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Chapter 17 Lecture Magnetism Prepared by Dedra Demaree, Georgetown University © 2014 Pearson Education, Inc. Magnetism • What causes the northern lights? • How does Earth protect us from the solar wind and cosmic rays? • Are we really walking northward when we follow a compass needle? © 2014 Pearson Education, Inc. Be sure you know how to: • Use the electric field concept to explain how electrically charged objects exert forces on each other (Section 15.1). • Find the direction of the electric current in a circuit (Section 16.1). • Apply Newton's second law to a particle moving in a circle (Section 4.4). © 2014 Pearson Education, Inc. What's new in this chapter • We learned that charged objects attract and repel each other—similar to the way magnets do. – Electrically charged objects do not exhibit magnetic properties. – Are electricity and magnetism unrelated phenomena, or are they connected in some way? • We will learn about the connections between electricity and magnetism. © 2014 Pearson Education, Inc. Magnetic interaction • If you bring the like poles of two magnets near each other, they repel each other. • If you bring opposite poles near each other, they attract each other. © 2014 Pearson Education, Inc. Magnetic interaction • Magnets always have two poles. • If you break a magnet into two pieces, each piece still has two poles—a north pole and a south pole. © 2014 Pearson Education, Inc. Magnetic interaction • A compass contains a tiny magnet on a lowfriction pivot. • The north pole of a compass points toward geographic north; the south pole points toward geographic south. © 2014 Pearson Education, Inc. Magnetic interaction • Earth acts as a giant magnet, with its magnetic south pole close to its geographic north pole and its magnetic north pole close to its geographic south pole. © 2014 Pearson Education, Inc. Magnetic and electrical interactions are different • Electrically charged objects do not interact with magnets in the same way that magnets interact with magnets. • Magnetic poles are not electric charges. © 2014 Pearson Education, Inc. Magnetic field • Magnets interact without contact; we introduce the magnetic field as the mechanism behind magnetic interactions. • We can assume that a magnet produces a magnetic field—a magnetic disturbance with which other objects with magnetic properties (e.g., another magnet, anything made of iron) interact. © 2014 Pearson Education, Inc. Direction of the magnetic field • We can use a compass to detect the direction of the magnetic field at a particular location. © 2014 Pearson Education, Inc. Direction of the magnetic field © 2014 Pearson Education, Inc. Representing the magnetic field: Field lines © 2014 Pearson Education, Inc. Tip © 2014 Pearson Education, Inc. Observational experiment © 2014 Pearson Education, Inc. Observational experiment © 2014 Pearson Education, Inc. Magnetic field produced by a current • Charged objects in motion produce a magnetic field; stationary charged objects do not. • The method for determining the shape of the B field produced by the electric current in a wire is called the righthand rule. © 2014 Pearson Education, Inc. Right-hand rule for the B field © 2014 Pearson Education, Inc. Conceptual Exercise 17.1 • Draw the magnetic field lines of a solenoid connected to a battery. © 2014 Pearson Education, Inc. Current loops and bar magnets • The B field produced by the current in a loop or a coil and that produced by a bar magnet are very similar. • Wire coils with current are known as electromagnets. © 2014 Pearson Education, Inc. Magnetic force exerted by the magnetic field on a current-carrying wire • If a current-carrying wire is similar in some ways to a magnet, then a magnetic field should exert a magnetic force on a current-carrying wire similar to the force it exerts on another magnet. • A magnet sometimes pulls on a wire and sometimes does not—the effect depends on the relative directions of the B field and the current in the wire. © 2014 Pearson Education, Inc. Magnetic field of a horseshoe magnet • We use a horseshoe magnet to generate a magnetic field with almost parallel field lines between the poles. © 2014 Pearson Education, Inc. Observational experiment © 2014 Pearson Education, Inc. Observational experiment © 2014 Pearson Education, Inc. Observational experiment © 2014 Pearson Education, Inc. Right-hand rule for the magnetic force © 2014 Pearson Education, Inc. Tip © 2014 Pearson Education, Inc. Forces that current-carrying wires exert on each other • If a current-carrying straight wire produces a magnetic field, the field should exert a force on a second current-carrying straight wire placed nearby. © 2014 Pearson Education, Inc. Testing experiment © 2014 Pearson Education, Inc. Testing experiment © 2014 Pearson Education, Inc. Interaction between two current carrying coils • We can predict what happens to two currentcarrying coils of wire when the current is as shown in the figure. © 2014 Pearson Education, Inc. Tip © 2014 Pearson Education, Inc. Ampere © 2014 Pearson Education, Inc. Expression for the magnetic force that a magnetic field exerts on a current-carrying wire • Knowing the spring constant of the springs and the mass of the wire, we can use the stretch of the springs to deduce the magnitude of the magnetic force exerted on different-length wires when different currents are in them. © 2014 Pearson Education, Inc. Magnitude of the magnetic force © 2014 Pearson Education, Inc. Magnetic force exerted on a current © 2014 Pearson Education, Inc. Example 17.2 • Instead of supporting your clothesline with two poles, could you replace the poles and the clothesline with a current-carrying wire in Earth's B field, which near the surface has magnitude 5 x 10–5 T and points north? Assume that your house is located near the equator, where the B field produced by Earth is approximately parallel to Earth's surface. The clothesline is 10 m long; the clothes and the line have a mass of 2.0 kg. 1. In which direction should you orient the clothesline and which current is needed to support it? 2. Is this a promising way to support the clothesline? © 2014 Pearson Education, Inc. Summary of the differences between gravitational, electric, and magnetic forces • The gravitational and electric forces exerted on objects do not depend on the direction of motion of those objects, whereas the magnetic force does. • The forces exerted by the gravitational and electric fields are always in the direction of the g or E field, but the force exerted by the magnetic field on a current-carrying wire is perpendicular to both the B field and the electric current. © 2014 Pearson Education, Inc. The direct current electric motor • A motor is a device that converts electric energy into mechanical energy. • A simple motor consists of a rectangular currentcarrying coil placed between the poles of a large electromagnet. © 2014 Pearson Education, Inc. The direct current electric motor • A commutator causes the current to reverse each time the coil passes the vertical orientation; this is necessary for the net torque to always remain clockwise. © 2014 Pearson Education, Inc. Torque exerted on a current-carrying loop • The magnitude of the torque depends on how far from the loop's rotation axis the magnetic forces are exerted. © 2014 Pearson Education, Inc. Magnetic dipole moment • The magnetic dipole moment is the product of the current I and area A. • The direction of the dipole moment vector is perpendicular to the surface of the loop and in the direction of the B field produced by the current at the center of the loop. © 2014 Pearson Education, Inc. Using a coil in a magnetic field to measure current: An ammeter • We can use the following equation as the basis for a method to measure the current through a wire: © 2014 Pearson Education, Inc. Magnetic force exerted on a single moving charged particle • The magnetic field exerts a force on a current-carrying wire, which is made of moving electrons. – The magnetic field also exerts a force on each individual electron. – The magnetic field also exerts a force on other moving charged particles, such as protons and helium nuclei. © 2014 Pearson Education, Inc. Direction of the force that the magnetic field exerts on a moving charged particle • We can use the right-hand rule for the magnetic force to predict the direction in which electrons in the oscilloscope will be deflected. © 2014 Pearson Education, Inc. Magnitude of the force that a magnetic field exerts on a moving charged particle • We use the equation for the force a magnetic field exerts on a current-carrying wire to determine the force exerted on an individual charge: © 2014 Pearson Education, Inc. Magnitude of the force that a magnetic field exerts on a moving charged particle © 2014 Pearson Education, Inc. Right-hand rule for the direction of the magnetic force exerted on a moving charged particle © 2014 Pearson Education, Inc. Tip © 2014 Pearson Education, Inc. Quantitative Exercise 17.3 • Each of the lettered dots shown in the figure represents a small object with an electric charge +2.0 x 10–6 C moving at a speed 3.0 x 107 m/s in the directions shown. Determine the magnetic force (magnitude and direction) that a 0.10-T magnetic field exerts on each object. © 2014 Pearson Education, Inc. Circular motion in a magnetic field • The force exerted by the magnetic field always points perpendicular to the particle's velocity, toward the center of the particle's path. – The particle will move along a circular path in a plane perpendicular to the field. © 2014 Pearson Education, Inc. Cosmic rays • Cosmic rays are electrons, protons, and other elementary particles produced by various astrophysical processes, including those occurring in the Sun and sources outside the solar system. • Earth's magnetic field serves as a shield against harmful cosmic rays, causing them to deflect from their original trajectory toward Earth. © 2014 Pearson Education, Inc. Example 17.4 • Determine the path of a cosmic ray proton flying into Earth's atmosphere above the equator at a speed of 107 m/s and perpendicular to Earth's magnetic field. The average magnitude of Earth's magnetic field in this region is 5 x 10–5 T. The mass m of a proton is 10–27 kg. © 2014 Pearson Education, Inc. Tip © 2014 Pearson Education, Inc. The auroras • Charged particles moving in Earth's magnetic field follow helical paths around the magnetic field lines. © 2014 Pearson Education, Inc. The magnetic field produced by an electric current in a long straight wire • To determine the magnitude of the magnetic field at various locations near the wire, we need to place some kind of a detector of magnetic fields at different locations. © 2014 Pearson Education, Inc. Observational experiment © 2014 Pearson Education, Inc. The magnetic field produced by an electric current in a long straight wire • The magnitude of the magnetic field at a perpendicular distance r from a long straight current-carrying wire is expressed as: – The farther you move from the currentcarrying wire, the smaller the magnitude of the magnetic field. – The greater the current, the larger the magnitude of the magnetic field. © 2014 Pearson Education, Inc. Magnetic permeability • The constant μo is known as the magnetic permeability. It is used when calculating the magnetic field in a vacuum, although the value is approximately the same for air. • μ is the magnetic permeability of a substance and replaces μo if the magnetic field is being calculated inside a material. – μ for iron is approximately 1000 times larger than μo. © 2014 Pearson Education, Inc. Magnetic fields produced by different shapes of current-carrying wires © 2014 Pearson Education, Inc. Magnetic field due to electron motion in an atom • In an early model of the hydrogen atom, electron motion was depicted as a circular electric current. • The magnetic field at the center of a currentcarrying loop of radius r is: – This motion also describes a magnetic dipole moment for atoms, making this model potentially useful for explaining magnetic properties of materials. © 2014 Pearson Education, Inc. Example 17.5 • In the early 20th-century model of the hydrogen atom, the electron was thought to move in a circle of radius 0.53 x 10–10 m, orbiting once around the nucleus every 1.5 x 10–16 s. Determine the magnitude of the magnetic field produced by the electron at the center of its circular orbit and its dipole moment. © 2014 Pearson Education, Inc. Skills for analyzing magnetic processes • Problems involving magnetic interactions are of two main types: – Determine the magnetic force exerted on a current or on an individual moving charged object by the magnetic field. – Determine the magnetic field produced by a known source such as an electric current. © 2014 Pearson Education, Inc. Skills for analyzing magnetic processes • When solving problems: – Sketch the direction of the magnetic field and the current (or the velocity of a charged particle) if known. – Decide whether the magnetic field can be considered uniform in the region of interest. – Use the right-hand rule for the magnetic field if the problem is about the field of a known source. © 2014 Pearson Education, Inc. Example 17.6 • A horizontal metal wire of mass 5.0 g and length 0.20 m is supported at its ends by two very light conducting threads. The wire hangs in a 49-mT magnetic field, which points perpendicular to the wire and out of the page. The maximum force each thread can exert on the wire before breaking is 39 mN. What is the minimum current through the wire that will cause the threads to break? © 2014 Pearson Education, Inc. Example 17.7 • Determine the magnetic field 5.0 cm from a long straight wire that is connected in series with a 5.0-ohm resister and a 9.0-V battery. © 2014 Pearson Education, Inc. Intensity-modulated radiation therapy (IMRT) • An IMRT machine accelerates electrons to the desired kinetic energy, then uses a magnetic field to bend them into a target, resulting in the production of X-rays. Movable metal leaves then shape the X-ray beam to match the shape of the tumor. © 2014 Pearson Education, Inc. Example 17.8 • Estimate the magnitude of the magnetic field needed for an IMRT machine. For the estimate, assume that the electrons are moving at a speed of 2 x 108 m/s, the mass of the electrons is 9 x 10–31 kg, and the radius of the turn is 5 cm. © 2014 Pearson Education, Inc. Flow speed, electric generator, and mass spectrometer: Putting it all together • We will examine some applications that involve both magnetic and electric phenomena. – These applications involve electrically charged objects moving in a region that has both nonzero magnetic field and electric fields perpendicular to each other. • We will also investigate how our knowledge of magnetic fields helps us determine the masses of ions using a mass spectrometer. © 2014 Pearson Education, Inc. Ions moving through a perpendicular magnetic field and electric field • This device separates positively and negatively charged particles. • When the electric and magnetic forces exerted on the moving charged particles balance, the ions travel with constant velocity downward despite the presence of both a magnetic field and an electric field. © 2014 Pearson Education, Inc. Magnetohydrodynamic (MHD) generator • An MHD generator converts the random kinetic energy of high-temperature charged particles into electric potential energy. • MHD generators are used at some older coal-fired power plants to improve the efficiency of power generation. © 2014 Pearson Education, Inc. Magnetic flow meter • A magnetic flow meter works only for fluids with moving ions, which includes most fluids. • A magnetic field is oriented perpendicular to the vessel through which the fluid flows. Oppositely charged ions in the fluid are pushed by the magnetic field to opposite walls, producing a potential difference across the walls of the vessel. • With this information, we can determine the fluid's volume flow rate. © 2014 Pearson Education, Inc. Quantitative Exercise 17.9 • Is the general magnetic flow meter idea feasible for measuring blood speed in an artery? Estimate the potential difference you would expect to measure as blood in an artery passes through a 0.10-T magnetic field region. Assume the heart pumps 80 cm3 of blood each second (the approximate volume for each heartbeat) and the diameter of the artery is 1.0 cm. © 2014 Pearson Education, Inc. Mass spectrometer • A mass spectrometer helps determine the masses of ions, molecules, and even elementary particles such as protons and electrons. • It can also determine the relative concentrations of atoms of the same chemical element that have slightly different masses. © 2014 Pearson Education, Inc. Quantitative Exercise 17.10 • An atom or molecule with a single electron removed is traveling at 1.0 x 106 m/s when it enters a mass spectrometer's 0.50-T uniform magnetic field region. Its electric charge is +1.6 x 10–19 C. It moves in a circle of radius 0.20 m until it hits the detector. 1. Determine the magnitude of the magnetic force that the magnetic field exerts on the ion. 2. Determine the mass of the ion. © 2014 Pearson Education, Inc. Magnetic properties of materials • Materials, even among metals, have widely varying magnetic properties. – Magnets strongly attract objects made from iron, such as paper clips, but do not exert an observable magnetic force on objects made from aluminum, such as soda cans. – Iron has the ability to greatly amplify the magnetic field surrounding it. – How can we explain this? © 2014 Pearson Education, Inc. Observational experiment © 2014 Pearson Education, Inc. Observational experiment © 2014 Pearson Education, Inc. Magnetic properties of materials • Materials that are repelled by magnets are called diamagnetic (e.g., pyrolytic carbon or water). • Materials that are weakly attracted are called paramagnetic (e.g., aluminum). • Materials that are strongly attracted are called ferromagnetic (e.g., iron). © 2014 Pearson Education, Inc. Magnetic properties of atoms • Each electron has a magnetic dipole moment (an electron orbital magnetic moment). • The electron itself acts like a tiny bar magnet, which also contributes to the total magnetic moment produced by the atom. © 2014 Pearson Education, Inc. Diamagnetic materials • In diamagnetic materials, the magnetic moments produced by individual electrons in the atoms cancel each other, making the total field produced by the atom zero. • In the presence of an external magnetic field, the motion of the electrons in the individual atoms changes slightly, and the net magnetic field in the material is no longer zero, causing the diamagnetic object to be repelled by the magnet. © 2014 Pearson Education, Inc. Paramagnetic materials • If the orbital magnetic moments of the electrons don't cancel, an atom will have a magnetic moment similar to that of a small bar magnet. • When a paramagnetic material is placed in an external magnetic field, the atoms behave like tiny compasses and tend to align with that external magnetic field. © 2014 Pearson Education, Inc. Ferromagnetic materials • Ferromagnetic materials have individual atoms with magnetic moments, just like paramagnetic materials. • The "magnetization" effect in an external magnetic field is thousands of times stronger in ferromagnetic materials than in paramagnetic materials. © 2014 Pearson Education, Inc. Summary © 2014 Pearson Education, Inc. Summary © 2014 Pearson Education, Inc. Summary © 2014 Pearson Education, Inc.