Magnetism I INTRODUCTION Magnetism, an aspect of electromagnetism, one of the fundamental forces of nature.

Magnetism I INTRODUCTION Magnetism, an aspect of electromagnetism, one of the fundamental forces of nature. Magnetic forces are produced by the motion of charged particles such as electrons, indicating the close relationship between electricity and magnetism. The unifying frame for these two forces is called electromagnetic theory (see Electromagnetic Radiation). The most familiar evidence of magnetism is the attractive or repulsive force observed to act between magnetic materials such as iron. More subtle effects of magnetism, however, are found in all matter. In recent times these effects have provided important clues to the atomic structure of matter. II HISTORY OF STUDY The phenomenon of magnetism has been known of since ancient times. The mineral lodestone (see Magnetite), an oxide of iron that has the property of attracting iron objects, was known to the Greeks, Romans, and Chinese. When a piece of iron is stroked with lodestone, the iron itself acquires the same ability to attract other pieces of iron. The magnets thus produced are polarized--that is, each has two sides or ends called north-seeking and south-seeking poles. Like poles repel one another, and unlike poles attract. The compass was first used for navigation in the West some time after AD1200. In the 13th century, important investigations of magnets were made by the French scholar Petrus Peregrinus. His discoveries stood for nearly 300 years, until the English physicist and physician William Gilbert published his book Of Magnets, Magnetic Bodies, and the Great Magnet of the Earth in 1600. Gilbert applied scientific methods to the study of electricity and magnetism. He pointed out that the earth itself behaves like a giant magnet, and through a series of experiments, he investigated and disproved several incorrect notions about magnetism that were accepted as being true at the time. Subsequently, in 1750, the English geologist John Michell invented a balance that he used in the study of magnetic forces. He showed that the attraction and repulsion of magnets decrease as the squares of the distance from the respective poles increase. The French physicist Charles Augustin de Coulomb, who had measured the forces between electric charges, later verified Michell's observation with high precision. III ELECTROMAGNETIC THEORY André Marie Ampère French physicist André Marie Ampère explored the relationship between electricity and magnetism. In 1820 he discovered the principle of electromagnetic reaction by observing the force exerted by a magnetic field when an electrical current passes through it. The ampere, or amp (the unit of measure that defines the rate of flow in an electric current), is named after him. Photo Researchers, Inc. In the late 18th and early 19th centuries, the theories of electricity and magnetism were investigated simultaneously. In 1819 an important discovery was made by the Danish physicist Hans Christian Oersted, who found that a magnetic needle could be deflected by an electric current flowing through a wire. This discovery, which showed a connection between electricity and magnetism, was followed up by the French scientist André Marie Ampère, who studied the forces between wires carrying electric currents, and by the French physicist Dominique François Jean Arago, who magnetized a piece of iron by placing it near a current-carrying wire. In 1831 the English scientist Michael Faraday discovered that moving a magnet near a wire induces an electric current in that wire, the inverse effect to that found by Oersted: Oersted showed that an electric current creates a magnetic field, while Faraday showed that a magnetic field can be used to create an electric current. The full unification of the theories of electricity and magnetism was achieved by the English physicist James Clerk Maxwell, who predicted the existence of electromagnetic waves and identified light as an electromagnetic phenomenon. Magnetic Fields and Currents Hans Christian Oersted predicted in 1813 that a connection would be found between electricity and magnetism. In 1819 he placed a compass near a current-carrying wire and observed that the compass needle was deflected. This discovery demonstrated that electric currents produce magnetic fields. As shown here, the magnetic field lines circle around the current-carrying wire. © Microsoft Corporation. All Rights Reserved. Subsequent studies of magnetism were increasingly concerned with an understanding of the atomic and molecular origins of the magnetic properties of matter. In 1905 the French physicist Paul Langevin produced a theory regarding the temperature dependence of the magnetic properties of paramagnets (discussed below), which was based on the atomic structure of matter. This theory is an early example of the description of large-scale properties in terms of the properties of electrons and atoms. Langevin's theory was subsequently expanded by the French physicist Pierre Ernst Weiss, who postulated the existence of an internal, "molecular" magnetic field in materials such as iron. This concept, when combined with Langevin's theory, served to explain the properties of strongly magnetic materials such as lodestone. Michael Faraday Michael Faraday made significant contributions to the study of electricity and magnetism. He found that a current flows in a wire that is moved through a magnetic field. The discovery of this phenomenon, which is called electromagnetic induction, contributed to the development of Maxwell's equations, and led to the invention of the electric generator. Culver Pictures After Weiss's theory, magnetic properties were explored in greater and greater detail. The theory of atomic structure of Danish physicist Niels Bohr, for example, provided an understanding of the periodic table and showed why magnetism occurs in transition elements such as iron and the rare earth elements, or in compounds containing these elements. The American physicists Samuel Abraham Goudsmit and George Eugene Uhlenbeck showed in 1925 that the electron itself has spin and behaves like a small bar magnet. (At the atomic level, magnetism is measured in terms of magnetic moments--a magnetic moment is a vector quantity that depends on the strength and orientation of the magnetic field, and the configuration of the object that produces the magnetic field.) The German physicist Werner Heisenberg gave a detailed explanation for Weiss's molecular field in 1927, on the basis of the newly-developed quantum mechanics (see Quantum Theory). Other scientists then predicted many more complex atomic arrangements of magnetic moments, with diverse magnetic properties. IV THE MAGNETIC FIELD Magnetic Field of a Permanent Magnet Iron filings arrange themselves along the lines of a magnetic force, making the lines visible. Magnets are surrounded by a magnetic field, and the magnetic lines of force run from one pole of the magnet to the other. Orion Press Photo Library Objects such as a bar magnet or a current-carrying wire can influence other magnetic materials without physically contacting them, because magnetic objects produce a magnetic field. Magnetic fields are usually represented by magnetic flux lines. At any point, the direction of the magnetic field is the same as the direction of the flux lines, and the strength of the magnetic field is proportional to the space between the flux lines. For example, in a bar magnet, the flux lines emerge at one end of the magnet, then curve around the other end; the flux lines can be thought of as being closed loops, with part of the loop inside the magnet, and part of the loop outside. At the ends of the magnet, where the flux lines are closest together, the magnetic field is strongest; toward the side of the magnet, where the flux lines are farther apart, the magnetic field is weaker. Depending on their shapes and magnetic strengths, different kinds of magnets produce different patterns of flux lines. The pattern of flux lines created by magnets or any other object that creates a magnetic field can be mapped by using a compass or small iron filings. Magnets tend to align themselves along magnetic flux lines. Thus a compass, which is a small magnet that is free to rotate, will tend to orient itself in the direction of the magnetic flux lines. By noting the direction of the compass needle when the compass is placed at many locations around the source of the magnetic field, the pattern of flux lines can be inferred. Alternatively, when iron filings are placed around an object that creates a magnetic field, the filings will line up along the flux lines, revealing the flux line pattern. Magnetic fields influence magnetic materials, and also influence charged particles that move through the magnetic field. Generally, when a charged particle moves through a magnetic field, it feels a force that is at right angles both to the velocity of the charged particle and the magnetic field. Since the force is always perpendicular to the velocity of the charged particle, a charged particle in a magnetic field moves in a curved path. Magnetic fields are used to change the paths of charged particles in devices such as particle accelerators and mass spectrometers. V KINDS OF MAGNETIC MATERIALS Paramagnetism Liquid oxygen becomes trapped in an electromagnet's magnetic field because oxygen (O2) is paramagnetic. Oxygen has two unpaired electrons whose magnetic moments align with external magnetic field lines. When this occurs, the O2 molecules themselves behave like tiny magnets, and become trapped between the poles of the electromagnet. Yoav Levy/Phototake NYC The magnetic properties of materials are classified in a number of different ways. One classification of magnetic materials--into diamagnetic, paramagnetic, and ferromagnetic--is based on how the material reacts to a magnetic field. Diamagnetic materials, when placed in a magnetic field, have a magnetic moment induced in them that opposes the direction of the magnetic field. This property is now understood to be a result of electric currents that are induced in individual atoms and molecules. These currents, according to Ampere's law, produce magnetic moments in opposition to the applied field. Many materials are diamagnetic; the strongest ones are metallic bismuth and organic molecules, such as benzene, that have a cyclic structure, enabling the easy establishment of electric currents. Paramagnetic behavior results when the applied magnetic field lines up all the existing magnetic moments of the individual atoms or molecules that make up the material. This results in an overall magnetic moment that adds to the magnetic field. Paramagnetic materials usually contain transition metals or rare earth elements that possess unpaired electrons. Paramagnetism in nonmetallic substances is usually characterized by temperature dependence; that is, the size of an induced magnetic moment varies inversely to the temperature. This is a result of the increasing difficulty of ordering the magnetic moments of the individual atoms along the direction of the magnetic field as the temperature is raised. A ferromagnetic substance is one that, like iron, retains a magnetic moment even when the external magnetic field is reduced to zero. This effect is a result of a strong interaction between the magnetic moments of the individual atoms or electrons in the magnetic substance that causes them to line up parallel to one another. In ordinary circumstances these ferromagnetic materials are divided into regions called domains; in each domain, the atomic moments are aligned parallel to one another. Separate domains have total moments that do not necessarily point in the same direction. Thus, although an ordinary piece of iron might not have an overall magnetic moment, magnetization can be induced in it by placing the iron in a magnetic field, thereby aligning the moments of all the individual domains. The energy expended in reorienting the domains from the magnetized back to the demagnetized state manifests itself in a lag in response, known as hysteresis. Ferromagnetic materials, when heated, eventually lose their magnetic properties. This loss becomes complete above the Curie temperature, named after the French physicist Pierre Curie, who discovered it in 1895. (The Curie temperature of metallic iron is about 770° C/1300° F.) VI OTHER MAGNETIC ORDERINGS In recent years, a greater understanding of the atomic origins of magnetic properties has resulted in the discovery of other types of magnetic ordering. Substances are known in which the magnetic moments interact in such a way that it is energetically favorable for them to line up antiparallel; such materials are called antiferromagnets. There is a temperature analogous to the Curie temperature called the Neel temperature, above which antiferromagnetic order disappears. Other, more complex atomic arrangements of magnetic moments have also been found. Ferrimagnetic substances have at least two different kinds of atomic magnetic moments, which are oriented antiparallel to one another. Because the moments are of different size, a net magnetic moment remains, unlike the situation in an antiferromagnet where all the magnetic moments cancel out. Interestingly, lodestone is a ferrimagnet rather than a ferromagnet; two types of iron ions, each with a different magnetic moment, are in the material. Even more complex arrangements have been found in which the magnetic moments are arranged in spirals. Studies of these arrangements have provided much information on the interactions between magnetic moments in solids. VII APPLICATIONS Magnetic Levitation Train Magnetic levitation trains levitate above the track by means of a magnetic suspension system, thus reducing or eliminating vibration, friction, and noise. Magnetic levitation trains can reach extremely high speeds. This experimental train in Germany reaches 435 km/hr (270 mph). Thomas Raupach/Woodfin Camp and Associates, Inc. Numerous applications of magnetism and of magnetic materials have arisen in the past 100 years. The electromagnet, for example, is the basis of the electric motor and the transformer. In more recent times, the development of new magnetic materials has also been important in the computer revolution. Computer memories can be fabricated using bubble domains. These domains are actually smaller regions of magnetization that are either parallel or antiparallel to the overall magnetization of the material. Depending on this direction, the bubble indicates either a one or a zero, thus serving as the units of the binary number system used in computers. Magnetic materials are also important constituents of tapes and disks on which data are stored. In addition to the atomic-sized magnetic units used in computers, large, powerful magnets are crucial to a variety of modern technologies. Powerful magnetic fields are used in nuclear magnetic resonance imaging, an important diagnostic tool used by doctors. Superconducting magnets are used in today's most powerful particle accelerators to keep the accelerated particles focused and moving in a curved path. Scientists are developing magnetic levitation trains that use strong magnets to enable trains to float above the tracks, reducing friction. Contributed By: Martin Blume Microsoft ® Encarta ® 2009. © 1993-2008 Microsoft Corporation. All rights reserved.