Lorentz force
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In physics, the Lorentz force is the force exerted on a charged particle in an electromagnetic field. The particle will experience a force due to electric field of qE, and due to the magnetic field qv × B. Combined they give the Lorentz force equation (or law):
- <math>\mathbf{F} = q (\mathbf{E} + \mathbf{v} \times \mathbf{B}),</math>
where
- F is the force (in newtons)
- E is the electric field (in volts per meter)
- B is the magnetic field (in webers per square meter, or equivalently, teslas)
- q is the electric charge of the particle (in coulombs)
- v is the instantaneous velocity of the particle (in meters per second)
- and × is the cross product.
Thus a positively charged particle will be accelerated in the same linear orientation as the E field, but will curve perpendicularly to the B field according to the right-hand rule.
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Alternative form
Equivalently, we can express the Lorentz force law in terms of the electric charge density ρ and current density J as
- <math>\mathbf{F} = \int_V ( \rho \mathbf{E} + \mathbf{J} \times \mathbf{B}) \cdot dV</math>
Applications
The Lorentz force is a principle exploited in many devices including:
- Cyclotrons and other circular path particle accelerators
- Homopolar generators
- Magnetrons
- Magnetoplasmadynamic thrusters
- Mass spectrometers
- Railguns
- Generators
- Motors
See also
Reference
da:Lorentzkraft de:Lorentzkraft es:Fuerza de Lorentz fr:Force de Lorentz ko:로렌츠 힘 it:Forza di Lorentz he:כוח לורנץ nl:Lorentzkracht ja:ローレンツ力 sl:Lorentzova sila zh:洛仑兹力