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Chapter 23 Magnetic Flux and Faraday’s Law of induction ...

Chapter 23 Magnetic flux and faraday s Law of inductionOutline23-1 Induced Electromotive Force23-2 Magnetic Flux23-3 faraday s Law of Induction23-4 Lens s Law23-5 Mechanical Work23-6 Generators and Motors23-10 Transformers23-3 faraday s Law of InductionFaraday s Lay of InductionSI unit: V)323( initialfinalinitialfinalTTNtN Where, N is the number of turns in the induced emf (voltage) is proportional to the rate of the Magnetic flux change with the time:Magnitude of the Induce EMFSI unit: V)423( initialfinalinitialfinalTTNtN Problem 23-15 The area of a 120-turn coil / loop oriented its plane perpendicular to a Magnetic field is m2. Find the average induced emf in this coil, if the Magnetic field reverses its direction in s. 222 T sBABABANNNtt t Solution:The Magnetic flux is changed from BA to BA.

23-3 Faradays Law of Induction Faradays Lay of Induction SI unit: V (23 3) final initial final initial T T N t N Where, N is the number of turns in the loop. The induced emf (voltage) is proportional to the rate of the magnetic flux change with the time:

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Transcription of Chapter 23 Magnetic Flux and Faraday’s Law of induction ...

1 Chapter 23 Magnetic flux and faraday s Law of inductionOutline23-1 Induced Electromotive Force23-2 Magnetic Flux23-3 faraday s Law of Induction23-4 Lens s Law23-5 Mechanical Work23-6 Generators and Motors23-10 Transformers23-3 faraday s Law of InductionFaraday s Lay of InductionSI unit: V)323( initialfinalinitialfinalTTNtN Where, N is the number of turns in the induced emf (voltage) is proportional to the rate of the Magnetic flux change with the time:Magnitude of the Induce EMFSI unit: V)423( initialfinalinitialfinalTTNtN Problem 23-15 The area of a 120-turn coil / loop oriented its plane perpendicular to a Magnetic field is m2. Find the average induced emf in this coil, if the Magnetic field reverses its direction in s. 222 T sBABABANNNtt t Solution:The Magnetic flux is changed from BA to BA.

2 According to (23-4),Example 23-2 Bar Magnetic InductionA bar magnet is moved rapidly toward a 40-turn circular coil of wire. As the magnet moves, the average value of Bcos over the area of the coil increase from to T in s. If the radius of the coils is cm, and the resistance of its wire is , find the magnet of (a)the induced emf and (b)the induced 23-2 Bar Magnet InductioninitialfinalinitialfinalTTNtN SolutionA1). The Magnetic flux through the loop, 2) The induced emf,B3) Using Ohm s law to find the current, ) () ()cos(mTmTABii ) () (cosmTmTABff )40(2523 23-4 Lens s LawLens s law can be used to explain the minus sign of faraday s law and determine the direction of the induced current in a s LawAn induced current always flows in a direction that opposes the change (of the Magnetic flux ) that causes it.

3 Two Cases:Figure 23-8 Applying Lenz s Law to a Magnet Moving Toward ( a), and Away (b)From a Current LoopThe Force also against the moving!Another ExampleFigure 23-9 Lenz s Law Applied to a Decreasing Magnetic FieldMotional EMFF igure 23-10 Motional emfA rod is falling down in a uniform B (because of gravity). Since the change of the Magnetic flux in the loop, it creates a to determine the direction of the current?Figure 23-11 Determining the Direction of an Induced CurrentLens s Law is applied to determined the direction of the current !SummaryFaraday s Lay of InductionSI unit: V)323( initialfinalinitialfinalTTNtN Lens s LawAn induced current always flows in a direction that opposes the change (of the Magnetic field) that causes it. Exercise 23-1 The induced emf in a single loop of wire has a magnitude of when the Magnetic flux is changed from T m2 to m2.

4 How much time is required for this change flux ? (1)0 . 5 0 NTmTmsV )423( initialfinalinitialfinalTTNtN We hav


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