# Magnetic Force Between Current-Carrying Conductors ## Introduction The interaction between two parallel current-carrying conductors gives rise to a magnetic force. This force results directly from the magnetic fields generated by the moving charges within the wires. The direction of this force, whether attractive or repulsive, depends entirely on the relative direction of the currents in the two conductors. ## Direction of the Force The nature of the force between two parallel wires is determined by the direction of their currents. ### Attractive Force: Currents in the Same Direction When two conductors carry currents flowing in the **same direction**, they attract each other. The magnetic field produced by each wire circulates around it. Between the wires, these two fields are in opposite directions, leading to a region of weaker net magnetic field. Outside the wires, the fields reinforce each other. The force acts from the stronger external field towards the weaker internal field, pushing the wires together. A point exists between the conductors where the magnetic fields from each wire are equal and opposite, cancelling each other out completely. This is the **neutral point**. Its position depends on the magnitude of the currents; it is exactly midway if the currents are equal. ### Repulsive Force: Currents in Opposite Directions When two conductors carry currents flowing in opposite directions, they repel each other. In this configuration, the magnetic fields between the wires are in the same direction, combining to create a region of stronger net magnetic field. The force acts from this stronger internal field towards the weaker external fields, pushing the wires apart. ## Mathematical Expression for the Force The magnitude of the force between two long, parallel current-carrying wires can be calculated mathematically. ### Magnetic Field of a Single Wire The magnetic field ($B$) at a distance $r$ from a long, straight conductor carrying a current $I$ is given by Ampere's Law: $$B = \frac{\mu_0 I}{2 \pi r}$$ ### Force on a Wire in a Magnetic Field A wire of length $L$ carrying a current $I_2$ placed in an external magnetic field $B_1$ experiences a force: $$F = B_1 I_2 L$$ ### Force Per Unit Length By combining these two principles, the force that wire 1 (current $I_1$) exerts on wire 2 (current $I_2$) can be determined. 1. The magnetic field produced by wire 1 at the location of wire 2 is $B_1 = \frac{\mu_0 I_1}{2 \pi r}$. 2. The force on a length $L$ of wire 2 due to this field is $F_{12} = B_1 I_2 L = \left(\frac{\mu_0 I_1}{2 \pi r}\right) I_2 L$. This gives the force per unit length: $$\frac{F}{L} = \frac{\mu_0 I_1 I_2}{2 \pi r}$$ By Newton's Third Law, the force exerted by wire 2 on wire 1 ($F_{21}$) is equal in magnitude and opposite in direction to $F_{12}$. They form an action-reaction pair. ## Definition of Ampere The SI unit of current, the Ampere, is defined based on the force between two parallel conductors. One Ampere is that constant current which, if maintained in two straight parallel conductors of infinite length, of negligible circular cross-section, and placed 1 metre apart in vacuum, would produce between these conductors a force equal to $2 \times 10^{-7}$ Newtons per metre of length. ## Possible Questions and Answers **Q:** Why do parallel currents in the same direction attract? **A:** Because the magnetic fields between the wires oppose and partially cancel each other, creating a weaker field region between them. The force pushes the wires from the stronger outer field toward this weaker inner field. **Q:** What is a neutral point? **A:** It is a point between two conductors with parallel currents where the magnetic fields from both wires are equal in magnitude and opposite in direction, resulting in a net magnetic field of zero. | Key Formula | | | :--- | :--- | | **Force per unit length between two parallel wires** | $$\frac{F}{L} = \frac{\mu_0 I_1 I_2}{2 \pi r}$$ | This interaction is a fundamental principle in electromagnetism, essential for understanding the behavior of in magnetic fields.

Magnetic Force Between Current Carrying Conductors | Electromagnetism | Physics 11