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Topic #21, Magnetic Fields and Magnetic Phenomenon Part I: Magnetic Fields 1. General Properties of Magnets 2. Magnetic Fields Around Permanent Magnets 3. Electromagnetism 4. Magnetic Field Around a Coil 5. Forces on Currents in Magnetic Fields 6. Measuring the Force on a Wire (not printed in notes) 7. Galvanometers 8. Electric Motors 9. The Force on a single Charged Particle (Optional / not printed in the passage) Part II: Electromagnetic Induction 1. Faraday's Discovery 2. Induced EMF 3. Electric Generators 4. Alternating-Current Generators 5. Generators and Motors 6. Lenz's Law 7. Self-Inductance 8. Transformers Notes Should Include: Special Note: It is said that Benjamin Franklin, who was a scientist as well as a statesman and a publisher, defined electricity as the flow of positive charge. This occurred long before the discovery of the electron or any other subatomic particle. It turns out that it is the electron, the negatively charged particle, that actually moves when electric current flows. On the other hand, the applications of the principles and equations to the study of magnetism work just fine using either definition. This is important to know when you study the relationship between electricity and magnetism. In the following passage you will encounter several left hand rules based upon actual movement of electrons through wires. There is a counterpart to all of this when describing electricity as the flow of positive charge. First of all electric current is called “conventional current” when the current is defined as the flow of positive charge. Second of all the left hand rules referred to here are redefined as right hand rules. You may be expected to know both. Part I: Magnetic Fields General Properties of Magnets: Naturally occurring magnetic rocks are called lodestones. Though these rocks were known about more than 2,000 years ago, and were used for navigation once it was realized that they aligned themselves with the north and south directions, it wasn't until the beginning of the 17th century that an investigation was carried out on magnets and magnetic phenomenon. A person by the name of William Gilbert conducted this research. The properties of naturally occurring and artificial magnets (magnets produced by magnetizing material which was not previously magnetized) are discussed here. www.physicsphenomena.com / Magnetic Fields and Magnetic Phenomenon 1 Characteristic Properties: First - magnets have polarity. The end that points north is often referred to as the north seeking end of the magnet or what is frequently called the north pole of the magnet. Likewise, the end that points towards the south is called the south seeking end of the magnet or the south pole of the magnet. Though these poles are distinct (very different from one another), they cannot be separated from each other. A magnet cannot just have a north pole or a south pole by itself. This has to do with the nature of magnetism. Second - Like magnetic poles, as in two north or two south poles, repel one another while unlike magnetic poles attract each other. Third - A compass is a small needle shaped magnet that is suspended so it can turn freely without any significant amount of friction. The end of the magnet pointing towards the north is not actually pointing towards the geographical north (the north pole of the earths axis), but rather is pointing towards the earth's magnetic north pole. In recent years the north magnetic pole has been in northern part of Canada not far from the Arctic Circle, but it may not remain there. The magnetic poles drift over the course of time. The poles can move around considerably each day, but migrates on average about 10 kilometers to 40 kilometers each year. Fourth - The materials that show magnetic properties are Iron, Nickel, and Cobalt. Permanent magnets are made of alloys of these materials. A magnet made for commercial sale is often made out of an alloy of aluminum, nickel, cobalt, and iron called ALNICO. Permanent magnets retain their magnetism for a long time. Fifth - Iron, Cobalt, and Nickel can be magnetized by induction. Bringing a piece of iron into contact with a permanent magnet will cause the iron to become a temporary magnet. Remove the permanent magnet and the piece of iron loses most if not all of the magnetism. Some residual magnetism may remain. Magnetic Fields Around Permanent Magnets: Magnets, like mass and charge, exert force over distance. This means that a magnet has a field around it that can affect other objects with magnetic properties. If another object, a magnet or a material that responds to a magnet, is brought into this field at some specified distance, there will be either a force of attraction or repulsion between the original magnet and the object. This region around the magnet is called a magnetic field. The magnetic fields around magnets can be made visible by placing a sheet of paper over the magnet and then sprinkling iron filings over the piece of paper. The magnetic field will align the filings along the magnetic field. The pattern looks like lines because the particles are long and thin. Often these lines are called magnetic field lines. You should remember that these lines are just a model used to visualize the invisible field and are not the field itself, though for convenience it may be convenient to discuss the field as though it were made up of the lines. For example, there is a measurement called the magnetic flux. The magnetic flux measures the number of magnetic field lines in any given location within a magnet's magnetic field. It follows that the flux per unit cross sectional area is a means of describing the strength of the magnetic field at that location. If you made a sketch of a magnet such as a bar magnet and included the magnetic field lines, it would be appropriate to place arrows on the lines to show the direction of the field. The field lines would appear to move out from the north pole of the magnet and curve around to the south pole of the magnet. All of the lines arriving at the south pole of the magnet would go straight up the magnet to the north pole of the magnet where they would again move out and curve back towards the south pole of the magnet. One limitation of such a diagram is that it is only twodimensional and therefore only shows the lines in one plane. The actual field and therefore the lines that represent it would best be shown as a three dimensional image. Electromagnetism: Back around 1820, a Danish scientist by the name of Hans Christian Oersted, discovered that electric current affects magnets. He laid a current carrying wire across a www.physicsphenomena.com / Magnetic Fields and Magnetic Phenomenon 2 compass and observed that the needle was deflected when the current flowed, but returned to its normal north - south orientation when the current was turned off. He deduced that the current was producing a magnetic field. This field can be visualized using iron filings. Attach a wide cardboard collar around a wire. Set the wire up vertically and make the collar perpendicular to it. Shake some iron filings onto the collar and run a current through the wire. What you would see is the alignment of the filings forming a circular line around the wire. The filings are aligning themselves in the magnetic field produced by the electrical charges flowing through the wire. The pattern observed shows us that the magnetic field lines form “closed circles” (loops) around the wire. The larger the current flowing through the wire the larger the magnetic field formed around the wire. The strength of the magnetic field drops off with the square of the distance from the wire. To find the direction of the magnetic field around the wire (i.e. clockwise or counterclockwise from your perspective) use the first left - hand rule. The left hand rule says to grasp the wire in your left hand with your thumb pointing in the direction of the electron flow. The fingers of you hand point in the direction of the magnetic field. If you were describing electric current as the flow of positive charge (perceived as flowing in the opposite direction to the electrons) you would use the right hand and it would be called the right hand rule. In either case the direction of the magnetic field is the same around the wire. A Magnetic Field Around a Coil: An interesting phenomenon occurs when a wire is formed into a circle (loop) at some point in a circuit. A magnetic field will appear all around the loop when a current flows through the wire. The left - hand rule will show what direction the magnetic field is pointing in terms of the plane the loop lies in. For an example, consider a loop of wire lying in a horizontal plane in front of you. The wire feeds electrons into and out of the loop so as you look down on the loop the current is flowing clockwise around the loop. Applying the left hand rule you would discover that the magnetic field points up out of the plane the loop is in. Inside this single coil (loop) there is a continuous magnetic field pointing upwards. Outside the coil the field acts in a downward direction. The coil acts like a permanent magnet with one side of the coil (the top side in this case) acting as the north pole of the magnet and the other side of the coil (the bottom side in this case) acting as a south pole of the magnet. Bring a north pole of a permanent magnet near the north pole of this coil (loop) and it would be repelled. Bring a south pole of a permanent magnet near the north pole of this coil and it would be attracted. A current carrying wire can be looped a number of times rather than just once. Technically, a coil is not a single loop, though you might call it that. A coil consists of more than one loop. A coil having a magnetic field produced by a current traveling through the wire making up the coil is called an electromagnet. The magnetic field’s direction in a coil of wire can be found by the use of the second left - hand rule. The second left-hand rule says to grasp the coil with your left hand so that your finger wrap around the loops of the coil in the direction the current is traveling through the wires that make up the loops in the coil. Your thumb will point in the direction of the north pole of the coil (electromagnet). The strength of the electromagnet field can be increased when an iron rod, often called a core, is placed inside the coil. This core is magnetized by induction and its magnetic field combines with the coils magnetic field to produce a stronger field. Increasing the number of loops in a coil also increases the strength of the magnetic field produced by the electromagnet. Magnetic Materials: Around the turn of the 18th century, a scientist by the name of Andre Ampere suggested that magnetism in magnets was due to little "loops of current" existing within the bar. It appears that he knew something of the nature of electromagnetism and concluded that www.physicsphenomena.com / Magnetic Fields and Magnetic Phenomenon 3 there must be a similar phenomenon happening within the structure of materials which exhibited magnetic characteristics. Based upon what we know about the atom's structure and how that structure helps us to explain magnetic phenomenon, he was essentially correct, though not very technical, because atomic structure wasn't even known about yet, much less understood. In the atom the electrons move about the nucleus. These electrons also spin. Each electron, in effect, acts like a very tiny magnet. (remember that moving charge produces magnetic fields) It is possible for the electrons' magnetic fields to combine making for even a larger and stronger field. This can happen among neighboring atoms in some materials. These clusters of atoms collectively producing a magnetic field are called domains. Even though these domains may consist of hundreds of atoms, domains are quite small compared to even the smallest magnet that you can see and hold in your hand. If these domains in a material like iron point off in many different directions, the piece of metal as a whole does not exhibit any significant magnetic properties. However, if the domains can be made to line up so their individual magnetic fields reinforce each other, the piece of iron exhibits magnetic properties and acts as a magnet. In a temporary magnet enough domains line up as long as the material is in a strong magnetic field. Fairly soon after the magnetic field is cut off or moved away from the temporary magnet, its domains shift back to their random patterns as before being exposed to the field. In permanent magnets the iron is alloyed with other materials that contribute to keeping the domains aligned. Forces on Currents in Magnetic Fields: Andre Ampere also hypothesized that a magnetic field should exert a force on a wire that had a current flowing through it. The strength of a magnetic field is called magnetic induction (Symbol B). A scientist by the name of Michael Faraday, during the first half of the 19th century, determined that the force on the wire caused by the magnetic is at right angles to the magnetic field. The force is also at right angles to the direction of the current as well. The direction of the force is determined through the third left - hand rule. This rule is used when the current carrying wire is placed between the two poles of a magnet. This rule says to point the fingers of the left hand in the direction of the magnetic field. Then point the thumb in the direction of the current flow. Finally, the palm of the hand faces in the direction of the force acting on moving the wire. Galvanometers: The galvanometer is a device used to measure very small currents and is found in many voltmeters and ammeters. Structurally, the galvanometer has coil of wire placed in the magnetic field of a strong magnet. When current flows through the coil it rotates in the magnetic field. According to the third left - hand rule one side of the coil is pressed down while the other side is of the loop is forced up. The loop is sitting on a shaft that allows it to rotate, and when current is flowing through the coil it does rotate. The more current in the loop the further it turns. The force on the coil varies directly with the current traveling through the coil. The turning coil is working against a small spring, which if current is not present would pull the coil back to a starting position. A needle pointing to a scale moves across the scale indicating the amount of current flowing through the coil. The scale is calibrated by using known amounts of currents so values can be printed up on the scale. When the galvanometer is used as an ammeter a resistor is placed in parallel to the circuit having the coil. This resistor is kept small and acts as a shunt for most of the current that would be blocked by the resistance of the main galvanometer circuit. The meter is sensitive to small currents so very little needs to pass through the coil to get a measurement of current in the electrical circuit the ammeter has been placed in. When the galvanometer is used as a voltmeter, a resistor called a multiplier is placed in series with the galvanometer circuit. The meter is www.physicsphenomena.com / Magnetic Fields and Magnetic Phenomenon 4 calibrated to read in volts, though the galvanometer measures the current passing through it. The ammeter is wired in series with the path in which the current is flowing and its resistance must be low so the effective resistance of the circuit remains essentially unaffected. The voltmeter is wired in parallel with the device whose voltage drop is being measured and its resistance must be very high so little current passes through it changing the parameters of the circuit. Ammeters and voltmeters should have very little if any impact on the circuit they are being used on, if the data collected from the instruments is to mean much. Electric Motors: The small coil in a galvanometer is limited to a maximum rotation of 180o. For a loop to turn beyond 180o and be able to turn through 360o and so on, the current has to be able be reversed so each 180 degrees the forces are in opposition. To allow the current to change direction every 180 degrees a split ring commutator is used to connect the coil part of the circuit with the source of the voltage. In simple terms half of the ring is attached to a wire connected to one wire of the coil and the other half of the ring is attached to the other wire of the coil. Current flows from a voltage source through a wire which has a brush (a sliding metal contact) which touches one half of the ring and returns to the voltage source through the other half of the ring which has a second brush touching it which in turn is connected to the second wire (the return wire) that is connected to the voltage source. Part II: Electromagnetic Induction Faradays Discovery: Michael Faraday spent about ten years trying to produce a current in a wire using magnetic fields of constant magnitude. Finally, he discovered that a changing magnetic field could produce an electric current. He found that when he moved a wire through a magnetic field an electric current was induced in the wire. If the wire was moved up through the field, the current would flow in one direction and if the wire were moved down through the field the current would flow in the opposite direction. If the wire is held stationary in the field, no current flows through the wire. If the wire is moved parallel to the field, no current flows through the wire. The wire has to "cut through" the field for an electric current to be produced. Moving the field with respect to the wire while the wire remains stationary will also produce an electric current as long as the motion still in effect causes the field to be "cut through" by the wire. This method of producing electric current by causing a wire to move perpendicularly through a magnetic field is called electromagnetic induction. If the wire in effect passes at an angle through the field, neither moving parallel to the field (no current produced) nor moving perpendicular to the field (current produced), only the portion of the wire's motion that is perpendicular to the field will produce some current. This amount of current will be between zero amperes and the amount that could be produced if the wire moved perpendicularly through the field. To determine the direction of the current through the wire use the third left - hand rule. In this case point the thumb in the direction the wire is moving and point the fingers in the direction of the magnetic field. The palm of the hand points in the direction of the force pushing the electrons, which is the direction the electrons will move, as in the direction current will flow. Induced EMF: In a very real sense an electron pump is needed to make electrons move (electricity). The potential difference (voltage) necessary to move the charges can be referred to as the electromotive force (EMF). This, contrary to the name, is NOT a force, but is a measurement of the electrical potential difference expressed in the units volts. Think of electrical potential as being similar to gravitational potential energy. The water at the top of a water fall has potential energy. When the water is not being blocked by the use of a dam, it will flow, and as it www.physicsphenomena.com / Magnetic Fields and Magnetic Phenomenon 5 does its potential energy becomes kinetic energy. If the water is dammed up and stored in a reservoir waiting to flow through a channel, it retains its potential energy until it is allowed to flow. Similarly a fully charged battery is an electrical reservoir full of charge waiting to flow through a circuit. When a wire is moved through a magnetic field, the electrons experience an increase in energy. In effect, they experience an increase in electrical potential. This increase in electrical potential is the called the induced EMF, and is expressed in volts. When the wire was stationary its EMF was zero. The EMF the wire experiences is a function of the magnetic induction, the length of wire in the field, and the velocity of the wire in the field. Producing an EMF doesn't mean that a current will automatically flow through the wire. The wire needs to be part of a circuit for current to actually flow. This is similar to a battery. It too has electrical potential when charged, but no current flows either from it or into it, unless it is part of a circuit. Electric Generators: Michael Faraday is credited with inventing the electric generator. An electric generator has a coil of wire loops placed in a magnetic field. A mechanical device is attached to a shaft that the coil is mounted on. As the coil is turned by a crank or even a steam turbine (used in electrical generating plants) current is produced in the wire loops of the coil. The wire loops in the coil are sometimes called windings and the windings mounted on a shaft are called an armature. The coil of loops mounted on a shaft in an electric motor is also called an armature. The wire in these windings must have a thin but strong insulation around them, so no current jumps between the loops causing a short circuit. As the armature in the generator is turned, the moving loops of wire in the rotating coil cause the EMF to fluctuate from zero (where the loop is moving parallel to the field) to a maximum value (where the loop is moving exactly perpendicular to the field). This process happens twice during one 360o rotation. Within the first 180 degrees the EMF goes between zero and a maximum value causing current to rise and fall in one direction proportional to the EMF value. Within the second 180 degrees The EMF again goes from zero to a maximum, but the EMF is in the opposite direction, causing the current to rise and fall in the opposite direction proportional to the EMF value. So for each turn of the crank, there are two current spikes, one occurring during the first half of a turn and the other occurring during the second half of the turn. The two current spikes however are in opposite directions, so what you have is alternating current not direct current. The actual increase and decrease of current during one half of a turn is not really sudden as the term spike might suggest, but rather a smooth increase and decrease. A graph of the rise and fall of the current is cyclical and resembles a sign curve. As the armature turns the angle keeps changing and the EMF (voltage) and the current (amperage) are changed proportionally with each other. Alternating Current Generator: In the United States one cycle of armature rotation has a period of 1/60 of a second and the frequency is 60 hertz. This means that since each cycle of the armature causes the current to flow first in one direction and then in the opposite direction, the current changes direction 120 times each second. One wire from the armature coil connects to a slip (not split, as in an electric motor) ring on the shaft. A brush attached to a wire from the rest of the circuit makes contact with this ring. The other wire from the windings is attached to a second slip ring also mounted on the shaft of the armature. A second brush attached this second wire coming from the circuit makes contact with this second ring. When all contact points are closed (touching without any breaks in the circuit, including a closed switch) current flows from the generator through circuit and back. Of course the direction of this current is constantly reversing itself. If there is not a continuous circuit for current to flow through the rotation of the armature will still produce an oscillating EMF, but no current will be able to flow. www.physicsphenomena.com / Magnetic Fields and Magnetic Phenomenon 6 Generators and Motors: Generators and motors are of similar construction. In the motor, current is sent into the wire loops in the coil of the armature to produce a repulsive force between the magnetic field of the magnet and the magnetic field produced in the loops of wire in the coil. The opposing forces caused the armature to turn producing mechanical energy. In the case of the generator no current is sent into the wire loops in the coil of the armature. Instead mechanical energy is used to turn the armature. When the wire loops in the coil of the armature rotate in the magnetic field an oscillating EMF is produced. If the generator is connected to a circuit alternating current flows through the circuit. Lenz's Law: It is interesting to note that even though a current is produced in the wire loops on the armature as the loops move through the magnetic field, the presence of the current in the wire loops produce a magnetic field of their own. This field produces a force that opposes the motion of the turning loops of wire. This force acts in the direction opposite that of the motion of the wire and actually slows down the rotation. The direction of this force was determined by H. F. E. Lenz in 1834. This observation is called Lenz's law, which says that the current induced in a direction such that the magnetic effects produced by that current oppose the change in flux that induced the current. The change in flux is being opposed not the flux itself. When the generator is producing only a little current the opposing force is small, but when the generator is producing a large amount of current the opposing force is large. Electric motors experience this phenomenon as well. When a current carrying wire moves in a magnetic field an EMF is produced. This EMF opposes the current flow and is called "Back EMF". When an electric motor is first turned on, there is a large flow of current because of the low resistance in the wire of the armature. As the motor starts turning the movement of the wires across the magnetic field induces back EMF. This back EMF opposes the current flow. As a consequence the current flowing through the motor is reduced. If a mechanical load is placed on the motor (this means the motor is used to do work and not just sit there with its armature shaft spinning) the load slows down the rotational speed of the wire. This means the wire loops in the armature are now moving through the magnetic field at a slower rate and are producing less back EMF. This results in an increase in the flow of current flows. Should the load be so great as to stop the armature from turning at all, such as in the case of an electric saw's blade binding in a piece of wood, the current flow can increase to such an extent that the wires will overheat melting or burning up the insulation. This can result in a short circuit, blown fuse, and one damaged motor. The large current flow when a motor is first started can cause voltage drops across the wires that bring electricity to the motor. Wires do have resistances and in certain circumstances the voltage drops across these resistances can be significant. The wires, referred to here, are the wires in the motor circuit that are outside of the motor itself. If an ordinary light bulb were wired in parallel with a motor, it would be seen to dim when the motor is first turned on and brighten again once the motor was up to speed. What is happening here is that there is no significant back EMF when the motor is first turned on. As a consequence there is an initial surge in current affecting both the voltage drop across the wires that feed current to the motor and the voltage drop across the motor. Initially this results in a momentary current surge in the circuit containing the motor. Since the resistance of the light bulb does not change in the parallel path, more current initially goes through the branch with the motor and less through the path with the light bulb. Consequently the bulb appears to dim when the motor is first turned on. As the motor picks up speed the back EMF increases and the current through the motor’s path decreases and the current through the light www.physicsphenomena.com / Magnetic Fields and Magnetic Phenomenon 7 bulb increases causing the bulb to brighten once again. See the explanation in terms of Ohm’s law in the next paragraph. Ohm's law tells us that V = I R. So when I suddenly increases a lot even though R is small, V will increase a lot to. As the back EMF slows the current down after start up, the voltage drop decreases and current to the light and in turn its brightness returns to normal. Another interesting phenomenon associated with this situation involves the turning off or unplugging the motor while its running. The sudden loss in the electromagnetic field will produce a back EMF that will cause a spark to jump across the switch or across from the plug to the outlet. Self - Inductance: As a current in a coil changes, an induced EMF is produced in that coil. This process is called self - inductance. The direction of this EMF is opposite to the current flow. Therefore, this EMF is opposing the flow of current. This opposition to the flow of current explains why the current flow when a switch is thrown is not instantly at a maximum value but requires a short amount of time to be reached. Once the desired current is reached, the current remains constant, the magnetic flux is constant, and the EMF is zero. It is most important to remember that it the change in the magnetic flux that induces this EMF, not the magnetic flux itself. A decrease in current will cause a decrease in the magnetic flux and an EMF will be generated that opposes the decrease in the current. (Rem: Magnetic flux is a measure of the strength of a magnetic field. This is true whether it’s the field around a permanent magnet or current carrying wire. Flux lines, used to represent magnetic fields, are always closed loops.) Transformers: A transformer is an electrical device that is used to either increase or decrease alternating current voltages. This is an example of electromagnetic induction at work. Structurally, a transformer consists of two electrical coils wound around the same iron core. One of the coils is called the primary coil while the other is called the secondary coil. When an AC voltage source called the primary voltage is connected to the primary coil, the alternating (changing) current produces a varying magnetic flux caused by the continual flip flopping of current direction. This varying magnetic flux is carried by means of the core to the secondary coil. This varying flux in the secondary core induces a varying EMF. The effect is called mutual inductance. This induced EMF in the secondary coils is called the secondary voltage. The magnitude of this secondary voltage is dependent upon the ratio of turns between the secondary and the primary coil. The equation to calculate the secondary voltage is written VS / VP = NS / NP. In this equation V is representing voltage and N is representing the number of turns in the coil. It should be noted that, if the secondary voltage is larger than the primary voltage the transformer is called a step - up transformer, but if the secondary voltage is less than the primary voltage the transformer is called a step - down transformer. Ideally the electric power delivered by the secondary circuit is equal to the power used by the primary circuit. The equation representing this relationship is based on P = V I and is written as VP IP = VS IS. Step up transformers are used at the electrical generating plants to develop high voltages for the transmission lines, while step down transformers are used at substations and on poles to get the voltage down to the value used by homes and businesses. In your automobile the spark or ignition coil is designed to step up the 12 volts from your battery to thousands of volts in order to supply the power necessary to run that small electric starter motor that cranks your gasoline engine until it starts. (It sure beats hand cranking your engine like people had to do in early cars and trucks.) www.physicsphenomena.com / Magnetic Fields and Magnetic Phenomenon 8 Vocabulary: Part I: polarized, magnetic field, magnetic flux, first left hand rule / first right hand rule, solenoid, electromagnet, second left hand rule / second right hand rule, domain, third left hand rule / third left hand rule, galvanometer, electric motor, armature; Part II: electromagnetic induction, electromotive force, electric generator, Lenz’s Law, eddy current, self inductance, transformer, primary coil, secondary coil, mutual inductance, step up transformer, step down transformer Skills to be learned: Solve problems using the left (or right) hand rules Solve problems involving transformers Assignments: Textbook: Read / Study / Learn about Magnetism and Its Applications WB Exercise(s): Activities: TBA Resources: This Handout and the Overhead and Board Notes discussed in class Textbook: Chapters 23 and 25 WB Lessons and Problem Sets www.physicsphenomena.com - “Magnetic Fields and Magnetic Phenomenon” www.physicsphenomena.com / Magnetic Fields and Magnetic Phenomenon 9