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Lecture 9 – Electromagnetic Induction

Lecture 9 – Electromagnetic Induction. Chapter 29 Electromagnetic Induction and Faraday’s Law. Units of Chapter 29. Induced EMF Faraday’s Law of Induction; Lenz’s Law EMF Induced in a Moving Conductor Electric Generators Transformers and Transmission of Power

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Lecture 9 – Electromagnetic Induction

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  1. Lecture 9 – Electromagnetic Induction

  2. Chapter 29Electromagnetic Induction and Faraday’s Law

  3. Units of Chapter 29 • Induced EMF • Faraday’s Law of Induction; Lenz’s Law • EMF Induced in a Moving Conductor • Electric Generators • Transformers and Transmission of Power • A Changing Magnetic Flux Produces an Electric Field

  4. 29-1 Induced EMF Almost 200 years ago, Faraday looked for evidence that a magnetic field would induce an electric current with this apparatus:

  5. 29-1 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. 29-1 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. 29-2 Faraday’s Law of Induction; Lenz’s Law 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. 29-2 Faraday’s Law of Induction; Lenz’s Law This drawing shows the variables in the flux equation:

  9. 29-2 Faraday’s Law of Induction; Lenz’s Law 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. 29-2 Faraday’s Law of Induction; Lenz’s Law Conceptual Example 29-1: 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. 29-2 Faraday’s Law of Induction; Lenz’s Law 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. 29-2 Faraday’s Law of Induction; Lenz’s Law Example 29-2: 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. 29-2 Faraday’s Law of Induction; 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. 29-2 Faraday’s Law of Induction; Lenz’s Law Magnetic flux will change if the area of the loop changes.

  15. 29-2 Faraday’s Law of Induction; Lenz’s Law Magnetic flux will change if the angle between the loop and the field changes.

  16. 29-2 Faraday’s Law of Induction; Lenz’s Law Conceptual Example 29-3: 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. 29-2 Faraday’s Law of Induction; 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. 29-2 Faraday’s Law of Induction; Lenz’s Law Conceptual Example 29-4: Practice with Lenz’s law. In which direction is the current induced in the circular loop for each situation?

  19. 29-2 Faraday’s Law of Induction; Lenz’s Law Example 29-5: 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. 29-3 EMF Induced in a Moving Conductor This image shows another way the magnetic flux can change:

  21. 29-3 EMF Induced in a Moving Conductor The induced current is in a direction that tends to slow the moving bar – it will take an external force to keep it moving.

  22. 29-3 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).

  23. 29-3 EMF Induced in a Moving Conductor Example 29-6: 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?

  24. 29-3 EMF Induced in a Moving Conductor Example 29-8: 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?

  25. 29-6 Transformers and Transmission of Power A transformer consists of two coils, either interwoven or linked by an iron core. A changing emf in one induces an emf in the other. The ratio of the emfs is equal to the ratio of the number of turns in each coil:

  26. 29-6 Transformers and Transmission of Power This is a step-up transformer – the emf in the secondary coil is larger than the emf in the primary:

  27. 29-6 Transformers and Transmission of Power Energy must be conserved; therefore, in the absence of losses, the ratio of the currents must be the inverse of the ratio of turns:

  28. 29-6 Transformers and Transmission of Power Example 29-12: Cell phone charger. The charger for a cell phone contains a transformer that reduces 120-V ac to 5.0-V ac to charge the 3.7-V battery. (It also contains diodes to change the 5.0-V ac to 5.0-V dc.) Suppose the secondary coil contains 30 turns and the charger supplies 700 mA. Calculate (a) the number of turns in the primary coil, (b) the current in the primary, and (c) the power transformed.

  29. 29-6 Transformers and Transmission of Power Transformers work only if the current is changing; this is one reason why electricity is transmitted as ac.

  30. 29-7 A Changing Magnetic Flux Produces an Electric Field . A changing magnetic flux induces an electric field; this is a generalization of Faraday’s law. The electric field will exist regardless of whether there are any conductors around:

  31. Summary of Chapter 29 • Magnetic flux: • Changing magnetic flux induces emf: • Induced emf produces current that opposes original flux change.

  32. Summary of Chapter 29 . • Changing magnetic field produces an electric field. • General form of Faraday’s law:

  33. Summary of Chapter 29 • Transformer changes magnitude of voltage in ac circuit; ratio of currents is inverse of ratio of voltages: and

  34. Chapter 30Inductance

  35. Units of Chapter 30 • Mutual Inductance • Self-Inductance • Energy Stored in a Magnetic Field

  36. 30-1 Mutual Inductance Mutual inductance: a changing current in one coil will induce a current in a second coil: And vice versa; note that the constant M, known as the mutual inductance, is the same:

  37. 30-1 Mutual Inductance Unit of inductance: the henry, H: 1 H = 1 V·s/A = 1 Ω·s. A transformer is an example of mutual inductance.

  38. 30-1 Mutual Inductance Example 30-1: 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.

  39. 30-1 Mutual Inductance Conceptual Example 30-2: Reversing the coils. How would Example 30–1 change if the coil with turns was inside the solenoid rather than outside the solenoid?

  40. 30-2 Self-Inductance A changing current in a coil will also induce an emf in itself: Here, L is called the self-inductance:

  41. 30-2 Self-Inductance Example 30-3: Solenoid inductance. (a) Determine a formula for the self-inductance L of a tightly wrapped and long solenoid containing N turns of wire in its length l and whose cross-sectional area is A. (b) Calculate the value of L if N = 100, l = 5.0 cm, A = 0.30 cm2, and the solenoid is air filled.

  42. 30-2 Self-Inductance Conceptual Example 30-4: Direction of emf in inductor. Current passes through a coil from left to right as shown. (a) If the current is increasing with time, in which direction is the induced emf? (b) If the current is decreasing in time, what then is the direction of the induced emf?

  43. 30-2 Self-Inductance Example 30-5: Coaxial cable inductance. Determine the inductance per unit length of a coaxial cable whose inner conductor has a radius r1 and the outer conductor has a radius r2. Assume the conductors are thin hollow tubes so there is no magnetic field within the inner conductor, and the magnetic field inside both thin conductors can be ignored. The conductors carry equal currents I in opposite directions.

  44. 30-3 Energy Stored in a Magnetic Field Just as we saw that energy can be stored in an electric field, energy can be stored in a magnetic field as well, in an inductor, for example. Analysis shows that the energy density of the field is given by

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