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The Lorentz force is the force exerted by a magnetic field on a charged moving particle. As mentioned in a previous article (Motion of a Charge in a Uniform Magnetic Field), a moving charged particle will be pulled in a direction that is perpendicular to its current velocity. This is caused by the Lorentz force. This force can be calculated using the following equation: F⃗=qv⃗×B⃗\vec{F} = q \vec{v}\times \vec{B}

This means that the magnitude of the force is: ∣F⃗∣=q∣v⃗∣∣B⃗∣sin⁡θ|\vec{F}| = q |\vec{v}| |\vec{B}|\sin{\theta} where θ\theta equals the angle between v⃗\vec{v} and B⃗\vec{B}

The derivation of this formula involves complex calculus starting from the Biot-Savart Law, which is too lengthy and complicated to explain here.

However, there are certain interesting implications of the above formula, for example, we can derive the force experienced by a current carrying wire within a magnetic field. Note that the total force experienced by the wire is equal to the sum of all forces experienced by individual charges within the wire. Each charge has equal qq and their v⃗\vec{v} is the drifting velocity within the wire. We know that current is equal to drift velocity times charge divided by the length. We get: F⃗=qV⃗LL×B⃗\vec{F} = \frac{q\vec{V}}{L}L\times\vec{B} F⃗=LI⃗×B⃗\vec{F} = L\vec{I}\times\vec{B}

Type a concept, like “slope” or “photosynthesis”.

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