1. A magnetic circuit containing a toroidal ferromagnetic core with a narrow air-gap is shown in Fig. 1.1. The toroidal ferromagnetic core has a circular cross-section and is made from soft cast steel (magnetisation curves are given in Fig. 1.2). The core is excited by two coils: Coil 1 (N₁ = 1500 turns) with terminals A and B, and Coil 2 (N₂ = 500 turns) with terminals C and D. The magnetic flux density in the core is Be = 0.7 T. Magnetic flux density, T B Air-gap 1, = 0.5 mm I (A) R₁ = 100 mm A Coil 1 (1500 turns) R₂ = 140 mm Coil 2 (500 turns) ° 1.5 Figure 1.1. 1.4 1.3 1.2 Nickel-iron alloy 1.1 10 0.9 Medium silicon sheet stee Soft cast steel 0.8 0.7 0.6 Cast iron 0.5 0.4 0.3 0.2 0.1 10 20 30 40 60 80 100 200 300 400 600 Magnetic field intensity, At/m 1000 2000 4000 10,000 (a) In magnetic circuit analysis, what is meant by the term 'fringing', and how are the effects of fringing usually accounted for in the calculation process? (b) Calculate the mean flux path length l of the magnetic core. (c) Calculate the reluctance Re (H¹) of the magnetic core. (d) Calculate the reluctance R, (H-1) of the air-gap. (Hint: As the air-gap is very narrow you can ignore the effects of fringing.) (e) Calculate the magnetic flux (Wb). (f) If terminal B (of Coil 1) is connected to terminal D (of Coil 2), calculate the current I required to establish a magnetic flux density B, = 0.7 T in the air-gap. (g) If terminal B (of Coil 1) is disconnected from terminal D (of Coil 2) and reconnected to terminal C (of Coil 2), calculate the new current I' required to establish a magnetic flux density B, = 0.7 T in the air-gap.
1. A magnetic circuit containing a toroidal ferromagnetic core with a narrow air-gap is shown in Fig. 1.1. The toroidal ferromagnetic core has a circular cross-section and is made from soft cast steel (magnetisation curves are given in Fig. 1.2). The core is excited by two coils: Coil 1 (N₁ = 1500 turns) with terminals A and B, and Coil 2 (N₂ = 500 turns) with terminals C and D. The magnetic flux density in the core is Be = 0.7 T. Magnetic flux density, T B Air-gap 1, = 0.5 mm I (A) R₁ = 100 mm A Coil 1 (1500 turns) R₂ = 140 mm Coil 2 (500 turns) ° 1.5 Figure 1.1. 1.4 1.3 1.2 Nickel-iron alloy 1.1 10 0.9 Medium silicon sheet stee Soft cast steel 0.8 0.7 0.6 Cast iron 0.5 0.4 0.3 0.2 0.1 10 20 30 40 60 80 100 200 300 400 600 Magnetic field intensity, At/m 1000 2000 4000 10,000 (a) In magnetic circuit analysis, what is meant by the term 'fringing', and how are the effects of fringing usually accounted for in the calculation process? (b) Calculate the mean flux path length l of the magnetic core. (c) Calculate the reluctance Re (H¹) of the magnetic core. (d) Calculate the reluctance R, (H-1) of the air-gap. (Hint: As the air-gap is very narrow you can ignore the effects of fringing.) (e) Calculate the magnetic flux (Wb). (f) If terminal B (of Coil 1) is connected to terminal D (of Coil 2), calculate the current I required to establish a magnetic flux density B, = 0.7 T in the air-gap. (g) If terminal B (of Coil 1) is disconnected from terminal D (of Coil 2) and reconnected to terminal C (of Coil 2), calculate the new current I' required to establish a magnetic flux density B, = 0.7 T in the air-gap.
Introductory Circuit Analysis (13th Edition)
13th Edition
ISBN:9780133923605
Author:Robert L. Boylestad
Publisher:Robert L. Boylestad
Chapter1: Introduction
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