Matches in DBpedia 2016-04 for { ?s ?p "In classical electromagnetism, Ampère's circuital law, discovered by André-Marie Ampère in 1823, relates the integrated magnetic field around a closed loop to the electric current passing through the loop. James Clerk Maxwell derived it again using hydrodynamics in his 1861 paper On Physical Lines of Force and it is now one of the Maxwell equations, which form the basis of classical electromagnetism."@en }
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- Ampxc3xa8res_circuital_law abstract "In classical electromagnetism, Ampère's circuital law, discovered by André-Marie Ampère in 1823, relates the integrated magnetic field around a closed loop to the electric current passing through the loop. James Clerk Maxwell derived it again using hydrodynamics in his 1861 paper On Physical Lines of Force and it is now one of the Maxwell equations, which form the basis of classical electromagnetism.".
- Q51500 abstract "In classical electromagnetism, Ampère's circuital law, discovered by André-Marie Ampère in 1823, relates the integrated magnetic field around a closed loop to the electric current passing through the loop. James Clerk Maxwell derived it again using hydrodynamics in his 1861 paper On Physical Lines of Force and it is now one of the Maxwell equations, which form the basis of classical electromagnetism.".
- Ampxc3xa8res_circuital_law comment "In classical electromagnetism, Ampère's circuital law, discovered by André-Marie Ampère in 1823, relates the integrated magnetic field around a closed loop to the electric current passing through the loop. James Clerk Maxwell derived it again using hydrodynamics in his 1861 paper On Physical Lines of Force and it is now one of the Maxwell equations, which form the basis of classical electromagnetism.".
- Q51500 comment "In classical electromagnetism, Ampère's circuital law, discovered by André-Marie Ampère in 1823, relates the integrated magnetic field around a closed loop to the electric current passing through the loop. James Clerk Maxwell derived it again using hydrodynamics in his 1861 paper On Physical Lines of Force and it is now one of the Maxwell equations, which form the basis of classical electromagnetism.".