Magnetic Fields Due to Currents JH

Slides:



Advertisements
Similar presentations
Magnetism and Currents. A current generates a magnetic field. A magnetic field exerts a force on a current. Two contiguous conductors, carrying currents,
Advertisements

1 My Chapter 19 Lecture Outline. 2 Chapter 19: Magnetic Forces and Fields Magnetic Fields Magnetic Force on a Point Charge Motion of a Charged Particle.
HW7 due on Friday Turn in HW6 Stand by to receive back HW5 EXAM 2 coming up on Monday !!!!! March 30 th.
Electromagnetic Induction Inductors. Problem A metal rod of length L and mass m is free to slide, without friction, on two parallel metal tracks. The.
Chapter 30 Sources of the magnetic field
Chapter 27 Sources of the magnetic field
Current and Resistance JH
Review 2.
Prof Viviana Vladutescu Problem Solving. A cylindrical pipe with a 1.0 cm wall thickness and an inner radius of 4.0 cm is centered on the z-axis and.
Chapter 28 Sources of Magnetic Field
Physics 121 Practice Problem Solutions 10 Magnetic Fields from Currents (Biot-Savart and Ampere’s Law) Contents: 121P10 - 1P, 5P, 8P, 10P, 19P, 29P,
Sources of Magnetic Field Chapter 28 Study the magnetic field generated by a moving charge Consider magnetic field of a current-carrying conductor Examine.
Ampere’s Law.
Two questions: (1) How to find the force, F on the electric charge, q excreted by the field E and/or B? (2) How fields E and/or B can be created?
AP Physics C Chapter 28.  s1/MovingCharge/MovingCharge.html s1/MovingCharge/MovingCharge.html.
Copyright © 2009 Pearson Education, Inc. Chapter 27 Magnetism.
Physics 121 Practice Problem Solutions 11 Faraday’s Law of Induction
INDUCTANCE Plan:  Inductance  Calculating the Inductance  Inductors with Magnetic materials.
Magnetic Field Strength Around a Wire. From the demonstration, we saw that: the magnetic field strength varies directly with the amount of current flowing.
Chapter 28--Examples.
Flux Density due to a current flowing in a long straight wire © David Hoult 2009.
Experimental Measurement of the Charge to Mass Ratio of the Electron Stephen Luzader Physics Department Frostburg State University Frostburg, MD.
Written by Dr. John K. Dayton MAGNETIC FIELDS THE MAGNETIC FIELD FORCES ON MOVING CHARGES THE MAGNETIC FIELD OF A LONG, STRAIGHT WIRE THE MAGNETIC FIELD.
Nov PHYS , Dr. Andrew Brandt PHYS 1444 – Section 003 Lecture #20, Review Part 2 Tues. November Dr. Andrew Brandt HW28 solution.
1 Chapter 29: Magnetic Fields due to Currents Introduction What are we going to talk about in chapter 30: How do we calculate magnetic fields for any distribution.
Monday, Mar. 27, 2006PHYS , Spring 2006 Dr. Jaehoon Yu 1 PHYS 1444 – Section 501 Lecture #16 Monday, Mar. 27, 2006 Dr. Jaehoon Yu Sources of Magnetic.
Copyright © 2009 Pearson Education, Inc. Ampère’s Law.
Magnetic Field Chapter 28 opener. A long coil of wire with many closely spaced loops is called a solenoid. When a long solenoid carries an electric current,
The wires are separated by distance a and carry currents I 1 and I 2 in the same direction. Wire 2, carrying current I 2, sets up a magnetic field B 2.
AP Physics C III.D – Magnetic Forces and Fields. The source and direction of magnetic fields.
Physics 2102 Magnetic fields produced by currents Physics 2102 Gabriela González.
Announcements  Homework for tomorrow… Ch. 32: CQ 6, Probs. 16 & : a) –(3.2 x T) jhatb) 0 Tc) +(1.1 x T) ihat 32.6: +(2.9 x
General Physics II, Additional Questions, By/ T.A. Eleyan 1 Additional Questions Lec. 15,16.
Review 1.
Thursday March 31, PHYS Dr. Andrew Brandt PHYS 1444 – Section 02 Lecture #16 Thursday Mar 31, 2011 Dr. Andrew Brandt HW7 Ch 27 is due Fri.
TUesday, April 12, PHYS Dr. Andrew Brandt PHYS 1444 – Section 02 Review #2 Tuesday April 12, 2011 Dr. Andrew Brandt TEST IS THURSDAY 4/14.
Electrostatics in Vacuum, in Conductors and in the Presence of Linear Dielectrics Principle of Superposition Charges were at rest.
CHAPTER 26 : CAPACITANCE AND DIELECTRICS

Magnetism #2 Induced EMF Ch.20. Faraday’s Law of Induction We now know that a current carrying wire will produce its own magnetic field with the lines.
Two questions: (1) How to find the force, F on the electric charge, Q excreted by the field E and/or B? (2) How fields E and/or B can be created?
Magnetic Fields. Magnetic Fields and Forces a single magnetic pole has never been isolated magnetic poles are always found in pairs Earth itself is a.
More Examples of Biot-Savart & Ampère’s Law. Recall: Biot-Savart Law: Ampere’s Law:
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
 B = BA Cos  Example 1.1 A coil consists of 200 turns of wire. Each turn is a square of side 18 cm, and a uniform magnetic field directed.
Magnetism quiz. Draw the magnetic field lines (3 pts each) N S 1. + e I I e N S I
Applications of Ampere’s Law
Week 9 Presentation 1 Electromagnets 1. Learning Objectives: 1. Determine the magnitude and direction of the magnetic field strength generated by a straight.
1© Manhattan Press (H.K.) Ltd magnetic fields due to currents Long straight wire Circular coil Long solenoid.
Chapter 28 Sources of Magnetic Field Ampère’s Law Example 28-6: Field inside and outside a wire. A long straight cylindrical wire conductor of radius.
Help Session Ch-23.
Calculating Magnetic Field due to an Electric Current
BABARIA INSTITUTE OF TECHNOLOGY ELECTRONICS & COMMUNICATION DEPARTMENT
Two questions: (1) How to find the force, F on the electric charge, q excreted by the field E and/or B? (2) How fields E and/or B can be created?
Ampère’s Law Figure Arbitrary path enclosing a current, for Ampère’s law. The path is broken down into segments of equal length Δl.
The Torque on a Current-Carrying Coil
WEEK 4 Day 1 Magnetic field
Magnetic Fields due to Currents
Ampère’s Law Figure Arbitrary path enclosing a current, for Ampère’s law. The path is broken down into segments of equal length Δl.
Magnetic Field produced by current
Magnetism From Electricity
Two questions: (1) How to find the force, F on the electric charge, q excreted by the field E and/or B? (2) How fields E and/or B can be created?
Flux density produced by a long coil (solenoid)
Applications of Ampere’s Law
Two long parallel conductors are separated by 1. 0 m
Magnetic Field produced by current
Chapter 32 Problems 6,7,9,16,29,30,31,37.
Chapter 31 Problems 2,5,13,20.
Presentation transcript:

Magnetic Fields Due to Currents JH CH29.Problems Magnetic Fields Due to Currents JH

Suggested Problems

47. The current density j inside a long, solid, cylindrical wire of radius a = 3.1 mm is in the direction of the central axis, and its magnitude varies linearly with radial distance r from the axis according to J = J0r/a, where J0 =310 A/m2. Find the magnitude of the magnetic field at (a) r = 0, (b) r = a/2, and (c) r= a. Answer: (a) 1.0x10-7 T = 0.10 uT ; (b) 4.0x10-7 T = 0.40 uT  

53. A long solenoid has 100 turns/cm and carries current i 53. A long solenoid has 100 turns/cm and carries current i. An electron moves within the solenoid in a circle of radius 2.30 cm perpendicular to the solenoid axis. The speed of the electron is 0.0460c (c = speed of light). Find the current i in the solenoid. Answer: 0.27200 A

56. Figure 29-71 shows an arrangement known as a Helmholtz coil 56. Figure 29-71 shows an arrangement known as a Helmholtz coil. It consists of two circular coaxial coils, each of 200 turns and radius R = 25.0 cm, separated by a distance s = R. The two coils carry equal currents i =12.2 mA in the same direction. Find the magnitude of the net magnetic field at P, midway between the coils. Answer: 8.76x10-6 T = 8.76 uT