AP Physics C Magnetic Fields and Forces. Currents Set up Magnetic Fields First Right-Hand Rule Hans Christian Oersted (1777-1851)

Slides:



Advertisements
Similar presentations
Magnetic Force Acting on a Current-Carrying Conductor
Advertisements

Chapter 22 Magnetism.
Magnetic Fields and Forces
Chapter 26: The Magnetic Field
Magnetism and Currents. A current generates a magnetic field. A magnetic field exerts a force on a current. Two contiguous conductors, carrying currents,
Many historians of science believe that the compass, which uses a magnetic needle, was used in China as early as the 13th century BC, its invention being.
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.
Chapter 19 Magnetism Conceptual questions: 5,6,8,14,16
Chapter 22 Magnetism AP Physics B Lecture Notes.
Chapter 20 Magnetism.
Magnetism Review and tid-bits. Properties of magnets A magnet has polarity - it has a north and a south pole; you cannot isolate the north or the south.
Chapter 28. Magnetic Field
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 19: Magnetic Forces and Fields.
Ch 20 1 Chapter 20 Magnetism © 2006, B.J. Lieb Some figures electronically reproduced by permission of Pearson Education, Inc., Upper Saddle River, New.
Magnetic Fields and Forces AP Physics B. Facts about Magnetism Magnets have 2 poles (north and south) Like poles repel Unlike poles attract Magnets create.
Magnetism! Chapter 19.
Magnetism and Electromagnetic Induction
When a charged particle moves through a magnetic field, the direction of the magnetic force on the particle at a certain point is Q in the direction.
Chapter 22 Magnetism.
Magnetic Fields Faraday’s Law
Magnetic Field and Magnetic Forces
Magnetism July 2, Magnets and Magnetic Fields  Magnets cause space to be modified in their vicinity, forming a “ magnetic field ”.  The magnetic.
Copyright © 2009 Pearson Education, Inc. Lecture 8 - Magnetism.
Magnetic Fields and Forces
Chapter 21.  Magnets, as you know, can exert forces on one another.  In electricity, we talk about negative and positive dipoles or charges.  In magnetism,
 Magnets can be created one of two ways: Naturally found in the Earth. They are called lodestones. It is permanently magnetized. Using electricity to.
Copyright © 2009 Pearson Education, Inc. Chapter 26 DC Circuits.
Whiteboard Warmup! A beam of electrons is being fired to the right, when a magnet is pointed toward the beam and brought closer. As a result, the beam.
Magnetism Magnetic materials have the ability to attract or repel other types of magnetic materials. But not all materials are magnetic.
Lecture Outline Chapter 19 College Physics, 7 th Edition Wilson / Buffa / Lou © 2010 Pearson Education, Inc.
When a current-carrying loop is placed in a magnetic field, the loop tends to rotate such that its normal becomes aligned with the magnetic field.
Chapter 29 Magnetism Ferromagnetism
Magnetic Fields and Currents The crossover between topics.
Chapter 26 Magnetism Poles – Location where the magnetic effect is the strongest –North pole – pole of a freely suspended magnet which points towards geographic.
Fields Model used when force act a distance. Quantity / unit measure.
Today4/9 Lab “Current Balance” Right Hand Rule for:
Chapter 21 Magnetic Forces and Magnetic Fields Magnetic Fields The needle of a compass is permanent magnet that has a north magnetic pole (N) at.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 22 Physics, 4 th Edition James S. Walker.
Review Problem Review Problem Review Problem 3 5.
P212c28: 1 Chapter 28: Magnetic Field and Magnetic Forces Iron ore found near Magnesia Compass needles align N-S: magnetic Poles North (South) Poles attracted.
Magnets and the magnetic field Electric currents create magnetic fields Magnetic fields of wires, loops, and solenoids Magnetic forces on charges and currents.
Chapter 28: Magnetic Fields Introduction What are we going to talk about in chapter 29: What are magnetic fields intensity (B)? How do we create magnetic.
A permanent magnet has a north magnetic pole and a south magnetic pole. Like poles repel; unlike poles attract.
Chapter 20 Magnetism. Units of Chapter 20 Magnets and Magnetic Fields Electric Currents Produce Magnetic Fields Force on an Electric Current in a Magnetic.
Electric Currents and Magnetic Fields. History Lodestones were discovered 2000 years ago and were magnetic. They were named after Magnesia which is a.
Magnetic Forces and Magnetic Fields
S-133 What do the following terms mean 1.Magnetism 2.Electromagnetic induction 3.Dipole.
1 Chapter 19: Magnetism The nature of magnetism Iron ore found near Magnesia Compass needles align N-S: magnetic Poles North (South) Poles attracted to.
Magnetism. Magnets, Magnetic Poles, and Magnetic Field Direction Magnets have two distinct types of poles; we refer to them as north and south.
Magnetic Fields and Forces AP Physics B. Facts about Magnetism Magnets have 2 poles (north and south) Like poles repel Unlike poles attract Magnets create.
Ch Magnetic Forces and Fields
Chapter 19: Magnetism Magnets  Magnets Homework assignment : 18,25,38,45,50 Read Chapter 19 carefully especially examples.
Chapter 20 Magnetism Magnets and Magnetic Fields Magnets have two ends – poles – called north and south. Like poles repel; unlike poles attract.
Lecture 27 Magnetic Fields: II
Magnetic Field and Magnetic Forces
A permanent magnet has a north magnetic pole and a south magnetic pole. Like poles repel; unlike poles attract.
Chapter 20 Magnetism Magnetism 20 Phy 2054 Lecture Notes.
PHY 102: Lecture Magnetic Field 6.2 Magnetic Force on Moving Charges 6.3 Magnetic Force on Currents 6.4 Magnetic Field Produced by Current.
Physics Chapter 21: Magnetism. ☺Magnets ☺Caused by the Polarization of Iron Molecules ☺Material Containing Iron (Fe)
Chapter 21 Magnetic Forces and Magnetic Fields Magnetic Fields The needle of a compass is permanent magnet that has a north magnetic pole (N) at.
Nighttime exam? If we have the exam in the evening of July 3 rd, we would cancel class on July 5 th and you get a long weekend. Would you prefer to have.
Magnets have two ends – poles – called north and south. Like poles repel; unlike poles attract. If you cut a magnet in half, you don’t get a north pole.
Solar Magnetic Fields. Capacitors in Circuits Charge takes time to move through wire  V is felt at the speed of light, however Change in potential across.
PHY 102: Lecture Magnetic Field
Phys102 Lecture 13, 14, 15 Magnetic fields
Unit 9: Electromagnetism
Unit 10: Magnetism Pre-AP Physics.
Active Figure 29.1 Compass needles can be used to trace the magnetic field lines in the region outside a bar magnet.
Magnetic Fields and Forces
Magnetic Fields and Forces
Presentation transcript:

AP Physics C Magnetic Fields and Forces

Currents Set up Magnetic Fields First Right-Hand Rule Hans Christian Oersted ( )

Right-Hand Rule for Magnetic Fields x: into the page or away from you · out of the page or towards you

Magnetic Field of a Current Loop:

Another look a Magnetic Fields of a Current Loop:

Electron as a Magnetic Dipole The electron spins on its axis, giving rise to a electron current in the direction of rotation. The electron is like a magnetic dipole, a miniature magnet, with a north end and a south end.

Magnetic Spin Dipoles in Iron

Dual polarity Cutting a magnet in half will not isolate a single north or south. One magnet becomes two, then four, and so on. This process will never end; even when the last electron spin dipole is reached, it cannot be cut to reveal a single north or single south pole.

Magnetic Fields of a Bar Magnet & the Earth B-field of bar magnet is similar to the Earth's magnetic field. B-field lines leave north face, enter at south face. Convection currents inside the earth set up magnetic field.

Bar Magnets If magnetic dipole loops are oriented the same on neighboring faces, the magnets attract. North is attracted to south, and is repelled by north.

Compass Needle is a Magnet: It Aligns with the B-Field

Magnetic Force on Current-Carrying Wire F = ILB sin θ The direction of the force on the wire may be determined by a second right-hand rule, a right hand rule for magnetic force. The other right-hand rule gave the direction of the magnetic field B.

Using the Right-Hand Rule To determine the direction of the magnetic force acting on the current-bearing wire

Using the RHR: In which direction, if any, will the metal rod be deflected?

Sample Problem A wire 2.80 m in length carries a current of 5.00 A in a region where a uniform magnetic field has a magnitude of T. Calculate the magnitude of the magnetic force on the wire if the angle between the magnetic field and the current is 60.0 degrees.

Sample Problem A thin, horizontal copper rod 1.0 m long and has a mass of 50 g. What is the minimum current in the rod that will cause it to float in a horizontal magnetic field that is perpendicular to the rod of 2.0 T?

Torque on a Current Loop What is the net force on the current loop? What is the net torque on the loop?

Torque on the Current Loop At what angle is the torque a maximum value? At what angle is the torque a minimum value?

Sample Problem A circular loop of radius 2.0 cm contains 50 turns of tightly wound wire. If the current in the windings is 0.30 A and a constant magnetic field of 0.20 T makes an angle of 25 degrees with a vector perpendicular with the loop, what torque acts on the loop?

DC Motor

Moving Charges in a B-Field: Electric force can be parallel to direction of velocity, but the magnetic force is always perpendicular to the velocity vector.

Magnetic Force on Moving Charges RHR F = qvB sin θ

Magnetic Force on Moving Charges If the velocity v is parallel to the magnetic field B, the magnetic force is zero because sin θ = 0.

Magnetic Force on Moving Charges What is the direction of the magnetic force on the moving charge in each situation?

Magnetic Force on Moving Charges What is the direction of the force F, if any, in each case?

Charges move in a circular path:

Circular Paths in Magnetic Fields

Circular Motion in B-Field Right Hand Rule for Force Fingers point in direction of magnetic field B. Thumb points in direction of the velocity vector v. Palm shows the direction of the force F.

Mass Spectrometer F = qvB sin θ θ = 90 deg F = qvB F = ma a = v 2 /r F = mv 2 /r qvB = mv 2 /r m = qBr/v

Sample Problem A singly charged positive ion moving at 4.6 x 10 5 m/s leaves a circular track of radius 7.94 mm along a direction perpendicular to the 1.80 T magnetic field of a bubble chamber. Compute the mass (in amus) of this ion, and identify it from that value.

Velocity Selector & Mass Spectrometer In the velocity selector, the E-force and the B-force are equal and opposite, so that, qE = qvB. Therefore, v = E/B. In 1897, J. J. Thomson used this set-up to determine the mass to charge ratio for electrons.

Sample Problem The electric field between the plates of a velocity selector is 2500 V/m, and the magnetic field in both the velocity selector and the deflection chamber has a magnitude of T. Calculate the radius of the path of a singly charged ion have a mass of 2.18 x kg.

Electron Beam in a B-Field Electrons are deflected downward. What is the direction of the magnetic field B?

Magnetic Flux Magnetic flux is the product of the average magnetic field times the perpendicular area that it penetrates.magnetic field

Magnetic Flux Illustrations The contribution to magnetic flux for a given area is equal to the area times the component of magnetic field perpendicular to the area. For a closed surface, the sum of magnetic flux is always equal to zero (Gauss' law for magnetism).magnetic fluxGauss' law for magnetism

Gauss’s Law for Magnetism The net magnetic flux out of any closed surface is zero. This amounts to a statement about the sources of magnetic field. For a magnetic dipole, any closed surface the magnetic flux directed inward toward the south pole will equal the flux outward from the north pole. The net flux will always be zero for dipole sources.magnetic flux

Sample Problem A cube of edge length 2.50 cm is positioned so that it is position with one corner at the origin, one face in the xy- plane, one face in the yz-plane and one in the xz-plane. A uniform magnetic field given by B = (5.00i +4.00j +3.00k) T exists throughout the region. Calculate the flux through the face that is parallel to the yz- plane. What is the total flux through the six faces?