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Maxwell's Equations

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Maxwell's equations are a set of coupled partial differential equations that, together with the Lorentz force law, form the foundation of classical electromagnetism, describing how electric and magnetic fields are generated by charges, currents and changing fields.

Facts
Proposed YearSourced to the subject's own account
1865 1
Proposed BySourced to the subject's own account
James Clerk Maxwell 1
Cross-Tradition Connections

Proposed By

Additional Source Maxwell's Equations (Wikipedia)Lead section (edge: proposed-by, Maxwell)
Sources
1. Maxwell's Equations (Wikipedia)
WikipediaLead section (entity-description)
Quote, Lead section (entity-description)
Maxwell's equations are a set of coupled partial differential equations that, together with the Lorentz force law, form the foundation of classical electromagnetism.
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1. Maxwell's Equations (Wikipedia)
WikipediaLead section (proposed-year)
Quote, Lead section (proposed-year)
James Clerk Maxwell presented the equations in their unified form in his 1865 paper A Dynamical Theory of the Electromagnetic Field.
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1. Maxwell's Equations (Wikipedia)
WikipediaLead section (proposed-by)
Quote, Lead section (proposed-by)
James Clerk Maxwell presented the equations in their unified form in his 1865 paper A Dynamical Theory of the Electromagnetic Field.
View the Source
1. Maxwell's Equations (Wikipedia)
WikipediaProposed By: James Clerk Maxwell, Lead section (edge: proposed-by, Maxwell)
Quote, Proposed By: James Clerk Maxwell, Lead section (edge: proposed-by, Maxwell)
Maxwell's equations are named after the physicist and mathematician James Clerk Maxwell, who, in 1861 and 1862, published an early form of the equations that included the Lorentz force law.
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