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A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.

Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line joining the source to the field point. The magnitude of the magnetic field is proportional to the particle’s speed, and it also depends on the sine of the angle; the velocity vector subtends with the line joining the source and the field point (Equation1).

Equation1

Considering a unit vector along a distance r to a field point, the equation for the magnetic field at field point P can be expressed as the cross-product of the velocity vector and the unit vector, as shown in Equation 2.

Equation2

The constant, µo, is the permeability of free space, and its value is 4π x 10−7 T·m·A−1.

The unit of the magnetic field is the Tesla, named after Nikola Tesla, and is expressed as “T”.

Tags
Magnetic FieldMoving ChargesElectric FieldPoint ChargeVelocity VectorDistancePerpendicularMagnetic Field MagnitudeSine AngleCross productPermeability Of Free SpaceTeslaNikola Tesla

Aus Kapitel 29:

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29.1 : Magnetic Field due to Moving Charges

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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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29.7 : Magnetfeld einer Stromschleife

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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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