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Force acting between two long, parallel, current-carrying conductors
© D Hoult 2008
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Current I2 flows through the field produced by current I1 (and vice versa)
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Current I2 flows through the field produced by current I1 (and vice versa)
Flux density near conductor 2 produced by I1 is given by
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Current I2 flows through the field produced by current I1 (and vice versa)
Flux density near conductor 2 produced by I1 is given by µo I1 B = 2 p r assuming that the medium is a vacuum (or air)
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Force acting on a length L of wire 2 is
F = I2 L B
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Force acting on a length L of wire 2 is
F = I2 L B Therefore, force per unit length acting on wire 2 is
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Force acting on a length L of wire 2 is
F = I2 L B Therefore, force per unit length acting on wire 2 is µo I1 I2 F = L 2 p r
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µo I1 I2 F = L 2 p r 1 A is the current which,
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µo I1 I2 F = L 2 p r 1 A is the current which, when flowing in each of two infinitely long, straight, parallel conductors,
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µo I1 I2 F = L 2 p r 1 A is the current which, when flowing in each of two infinitely long, straight, parallel conductors, separated by 1m,
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µo I1 I2 F = L 2 p r 1 A is the current which, when flowing in each of two infinitely long, straight, parallel conductors, separated by 1m, in a vacuum,
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µo I1 I2 F = L 2 p r 1 A is the current which, when flowing in each of two infinitely long, straight, parallel conductors, separated by 1m, in a vacuum, produces a force per unit length of 2 × 10-7 N m-1
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µo I1 I2 F = L 2 p r 1 A is the current which, when flowing in each of two infinitely long, straight, parallel conductors, separated by 1m, in a vacuum, produces a force per unit length of 2 × 10-7 N m-1
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