24-2 A Current Loop in a Uniform Field A magnetic dipole will rotate to line up with a magnetic field just as an electric

More information

Physics Lecture 13

Physics Lecture 13 Physics 113 Jonathan Dowling Physics 113 Lecture 13 EXAM I: REVIEW A few concepts: electric force, field and potential Gravitational Force What is the force on a mass produced by other masses? Kepler s

More information

LAB 03 Electric Fields and Potentials

LAB 03 Electric Fields and Potentials Group: LAB 03 Electric Fields and Potentials Names: (Principle Coordinator) (Lab Partner) (Lab Partner) Motto: Say map! Say map! Dora the Explorer Goals: Developing an intuitive picture of the electric

More information

Inquiry 4.1. Investigating Seasons on Earth

Inquiry 4.1. Investigating Seasons on Earth Inquiry 4.1 Investigating Seasons on Earth PROCEDURE 1. Insert the rod labeled E through your globe to form an axis of rotation. 2. Stick the rod of your globe into the center hole of Side B of the SEM

More information

Periodic Leaky-Wave Antennas for Orbital Angular Momentum Multiplexing System Master Thesis Final Presentation

Periodic Leaky-Wave Antennas for Orbital Angular Momentum Multiplexing System Master Thesis Final Presentation Periodic Leaky-Wave Antennas for Orbital Angular Momentum Multiplexing System Master Thesis Final Presentation Amar Al-Bassam 23.06.2014 Outline I. INTRODUCTION II. CONCEPT OF GENERATION III. ELECTROMAGNETIC

More information

Reading Question 30.2

Reading Question 30.2 Reading Question 30.2 The speed of electrons in a typical current-carrying wire is A. Extremely slow ( 10 4 m/s). B. Moderate ( 1 m/s). C. Very fast ( 10 4 m/s). D. The speed of light. Slide 30-13 Electric

More information

Name: School Name: PHYSICS CONTEST EXAMINATION

Name: School Name: PHYSICS CONTEST EXAMINATION PHYSICS CONTEST EXAMINATION - 2013 Unless otherwise specified, please use g as the acceleration due to gravity at the surface of the earth. Please note that i^, j^, and k^ are unit vectors along the x-axis,

More information

Columbia University Department of Physics QUALIFYING EXAMINATION

Columbia University Department of Physics QUALIFYING EXAMINATION Columbia University Department of Physics QUALIFYING EXAMINATION Monday, January 8, 2018 10:00AM to 12:00PM Classical Physics Section 1. Classical Mechanics Two hours are permitted for the completion of

More information

Quantum Physics Lecture 8

Quantum Physics Lecture 8 Quantum Physics Lecture 8 Applications of Steady state Schroedinger Equation Box of more than one dimension Harmonic oscillator Particle meeting a potential step Waves/particles in a box of >1 dimension

More information

Design of a Non-uniform High Impedance Surface for a Low Profile Antenna

Design of a Non-uniform High Impedance Surface for a Low Profile Antenna 352 Progress In Electromagnetics Research Symposium 2006, Cambridge, USA, March 26-29 Design of a Non-uniform High Impedance Surface for a Low Profile Antenna M. Hosseini 2, A. Pirhadi 1,2, and M. Hakkak

More information

Steady and unsteady diffusion

Steady and unsteady diffusion Chapter 5 Steady and unsteady diffusion In this chapter, we solve the diffusion and forced convection equations, in which it is necessary to evaluate the temperature or concentration fields when the velocity

More information

Candidacy Exam Department of Physics February 6, 2010 Part I

Candidacy Exam Department of Physics February 6, 2010 Part I Candidacy Exam Department of Physics February 6, 2010 Part I Instructions: ˆ The following problems are intended to probe your understanding of basic physical principles. When answering each question,

More information

Problem Score 1 /30 2 /15 3 /15 4 /20 5 /20 6 /20 7 /15 8 /25 9 /20 10 /20 Total /200

Problem Score 1 /30 2 /15 3 /15 4 /20 5 /20 6 /20 7 /15 8 /25 9 /20 10 /20 Total /200 PHYS 2114 Final Exam December 15, 2005 Time of Discussion Section: Name: Instructions: Do not open exam until so instructed. Write name and discussion time above; do not write anything in table at right.

More information

Math 152 Take Home Test 1

Math 152 Take Home Test 1 Math 5 Take Home Test Due Monday 5 th October (5 points) The following test will be done at home in order to ensure that it is a fair and representative reflection of your own ability in mathematics I

More information

Physics 54 Lecture March 1, Micro-quiz problems (magnetic fields and forces) Magnetic dipoles and their interaction with magnetic fields

Physics 54 Lecture March 1, Micro-quiz problems (magnetic fields and forces) Magnetic dipoles and their interaction with magnetic fields Physics 54 Lecture March 1, 2012 OUTLINE Micro-quiz problems (magnetic fields and forces) Magnetic dipoles and their interaction with magnetic fields Electromagnetic induction Introduction to electromagnetic

More information

Unit 2: Small Antennas + Some Antenna Parameters

Unit 2: Small Antennas + Some Antenna Parameters Unit 2: Small Antennas + Some Antenna Parameters Antenna Theory ENGI 9816 Khalid El-Darymli, Ph.D., EIT Dept. of Electrical and Computer Engineering Faculty of Engineering and Applied Science Memorial

More information

APPLIED OPTICS POLARIZATION

APPLIED OPTICS POLARIZATION A. La Rosa Lecture Notes APPLIED OPTICS POLARIZATION Linearly-polarized light Description of linearly polarized light (using Real variables) Alternative description of linearly polarized light using phasors

More information

Old Exams - Questions Ch-16

Old Exams - Questions Ch-16 Old Exams - Questions Ch-16 T081 : Q1. The displacement of a string carrying a traveling sinusoidal wave is given by: y( x, t) = y sin( kx ω t + ϕ). At time t = 0 the point at x = 0 m has a displacement

More information

PHYSICS - CLUTCH CH 23: ELECTRIC POTENTIAL.

PHYSICS - CLUTCH CH 23: ELECTRIC POTENTIAL. !! www.clutchprep.com CONCEPT: ELECTRIC POTENTIAL ENERGY If you release 2 charges, they move gain. Where did it come from? - Two charges have a stored energy between them, called - ENERGY CONSERVATION:

More information

{ 2{ water vapor prole is specied by the surface relative humidity and a water vapor scale height (set at 2 km). We nd a good, theoretically based (se

{ 2{ water vapor prole is specied by the surface relative humidity and a water vapor scale height (set at 2 km). We nd a good, theoretically based (se SMA TECHNICAL MEMO 123 Date: 3 June 1998 Estimates of Haystack Opacity at 225 GHz Mark A. Gurwell ABSTRACT We estimate opacity at 225 GHz for the SMA Haystack site, based upon local weather data, measurements

More information

σ ε ω 1 /σ ω ε α=ω 2 /ω 1

σ ε ω 1 /σ ω ε α=ω 2 /ω 1 The measurement line at the Antiproton Decelerator Ulrik Mikkelsen Institute for Storage Ring Facilities, ISA, University of Aarhus, DK{8000 Aarhus C, Denmark and PS-CA, CERN, CH-1211 Geneva 23, Switzerland

More information

Sec 4 Maths. SET A PAPER 2 Question

Sec 4 Maths. SET A PAPER 2 Question S4 Maths Set A Paper Question Sec 4 Maths Exam papers with worked solutions SET A PAPER Question Compiled by THE MATHS CAFE 1 P a g e Answer all the questions S4 Maths Set A Paper Question Write in dark

More information

Mu Alpha Theta State 2007 Euclidean Circles

Mu Alpha Theta State 2007 Euclidean Circles Mu Alpha Theta State 2007 Euclidean Circles 1. Joe had a bet with Mr. Federer saying that if Federer can solve the following problem in one minute, Joe would be his slave for a whole month. The problem

More information

4.4 Microstrip dipole

4.4 Microstrip dipole 4.4 Microstrip dipole Basic theory Microstrip antennas are frequently used in today's wireless communication systems. Thanks to their low profile, they can be mounted to the walls of buildings, to the

More information