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Motional Electromotive Force

1890
  • Hendrik Lorentz
Homopolar generator demonstrating motional electromotive force in electricity and magnetism.

(generated image for illustration only)

Motional EMF is generated when a conductor moves through a magnetic field. The magnetic component of the Lorentz force, \(\mathbf{F} = q(\mathbf{v} \times \mathbf{B})\), acts on the charge carriers within the conductor, causing them to move and create a charge separation. This separation establishes an electric field and a potential difference. The resulting EMF is given by the line integral \(\mathcal{E} = \oint (\mathbf{v} \times \mathbf{B}) \cdot d\mathbf{l}\).

Motional EMF is a direct consequence of the Lorentz force acting on mobile charges inside a conductor that is moving relative to a magnetic field. As the conductor moves with velocity \(\mathbf{v}\) through a magnetic field \(\mathbf{B}\), the free charges (electrons) within it experience a magnetic force \(\mathbf{F}_m = q(\mathbf{v} \times \mathbf{B})\). This force is perpendicular to both the velocity and the magnetic field, causing the charges to accumulate at one end of the conductor, leaving the other end with a net positive charge. This charge separation creates an internal electrostatic field \(\mathbf{E}_e\) that opposes the further migration of charges. Equilibrium is reached when the electrostatic force \(\mathbf{F}_e = q\mathbf{E}_e\) exactly balances the magnetic force, i.e., \(q\mathbf{E}_e = -q(\mathbf{v} \times \mathbf{B})\).

The effective electric field experienced by the charges, \(\mathbf{E}_{eff} = \mathbf{v} \times \mathbf{B}\), is a non-conservative field that drives the current. The EMF is the work done per unit charge by this effective field integrated along the length of the conductor. For a straight wire of length \(L\) moving perpendicular to a uniform field \(B\), the EMF simplifies to \(\mathcal{E} = BLv\). While motional EMF can be seen as a specific case of Faraday’s law of induction (in terms of changing flux), the Lorentz force perspective provides a more microscopic explanation of the mechanism responsible for the charge separation and the resulting voltage.

UNESCO Nomenclature: 2205
– Electricity and Magnetism

Type

Physical Phenomenon

Disruption

Substantial

Usage

Widespread Use

Precursors

  • Michael Faraday’s discovery of electromagnetic induction
  • James Clerk Maxwell’s equations of electromagnetism
  • Discovery of the electron by J.J. Thomson

Applications

  • homopolar generators
  • railguns
  • magnetohydrodynamic (mhd) generators
  • eddy current brakes
  • electrodynamic tethers in space

Patents:

NA

Potential Innovations Ideas

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Related to: motional EMF, Lorentz force, magnetic field, conductor, velocity, generator, charge separation, induction.

Historical Context

Motional Electromotive Force

1887
1888
1889
1890
1890
1895
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1885
1887
1889
1890
1890
1895
1895
1896

(if date is unknown or not relevant, e.g. "fluid mechanics", a rounded estimation of its notable emergence is provided)

Related Invention, Innovation & Technical Principles

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