Consider a circular loop with a radius a, that carries a current I. The magnetic field due to the current at an arbitrary point P along the axis of the loop can be calculated using the Biot-Savart law.

Figure1

Let axial point P be a distance x from the center of the loop. The magnetic field at P, produced by an infinitesimal current element dl, is directed at an angle θ. The current element and the unit vector along the line joining P are perpendicular at all points on the loop. Substituting this and rewriting r in terms of x and a gives the magnitude of the magnetic field due to the current element.

Equation1

The magnetic field can be resolved into two components: perpendicular and parallel to the axis. Due to different current elements around the loop, all the perpendicular components of the magnetic field cancel each other. Integrating all the parallel components over all the current elements along the loop, gives the magnetic field on the axis of a circular loop.

Equation2

For a coil of n closely spaced loops of the same radius, the total field is n times the field due to a single loop.

Tags
Magnetic FieldCurrent LoopRadiusBiot Savart LawAxial PointCurrent ElementUnit VectorPerpendicular ComponentsParallel ComponentsIntegrationCoilClosely Spaced Loops

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29.7 : Magnetic Field Of A Current Loop

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29.1 : Magnetfeld durch bewegte Ladungen

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29.2 : Biot-Savart-Gesetz

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29.3 : Biot-Savart-Gesetz: Problemlösung

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29.4 : Magnetfeld aufgrund eines dünnen geraden Drahtes

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29.5 : Magnetfeld durch zwei gerade Drähte

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29.6 : Magnetische Kraft zwischen zwei parallelen Strömen

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29.8 : Divergenz und Krümmung des Magnetfeldes

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29.9 : Das Amperesche Gesetz

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29.10 : Amperes Gesetz: Problemlösung

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29.11 : Magnetspulen

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29.12 : Magnetfeld eines Magneten

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29.13 : Ringkerne

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29.14 : Magnetisches Vektorpotential

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29.15 : Potential durch ein magnetisiertes Objekt

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