5. Magnetostatics The force is generated by the magnetic field B.

Slides:



Advertisements
Similar presentations
Electromagnetism II Week 9. Contents Bar Magnet Bar Magnet Earths Magnetic Dipole Earths Magnetic Dipole Oersteds Rule (RHR1) Oersteds Rule (RHR1) Solenoid.
Advertisements

Physics 2102 Lecture 15 Biot-Savart Law Physics 2102 Jonathan Dowling Jean-Baptiste Biot ( ) Felix Savart (1791–1841)
Copyright © 2007 Pearson Education, Inc. publishing as Addison-Wesley Goals for Chapter 20 To observe and visualize magnetic fields and forces. To study.
Magnetostatics Magnetostatics is the branch of electromagnetics dealing with the effects of electric charges in steady motion (i.e, steady current or DC).
Magnetic Field and Magnetic Forces
23-1 Physics I Class 23 Magnetic Force on Moving Charges.
Dr. Jie ZouPHY Chapter 30 Sources of the Magnetic Field.
Motors Lecture Hans Christian Oersted (1777 – 1851) Ref:
Problem 2 Find the torque about the left hand segment on the loop as a function of θ, the angle the plane makes with the horizontal plane.
In the circuit below, suppose the switch has been in position A for a very long time. If it is then switched to B at t=0, find the current as a function.
The Electric and Magnetic fields Maxwell’s equations in free space References: Feynman, Lectures on Physics II Davis & Snyder, Vector Analysis.
Physics 152 Magnetism Walker, Chapter B Field Outside a Wire Earlier we said that magnetic fields are created by moving charges. A current in a.
General Physics 2Magnetism1 E9 – Currents Create Magnetic Fields A moving charge creates a magnetic field Superposition principle for a wire segment Biot-Savart.
§5.2: Biot-Savart Law Christopher Crawford PHY
Period 2. What is magnetic declination??? A) Magnetic declination is the angle between you and Earth when you are standing on a level surface. B) Magnetic.
Sources of Magnetic Field
26. Magnetism: Force & Field. 2 Topics The Magnetic Field and Force The Hall Effect Motion of Charged Particles Origin of the Magnetic Field Laws for.
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.
MAGNETISM Percorso CLIL V B Linguistico Prof.sse M.Castracane e M.V.De Nigris a.s. 2014/2015.
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.
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.
Chapter 19 Magnetism 1. Magnets 2. Earth’s Magnetic Field 3. Magnetic Force 4. Magnetic Torque 5. Motion of Charged Particles 6. Amperes Law 7. Parallel.
Van Allen Radiation Belts The Van Allen radiation belts consist of charged particles surrounding the Earth in doughnut-shaped regions. The particles are.
Review Problem Review Problem Review Problem 3 5.
Chapter 5 Magnetostatics 5.1 The Lorentz Force Law 5.2 The Biot-Savart Law 5.3 The Divergence and Curl of 5.4 Magnetic Vector Potential.
Lecture 16 Magnetism (3) History 1819 Hans Christian Oersted discovered that a compass needle was deflected by a current carrying wire Then in 1920s.
Physics 2102 Magnetic fields produced by currents Physics 2102 Gabriela González.
5.3 Divergence and Curl of B Ampere’s law differential form.
Moving Electrical Charge Magnetic Field Moving Electrical Charge The Hall Effect The net torque on the loop is not zero. Hall coefficient magnetic dipole.
Electricity and magnetism
講者: 許永昌 老師 1. Contents ( 起 )Discovering magnetism Compass needle : a probe of Magnetic field ( 承 )Moving charge is the source of magnetic field ( 轉 )The.
Magnetism (3, Review). Like poles repel Unlike poles attract.
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,
Electricity & Magnetism Seb Oliver Lecture 14: Biot-Savart Law.
Magnetic Fields. MAGNETOSTATICS Magnetic Fields Fundamental Postulates of Magnetostatics in Free Space.
Magnetism: Force and Field. General Characteristics Like poles repel Unlike poles attract You can never isolate a north pole from a south pole. N S N.
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
Biot-Savart Law Biot-Savart law: The constant  o is called the permeability of free space  o = 4  x T. m / A.
O Aim of the lecture  Calculation of Magnetic Fields Biot-Savart Law Magnetic field, B  Ampres Law B field Case of static E field o Main learning outcomes.
Magnetism -the attraction of a magnet for another object -two magnets will either attract or repel each other -if the domain inside a magnet are aligned.
Week 9 Presentation 1 Electromagnets 1. Learning Objectives: 1. Determine the magnitude and direction of the magnetic field strength generated by a straight.
Last time Gauss' Law: Examples (Ampere's Law) 1. Ampere’s Law in Magnetostatics The path integral of the dot product of magnetic field and unit vector.
Magnetic Field due to a Current-Carrying Wire Biot-Savart Law
Medan Magnet Gaya Magnet pada Muatan Bergerak Gaya Magnet Lorentz
Magnetic Field due to a Current-Carrying Wire Biot-Savart Law
Fundamentals of Applied Electromagnetics
Comparison of Magnetostatics and Electrostatics
Magnetic Fields Due to Currents
Electricity & Magnetism
Chapter 3a Magnetostatic
Biot-Savart Law: B field from a current
Electromagnetic Theory
C Top view Side view (28 – 13).
Chapter 5 Magnetostatics
Lecture 19 Maxwell equations E: electric field intensity
Electricity and Magnetism
Answer the Following Draw the domain of an unmagnetized bar magnet
Magnetic Fields Chapter 26 Definition of B
Electricity and Magnetism
Magnetic Fields Due to Currents
Maxwell’s equations continued
26 Magnetic Field Force on moving charge/current
Magnetic Fields Due to Currents
Sources of Magnetic Fields
CHAPTER 3 MAGNETOSTATICS.
Chapter 28 Magnetic Fields
Electricity and Magnetism
Chapter 29 Magnetic Fields Due to Currents
Presentation transcript:

5. Magnetostatics The force is generated by the magnetic field B.

Early evidence for the magnetic field.

Magnetic Field Bar magnetMagnetic field lines

Magnetic Field of the Earth Direction measured by a compass.

Oersted, in 1820What he saw.

Qersted’s experiment, modern version

Biot and Savert found that the force on a compass encircles a wire. Formulated the Biot-Savert law.

Ampere stated that all magnetic field are generated by currents. The elementary magnetic dipoles are current loops.

The force is generated by the magnetic field B. How does the field act on the moving charge? How is the field generated by the moving charges?

Total force on a charge: Lorentz’s law: Right – hand rule Magnetic force on a moving charge:

Example 5.2 – Cyclotron Motion

Cloud Chamber 1.6 MeV proton 7 MeV alpha

The Cylcotron O. E. Lawrence M. S. Livingston 1934

Magnetic Bottle

Van Allen Belts Protons and electrons from the solar wind are trapped by the earth’s magnetic field.

Currents Line current I 1 A = 1 C/s

Magnetic forces do not work!

Example 5.3 B points into the page.

Surface current density

Volume current density continuity equation:

Example 5.4

Biot-Savart Law Magnetostatics: Steady currents Magnetic field of a steady line current Permeability of free space – defines the unit Ampere

Example 5.5

Example 5.6 ?

Superposition principle for the magnetic field gives the different versions of the Biot-Savart law. line current surface current volume current Moving point charge