Physics for Scientists and Engineers II, Summer Semester 2009 1 Lecture 12: June 17 th 2009 Physics for Scientists and Engineers II.

Slides:



Advertisements
Similar presentations
Magnetic Field due to a Current-Carrying Wire Biot-Savart Law
Advertisements

Sources of the Magnetic Field
The Magnetic Force Between Two Parallel Conductors AP Physics C Montwood High School R. Casao.
Lecture 8 Examples of Magnetic Fields Chapter 19.7  Outline Long Wire and Ampere’s Law Two Parallel Contours Solenoid.
Lecture 20 – Forces on Currents 26.6 Magnetic Forces on Current Carrying Conductors.
THE MAGNETIC FORCE BETWEEN TWO PARALLEL CONDUCTORS Lecture No.12 By. Sajid Hussain Qazi.
Today’s Concept: What Causes Magnetic Fields
Unit 4 Day 8 – Ampere’s Law & Magnetic Fields thru Solenoids & Toroids Definition of Current Ampere’s Law Magnetic Field Inside & Outside a Current Carrying.
Phy 213: General Physics III Chapter 29: Magnetic Fields to Currents Lecture Notes.
Physics 121 Practice Problem Solutions 10 Magnetic Fields from Currents (Biot-Savart and Ampere’s Law) Contents: 121P10 - 1P, 5P, 8P, 10P, 19P, 29P,
The unit of the magnetic field B (the Tesla) A] is the same as the electric field times a velocity B] is the same as the electric field divided by a velocity.
Lecture 21 Today Magnetic forces and Torques The Biot-Savart Law Magnetic force between two parallel conductors Maxwell’s magnetic potential.
Physics for Scientists and Engineers II, Summer Semester Lecture 8: June 8 th 2009 Physics for Scientists and Engineers II.
III–2 Magnetic Fields Due to Currents.
Lecture 8b – Sources of Magnetic Field
Physics for Scientists and Engineers II, Summer Semester 2009 Lecture 6: June 1 st 2009 Physics for Scientists and Engineers II.
Physics 121: Electricity & Magnetism – Lecture 10 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Ampere’s Law Physics 102 Professor Lee Carkner Lecture 18.
Physics for Scientists and Engineers II, Summer Semester Lecture 29: August 5 th 2009 Physics for Scientists and Engineers II.
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?
Physics for Scientists and Engineers II, Summer Semester Lecture 13: June 19 th 2009 Physics for Scientists and Engineers II.
Physics for Scientists and Engineers II, Summer Semester Lecture 11: June 15 th 2009 Physics for Scientists and Engineers II.
Electromagnet. Wire Field  A moving charge generates a magnetic field. Symmetry with experiencing force Perpendicular to direction of motion Circles.
AP Physics C Chapter 28.  s1/MovingCharge/MovingCharge.html s1/MovingCharge/MovingCharge.html.
Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com.
Today’s agenda: Magnetic Fields Due To A Moving Charged Particle. You must be able to calculate the magnetic field due to a moving charged particle. Biot-Savart.
Lecture 9 Magnetic Fields due to Currents Chp. 30 Cartoon - Shows magnetic field around a long current carrying wire and a loop of wire Opening Demo -
Ampere’s Law AP Physics C Mrs. Coyle Andre Ampere.
The magnetic force law (Lorentz law) The magnitude of the force is the B field x the perpendicular velocity x charge Or The velocity x the perpendicular.
Magnetic Forces and Fields. Magnetic Force Right Hand Rule: Cross Product.
Chapter 29 Magnetic Fields Due to Currents In this chapter we will explore the relationship between an electric current and the magnetic field it generates.
Sources of the Magnetic Field
Van Allen Radiation Belts The Van Allen radiation belts consist of charged particles surrounding the Earth in doughnut-shaped regions. The particles are.
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.
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.
Review Problem Review Problem Review Problem 3 5.
Fundamental Physics II PETROVIETNAM UNIVERSITY FACULTY OF FUNDAMENTAL SCIENCES Vungtau, 2013 Pham Hong Quang
CHECKPOINT: What is the current direction in this loop
Lecture 16 Magnetism (3) History 1819 Hans Christian Oersted discovered that a compass needle was deflected by a current carrying wire Then in 1920s.
Advanced Higher Physics Unit 2 Electromagnetism. Magnetic Field A current carrying conductor exerts a magnetic field. The strength of this field is measured.
Magnetic Fields Chapter Sources of the Magnetic Field The magnetic field of moving charges The magnetic field of currents Biot-Savart law Last.
Unit 4 Day 7: Magnetic Fields due to Wires Magnetic Field in a Straight Wire Magnetic Fields in 2 Parallel Conducting Wires, Side by Side Magnetic Forces.
Electricity & Magnetism Seb Oliver Lecture 14: Biot-Savart Law.
DC MOTOR PRINCIPLE Magnetic Force. M OTOR P RINCIPLE  When a straight wire carrying a current is placed in an external magnetic field, the interaction.
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?
Chapter 26 Sources of Magnetic Field. Biot-Savart Law (P 614 ) 2 Magnetic equivalent to C’s law by Biot & Savart . P. P Magnetic field due to an infinitesimal.
Lecture 28: Currents and Magnetic Field: I
20 Magnetic Field & Forces. Magnetism S N S N Extended…
Biot-Savart Law Biot-Savart law: The constant  o is called the permeability of free space  o = 4  x T. m / A.
Applications of Ampere’s Law
Physics 212 Lecture 14, Slide 1 Physics 212 Lecture 14 Biot-Savart Law :05.
PHY 112 (SECTION 001 ) Lecture 12,13 Chapter 28 of R Haliday Book.
More Examples of Magnetic Flux Biot-Savart Law Ampère’s Law.
Lecture 15-1 What we learned from last class Define magnetic dipole moment by where n is normal to the loop with RHR along I. Hall effect:  Determines.
Week 9 Presentation 1 Electromagnets 1. Learning Objectives: 1. Determine the magnitude and direction of the magnetic field strength generated by a straight.
Chapter 29. Magnetic Field Due to Currents What is Physics? Calculating the Magnetic Field Due to a Current Force Between Two Parallel.
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?
Ampere’s Law Basic Premise Elementary application.
Magnetic Field due to a Current-Carrying Wire Biot-Savart Law
Magnetic Field due to a Current-Carrying Wire Biot-Savart Law
Magnetic Fields Due To A Moving Charged Particle.
C Top view Side view (28 – 13).
CHECKPOINT: What is the current direction in this loop
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?
Applications of Ampere’s Law
Force acting between two long, parallel, current-carrying conductors
Two long parallel conductors are separated by 1. 0 m
Electricity & Magnetism
Chapter 30 Examples 4,8.
Presentation transcript:

Physics for Scientists and Engineers II, Summer Semester Lecture 12: June 17 th 2009 Physics for Scientists and Engineers II

Physics for Scientists and Engineers II, Summer Semester The Hall Effect d t y x z + - When positive charge carriers contribute to current I: Positive charges are deflected up. When negative charge carriers contribute to current I: Negative charges are deflected up.

Physics for Scientists and Engineers II, Summer Semester The Hall Effect (for Positive Charge Carriers) d t y x z

Physics for Scientists and Engineers II, Summer Semester The Hall Effect – what you can get from it.

Physics for Scientists and Engineers II, Summer Semester History

Physics for Scientists and Engineers II, Summer Semester The Biot-Savart Law

Physics for Scientists and Engineers II, Summer Semester An Example: Calculate the Magnetic Field at the Center of a Circular Conductor Carrying a Current I x y z

Physics for Scientists and Engineers II, Summer Semester An Example: Calculate the Magnetic Field at the Center of a Semicircular Conductor Carrying a Current I x y z Infinitely long straight sections

Physics for Scientists and Engineers II, Summer Semester An Example: Calculate the Magnetic Field at Point P x y z

Physics for Scientists and Engineers II, Summer Semester An Example:

Physics for Scientists and Engineers II, Summer Semester An Example: Calculate the Magnetic Field at Point P x y z

Physics for Scientists and Engineers II, Summer Semester Magnetic Force Between Two Parallel Conductors

Physics for Scientists and Engineers II, Summer Semester Now Place a Second Current Parallel to it…..

Physics for Scientists and Engineers II, Summer Semester Or, the force on the first wire…..

Physics for Scientists and Engineers II, Summer Semester The Definition of 1 Ampere When the magnitude of the force per unit length between two long, parallel wires that carry identical currents and are separated by 1m is 2x10 -7 N/m, the current in each wire is defined to be 1 A.

Physics for Scientists and Engineers II, Summer Semester Ampere’s Law Top View

Physics for Scientists and Engineers II, Summer Semester Ampere’s Law Top View

Physics for Scientists and Engineers II, Summer Semester Ampere’s Law