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Electromagnetic Induction

Electromagnetic Induction. Induced EMF Faraday’s Law of Induction; Lenz’s Law EMF Induced in a Moving Conductor Electric Generators Back EMF and Counter Torque; Eddy Currents. Transformers and Transmission of Power A Changing Magnetic Flux Produces an Electric Field. Induced EMF.

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Electromagnetic Induction

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  1. Electromagnetic Induction

  2. Induced EMF • Faraday’s Law of Induction; Lenz’s Law • EMF Induced in a Moving Conductor • Electric Generators • Back EMF and Counter Torque; Eddy Currents

  3. Transformers and Transmission of Power • A Changing Magnetic Flux Produces an Electric Field

  4. Induced EMF Almost 200 years ago, Faraday looked for evidence that a magnetic field would induce an electric current with this apparatus:

  5. Induced EMF He found no evidence when the current was steady, but did see a current induced when the switch was turned on or off.

  6. Induced EMF Therefore, a changing magnetic field induces an emf. Faraday’s experiment used a magnetic field that was changing because the current producing it was changing; the previous graphic shows a magnetic field that is changing because the magnet is moving.

  7. Magnetic Flux The induced emf in a wire loop is proportional to the rate of change of magnetic flux through the loop. Magnetic flux: Unit of magnetic flux: weber, Wb: 1 Wb = 1 T·m2.

  8. Magnetic Flux This drawing shows the variables in the flux equation:

  9. Magnetic Flux The magnetic flux is analogous to the electric flux – it is proportional to the total number of magnetic field lines passing through the loop.

  10. Magnetic Flux Determining flux. A square loop of wire encloses area A1. A uniform magnetic field B perpendicular to the loop extends over the area A2. What is the magnetic flux through the loop A1?

  11. Faraday’s Law of Induction Faraday’s law of induction: the emf induced in a circuit is equal to the rate of change of magnetic flux through the circuit: or

  12. Faraday’s Law of Induction A loop of wire in a magnetic field. A square loop of wire of side l = 5.0 cm is in a uniform magnetic field B = 0.16 T. What is the magnetic flux in the loop (a) when B is perpendicular to the face of the loop and (b) when B is at an angle of 30° to the area A of the loop? (c) What is the magnitude of the average current in the loop if it has a resistance of 0.012 Ω and it is rotated from position (b) to position (a) in 0.14 s?

  13. Lenz’s Law The minus sign gives the direction of the induced emf: A current produced by an induced emf moves in a direction so that the magnetic field it produces tends to restore the changed field. or: An induced emf is always in a direction that opposes the original change in flux that caused it.

  14. Faraday’s Law of Induction Magnetic flux will change if the area of the loop changes.

  15. Faraday’s Law of Induction Magnetic flux will change if the angle between the loop and the field changes.

  16. Faraday’s Law of Induction Induction stove. In an induction stove, an ac current exists in a coil that is the “burner” (a burner that never gets hot). Why will it heat a metal pan but not a glass container?

  17. Lenz’s Law • Problem Solving: Lenz’s Law • Determine whether the magnetic flux is increasing, decreasing, or unchanged. • The magnetic field due to the induced current points in the opposite direction to the original field if the flux is increasing; in the same direction if it is decreasing; and is zero if the flux is not changing. • Use the right-hand rule to determine the direction of the current. • Remember that the external field and the field due to the induced current are different.

  18. Lenz’s Law Practice with Lenz’s law. In which direction is the current induced in the circular loop for each situation?

  19. Lenz’s Law Pulling a coil from a magnetic field. A 100-loop square coil of wire, with side l = 5.00 cm and total resistance 100 Ω, is positioned perpendicular to a uniform 0.600-T magnetic field. It is quickly pulled from the field at constant speed (moving perpendicular to B) to a region where B drops abruptly to zero. At t = 0, the right edge of the coil is at the edge of the field. It takes 0.100 s for the whole coil to reach the field-free region. Find (a) the rate of change in flux through the coil, and (b) the emf and current induced. (c) How much energy is dissipated in the coil? (d) What was the average force required (Fext)?

  20. EMF Induced in a Moving Conductor This image shows another way the magnetic flux can change:

  21. EMF Induced in a Moving Conductor Force on the rod. To make the rod move to the right at speed v, you need to apply an external force on the rod to the right. (a) Explain and determine the magnitude of the required force. (b) What external power is needed to move the rod?

  22. Electric Generators A generator is the opposite of a motor – it transforms mechanical energy into electrical energy. This is an ac generator: The axle is rotated by an external force such as falling water or steam. The brushes are in constant electrical contact with the slip rings.

  23. Electric Generators If the loop is rotating with constant angular velocity ω, the induced emf is sinusoidal: For a coil of N loops,

  24. Electric Generators An ac generator. The armature of a 60-Hz ac generator rotates in a 0.15-T magnetic field. If the area of the coil is 2.0 x 10-2 m2, how many loops must the coil contain if the peak output is to be E0 = 170 V?

  25. Electric Generators A dc generator is similar, except that it has a split-ring commutator instead of slip rings.

  26. Electric Generators Automobiles now use alternators rather than dc generators, to reduce wear.

  27. Back EMF and Counter Torque An electric motor turns because there is a torque on it due to the current. We would expect the motor to accelerate unless there is some sort of drag torque. That drag torque exists, and is due to the induced emf, called a back emf.

  28. Back EMF and Counter Torque Back emf in a motor. The armature windings of a dc motor have a resistance of 5.0 Ω. The motor is connected to a 120-V line, and when the motor reaches full speed against its normal load, the back emf is 108 V. Calculate (a) the current into the motor when it is just starting up, and (b) the current when the motor reaches full speed.

  29. Back EMF and Counter Torque Motor overload. When using an appliance such as a blender, electric drill, or sewing machine, if the appliance is overloaded or jammed so that the motor slows appreciably or stops while the power is still connected, the device can burn out and be ruined. Explain why this happens.

  30. Back EMF and Counter Torque A similar effect occurs in a generator – if it is connected to a circuit, current will flow in it, and will produce a counter torque. This means the external applied torque must increase to keep the generator turning.

  31. Eddy Currents Induced currents can flow in bulk material as well as through wires. These are called eddy currents, and can dramatically slow a conductor moving into or out of a magnetic field.

  32. Origins of Induced EMFs Emf is the work done per unit charge by the source: Induced electric fields Motional emf

  33. Motional EMF The induced current is in a direction that tends to slow the moving bar – it will take an external force to keep it moving.

  34. EMF Induced in a Moving Conductor The induced emf has magnitude This equation is valid as long as B, l, and v are mutually perpendicular (if not, it is true for their perpendicular components).

  35. Motional EMF Does a moving airplane develop a large emf? An airplane travels 1000 km/h in a region where the Earth’s magnetic field is about 5 x 10-5 T and is nearly vertical. What is the potential difference induced between the wing tips that are 70 m apart?

  36. Induced Electric Fields E produced by changing B. A magnetic field B between the pole faces of an electromagnet is nearly uniform at any instant over a circular area of radius r0. The current in the windings of the electromagnet is increasing in time so that B changes in time at a constant rate dB/dt at each point. Beyond the circular region (r > r0), we assume B = 0 at all times. Determine the electric field E at any point P a distance r from the center of the circular area due to the changing B.

  37. Applications of Induction: Sound Systems, Computer Memory, Seismograph This microphone works by induction; the vibrating membrane induces an emf in the coil.

  38. Applications of Induction: Sound Systems, Computer Memory, Seismograph Differently magnetized areas on an audio tape or disk induce signals in the read/write heads.

  39. Applications of Induction: Sound Systems, Computer Memory, Seismograph A seismograph has a fixed coil and a magnet hung on a spring (or vice versa), and records the current induced when the Earth shakes.

  40. Summary • Magnetic flux: • Changing magnetic flux induces emf: • Induced emf produces current that opposes original flux change.

  41. Summary . • Changing magnetic field produces an electric field. • General form of Faraday’s law: • Electric generator changes mechanical energy to electrical energy; electric motor does the opposite.

  42. Inductance AC Circuits

  43. Mutual Inductance • Self-Inductance • Energy Stored in a Magnetic Field • LR Circuits • LC Circuits and Electromagnetic Oscillations • LC Circuits with Resistance (LRC Circuits) • AC Circuits with AC Source

  44. LRC Series AC Circuit • Resonance in AC Circuits • Impedance Matching • Three-Phase AC

  45. Induced emf in one circuit due to changes in the magnetic fieldproduced by the second circuit is called mutual induction. Induced emf in one circuit associated with changes in its own magnetic fieldis called self-induction. Inductance

  46. Inductance Unit of inductance: the henry, H: 1 H = 1 V·s/A = 1 Ω·s.

  47. Mutual Inductance Mutual inductance: magnetic flux through coil2 due to current in coil 1 Induced emf due to mutual induction:

  48. Mutual Inductance Solenoid and coil. A long thin solenoid of length l and cross-sectional area A contains N1 closely packed turns of wire. Wrapped around it is an insulated coil of N2 turns. Assume all the flux from coil 1 (the solenoid) passes through coil 2, and calculate the mutual inductance.

  49. Mutual Inductance Reversing the coils. How would the previous example change if the coil with turns was inside the solenoid rather than outside the solenoid?

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