Phys 0175 - Lecture 25

Phys 0175 - Lecture 25 - Lecture 25 (Mar. 18, 2009):...

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Lecture 25 (Mar. 18, 2009): Magnetic Fields due to Currents (cont’d): Applications of Ampere’s Law (solenoid, toroid) Current-carrying coil acting as a magnetic dipole Illustrative examples
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Magnetic field produced by a solenoid: The magnetic field inside the solenoid becomes more uniform as the number of turns per unit length increases.
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Apply Ampere’s Law to find the magnetic field inside a long solenoid with n turns per unit length: Therefore in the center of the solenoid: B = μ 0 in ( 29 0 0 b c d a b enc a b c d a B ds B ds B ds B ds B ds B ds Bh i i nh μ = + + + = = = = r r r r r r r r r r r r g g g g g g Ñ
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Variation of the magnetic field B at points along the axis of a solenoid of length 4a and diameter 2a:
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A toroidal solenoid (aka toroid): In the center of the toroid, in the region enclosed by the coils: The magnetic field is zero inside (r<a) and outside (r>b). 0 0 2 iN B in r μ π = = a b
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This note was uploaded on 04/06/2009 for the course PHYS 0175 taught by Professor Koehler during the Spring '08 term at Pittsburgh.

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Phys 0175 - Lecture 25 - Lecture 25 (Mar. 18, 2009):...

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