Wed. Mar. 26, 2008Physics 208, Lecture 171 Exam 2 covers Ch. 27-32, Lecture, Discussion, HW, Lab Chapter 27: Electric flux & Gauss’ law Chapter 29: Electric.

Slides:



Advertisements
Similar presentations
Sources of the Magnetic Field
Advertisements

Lecture 8 Examples of Magnetic Fields Chapter 19.7  Outline Long Wire and Ampere’s Law Two Parallel Contours Solenoid.
Physics 2102 Lecture 15 Biot-Savart Law Physics 2102 Jonathan Dowling Jean-Baptiste Biot ( ) Felix Savart (1791–1841)
Chapter 30 Sources of the magnetic field
Chapter 27 Sources of the magnetic field
Chapter 32 Magnetic Fields.
Chapter 22 Magnetism.
Phy 213: General Physics III Chapter 29: Magnetic Fields to Currents Lecture Notes.
Sources of Magnetic Field Chapter 28 Study the magnetic field generated by a moving charge Consider magnetic field of a current-carrying conductor Examine.
Dale E. Gary Wenda Cao NJIT Physics Department
Sources of Magnetic Field What are some sources of Magnetic Field? Moving Point Charges: Current Elements (Biot-Savart Law): points from source to field.
Ampere’s Law Physics 102 Professor Lee Carkner Lecture 18.
EEE340Lecture 221 Note that the correspondences between fields and circuits are: But and I are governed by Ampere’s circuital law in 90 o. According to.
K L University 1. 2 MAGNETOSTATICS 3 Introduction to Magneto statics – Magnetic field, Magnetic force, Magnetic flux Biot-Savat’s law -- Applications.
Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com.
Sources of Magnetic Field
Chapter 29. Magnetic Field Due to Currents What is Physics? Calculating the Magnetic Field Due to a Current Force Between Two Parallel.
Ampere’s Law AP Physics C Mrs. Coyle Andre Ampere.
The story so far… dB r dI Magnetic field generated by current element: Biot-Savart I Ampere’s law closed path surface bounded by path.
Magnetic Forces and Fields. Magnetic Force Right Hand Rule: Cross Product.
AP Physics C Montwood High School R. Casao
Magnetic Sources The Biot-Savart Law
Sources of the Magnetic Field
Magnetic Field and Magnetic Forces
Chapter 20 The Production and Properties of Magnetic Fields.
Magnetism 1. 2 Magnetic fields can be caused in three different ways 1. A moving electrical charge such as a wire with current flowing in it 2. By electrons.
Copyright © 2007 Pearson Education, Inc., publishing as Pearson Addison-Wesley PowerPoint ® Lecture prepared by Richard Wolfson Slide Magnetism:
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.
Gauss’ Law for magnetic fields There are no magnetic “charges”.
Lecture 29: WED 25 MAR Magnetic Fields Due to Currents II
1 Exam 2 covers Ch , Lecture, Discussion, HW, Lab Chapter 27: Electric flux & Gauss’ law Chapter 29: Electric potential & work Chapter 30: Electric.
Physics 202, Lecture 13 Today’s Topics Magnetic Forces: Hall Effect (Ch. 27.8) Sources of the Magnetic Field (Ch. 28) B field of infinite wire Force between.
30.5 Magnetic flux  30. Fig 30-CO, p.927
Chapter 19 (part 2) Magnetism. Hans Christian Oersted 1777 – 1851 Best known for observing that a compass needle deflects when placed near a wire carrying.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 22 Physics, 4 th Edition James S. Walker.
Review Problem Review Problem Review Problem 3 5.
Fundamental Physics II PETROVIETNAM UNIVERSITY FACULTY OF FUNDAMENTAL SCIENCES Vungtau, 2013 Pham Hong Quang
Lecture 16 Magnetism (3) History 1819 Hans Christian Oersted discovered that a compass needle was deflected by a current carrying wire Then in 1920s.
1 Exam 2 covers Ch , Lecture, Discussion, HW, Lab Chapter 27: The Electric Field Chapter 29: Electric potential & work Chapter 30: Electric potential.
Physics 2102 Magnetic fields produced by currents Physics 2102 Gabriela González.
Magnetic Fields Due to Currents
Exam 2 covers Ch , Lecture, Discussion, HW, Lab
Sources of the Magnetic Field March 23, 2009 Note – These slides will be updated for the actual presentation.
Lecture 28: MON 23 MAR Magnetic Fields Due to Currents: Biot-Savart Law Physics 2113 Jonathan Dowling Jean-Baptiste Biot ( ) Felix Savart (1791–1841)
Physics Sources of the Magnetic Field 30.1 Biot-Savart Law 30.2 Force between two parallel wires 30.3 Ampere’s Law 30.4 Magnetic Field (B) of.
Chapter 28 and 29 Hour 1: General introduction, Gauss’ Law Magnetic force (28.1) Cross product of vectors. Hour 2: Currents create B Fields: Biot-Savart,
1 Exam 2 covers Ch , Lecture, Discussion, HW, Lab Chapter 27: The Electric Field Chapter 29: Electric potential & work Chapter 30: Electric potential.
Lecture 17: THU 18 MAR 10 Ampere’s law Physics 2102 Jonathan Dowling André Marie Ampère (1775 – 1836)
22.7 Source of magnetic field due to current
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.
Lecture 28: Currents and Magnetic Field: I
Applications of Ampere’s Law
Applied Physics Lecture 14 Electricity and Magnetism Magnetism
Physics 212 Lecture 14, Slide 1 Physics 212 Lecture 14 Biot-Savart Law :05.
Sources of the Magnetic Field March 22, MarBREAK 1120-MarMagnetic FieldSources of B 1227-MarAmpere’s LawFaraday's LawFaraday’s Law 133-AprInductance.
Quiz 1 Borderline Trouble Deep Trouble.
Ph126 Spring 2008 Lecture #8 Magnetic Fields Produced by Moving Charges Prof. Gregory Tarl é
Last Time Magnetic Force Motors and Generators Gauss' Law 1.
Chapter 29. Magnetic Field Due to Currents What is Physics? Calculating the Magnetic Field Due to a Current Force Between Two Parallel.
Right-hand Rule 2 gives direction of Force on a moving positive charge Right-Hand Rule Right-hand Rule 1 gives direction of Magnetic Field due to current.
AP Physics ST Biot-Savart Law tutornext.com. Biot-Savart Law Shortly after Oersted discovered connection between a current-carrying wire and a magnetic.
The Biot-Savart Law. Biot and Savart recognized that a conductor carrying a steady current produces a force on a magnet. Biot and Savart produced an equation.
Lecture 9 Magnetic Fields due to Currents Ch. 30 Cartoon - Shows magnetic field around a long current carrying wire and a loop of wire Opening Demo - Iron.
Lecture 23: WED 11 MAR Ampere’s law Physics 2102 Jonathan Dowling André Marie Ampère (1775 – 1836)
Sources of the Magnetic Field
Exam 2 is Tuesday Oct. 27 5:30-7 pm, Birge 145
Lecture 9 Magnetic Fields due to Currents Ch. 30
Exam 3 covers Lecture, Readings, Discussion, HW, Lab
Exam 2 covers Ch , Lecture, Discussion, HW, Lab
Last time… RC circuits Magnetic fields Magnetic dipole torque
Presentation transcript:

Wed. Mar. 26, 2008Physics 208, Lecture 171 Exam 2 covers Ch , Lecture, Discussion, HW, Lab Chapter 27: Electric flux & Gauss’ law Chapter 29: Electric potential & work Chapter 30: Electric potential & field Chapter 28: Current & Conductivity Chapter 31: Circuits Chapter 32: Magnetic fields & forces (exclude 32.6,32.8,32.10) Exam 2 is Wed. Mar. 26, 5:30-7 pm, 2103 Ch: Adam(301,310), Eli(302,311), Stephen(303,306), 180 Science Hall: Amanda(305,307), Mike(304,309), Ye(308)

Wed. Mar. 26, 2008Physics 208, Lecture 172 Electric current produces magnetic field Current (flow of electric charges ) in wire produces magnetic field. That magnetic field aligns compass needle Current Magnetic field

Wed. Mar. 26, 2008Physics 208, Lecture 173 Law of Biot-Savart Each element of current produces a contribution to the magnetic field. r  I dsds B out of page dIdI dBdB r

Wed. Mar. 26, 2008Physics 208, Lecture 174 Magnetic field from long straight wire: Direction What direction is the magnetic field from an infinitely-long straight wire? I x y

Wed. Mar. 26, 2008Physics 208, Lecture 175 Current dependence How does the magnitude of the B-field change if the current is doubled? I x y A)Is halved B)Quadruples C)Stays same D)Doubles E)Is quartered

Wed. Mar. 26, 2008Physics 208, Lecture 176 Distance dependence How does the magnitude of the B-field at 2 compare to that at 1? I x y 1 2 A)B 2 =B 1 B)B 2 =2B 1 C)B 2 =B 1 /2 D)B 2 =4B 1 E)B 2 =B 1 /4

Wed. Mar. 26, 2008Physics 208, Lecture 177 Why? Biot-Savart says Why B(r)  1/r instead of 1/r 2 ? Large contribution from this current element. Decreases as 1/r 2 I Small contribution from this current element. ~ independent of r

Wed. Mar. 26, 2008Physics 208, Lecture 178 Long straight wire All current elements produce B out of page x a r  Add them all up:

Wed. Mar. 26, 2008Physics 208, Lecture 179 Forces between currents Which of these pairs of currents will attract each other? A. A B. A & C C. B D. A & B ABC

Wed. Mar. 26, 2008Physics 208, Lecture 1710 Force between current-carrying wires Attractive for parallel currents. Repulsive for antiparallel currents

Wed. Mar. 26, 2008Physics 208, Lecture 1711 Field from a circular loop Each current element produce dB All contributions add as vectors Along axis, all components cancel except for x-comp

Wed. Mar. 26, 2008Physics 208, Lecture 1712 Magnetic field from loop Which of these graphs best represents the magnetic field on the axis of the loop? BzBz z x y BzBz BzBz BzBz A. B. C. D. z z z z

Wed. Mar. 26, 2008Physics 208, Lecture 1713 Magnetic field from a current loop One loop: field still loops around the wire. Many loops: same effect

Wed. Mar. 26, 2008Physics 208, Lecture 1714 Solenoid electromagnet Sequence of current loops can produce strong magnetic fields. This is an electromagnet

Wed. Mar. 26, 2008Physics 208, Lecture 1715 Comparing Electric, Magnetic Biot-Savart: calculate B-field from current distribution. Resulting B-field is a vector, and… complication: current (source) is a vector! Coulomb: calculate E-field from charge distribution Resulting E is a vector but charge (source) is not a vector

Wed. Mar. 26, 2008Physics 208, Lecture 1716 A shortcut: Ampere’s law Integral around closed path proportional to current passing through any surface bounded by path. Ampere’s law closed path surface bounded by path I Right-hand ‘rule’: Thumb in direction of positive current Curled fingers show direction integration

Wed. Mar. 26, 2008Physics 208, Lecture 1717 ‘Testing’ Ampere’s law Long straight wire, B  r r I B(r)B(r) B||ds path has constant r path length = 2 π r Circular path Surface bounded by path

Wed. Mar. 26, 2008Physics 208, Lecture 1718 Using Ampere’s law Could have used Ampere’s law to calculate B r I B(r)B(r) Circular path Surface bounded by path B||ds B constant on path path length = 2 π r

Wed. Mar. 26, 2008Physics 208, Lecture 1719 Quick Quiz Suppose the wire has uniform current density. How does the magnetic field change inside the wire? A.Increases with r B.Decreases with r C.Independent of r D.None of the above r B

Wed. Mar. 26, 2008Physics 208, Lecture 1720 Building a solenoid

Wed. Mar. 26, 2008Physics 208, Lecture 1721 Ampere’s law for the solenoid