サインイン

Two long, straight, and parallel current-carrying conductors exert a force of equal magnitude on one another. The direction of the force depends on the current direction in the conductors.

The force exerted by the magnetic field due to the first conductor over a finite length of the second conductor is given as the product of the current in the second conductor and the vector product of the length vector along the current element and the field due to the first conductor. According to the right-hand rule for the cross-product, the force on the second conductor is directed towards the first conductor. Similarly, the field due to the second conductor exerts an equal magnitude of force on the first conductor and is directed towards the second conductor. Thus the forces are attractive when the current in the both the conductors flow in the same direction. Reversing the direction of current in any one of the conductors makes the force repulsive.

Since the wires are very long, the force is often expressed in terms of the force per unit length, which forms the basis for the definition of the unit 'Ampere' for the current. Quantitatively, one Ampere is the amount of current present in each of the two parallel conductors of an infinite length separated by one meter in empty space, which causes each conductor to experience a force of exactly 1 N/m.

This force is responsible for the pinch effect in electric arcs and other plasmas. The force is apparent if the overall charge density is zero; otherwise, the Coulomb repulsion overwhelms the magnetic attraction. An attractive force squeezes currents into a smaller tube in an electric arc, where charges are moving parallel to one another. In large circuit breakers, such as those used in neighbourhood power distribution systems, the pinch effect can concentrate an arc between plates of a switch trying to break a large current, burn holes, and even ignite the equipment. Another example of the pinch effect is found in solar plasma, where jets of ionized material, such as solar flares, are shaped by magnetic forces.

タグ
Magnetic ForceParallel CurrentsCurrent carrying ConductorsRight hand RuleForce Per Unit LengthAmpere DefinitionPinch EffectElectric ArcsCoulomb RepulsionSolar PlasmaIonized Material

章から 29:

article

Now Playing

29.6 : Magnetic Force Between Two Parallel Currents

磁場の発生源

3.3K 閲覧数

article

29.1 : 移動電荷による磁場

磁場の発生源

8.0K 閲覧数

article

29.2 : ビオ・サバール法

磁場の発生源

5.5K 閲覧数

article

29.3 : ビオ・サバールの法則:問題解決

磁場の発生源

2.2K 閲覧数

article

29.4 : 細い直線ワイヤーによる磁場

磁場の発生源

4.5K 閲覧数

article

29.5 : 2本の直線ワイヤによる磁場

磁場の発生源

2.2K 閲覧数

article

29.7 : 電流ループの磁場

磁場の発生源

4.1K 閲覧数

article

29.8 : 磁場の発散とカール

磁場の発生源

2.6K 閲覧数

article

29.9 : アンペアの法則

磁場の発生源

3.5K 閲覧数

article

29.10 : アンペアの法則:問題解決

磁場の発生源

3.4K 閲覧数

article

29.11 : ソレノイド

磁場の発生源

2.4K 閲覧数

article

29.12 : ソレノイドの磁場

磁場の発生源

3.5K 閲覧数

article

29.13 : トロイド

磁場の発生源

2.7K 閲覧数

article

29.14 : 磁気ベクトルポテンシャル

磁場の発生源

445 閲覧数

article

29.15 : 磁化された物体による電位

磁場の発生源

227 閲覧数

See More

JoVE Logo

個人情報保護方針

利用規約

一般データ保護規則

研究

教育

JoVEについて

Copyright © 2023 MyJoVE Corporation. All rights reserved