on physical lines of force造句

• James Clerk Maxwell drew attention to this fact in his 1861 paper " On Physical Lines of Force ".
• He added this displacement current to Amp鑢e's circuital law at equation 112 in his 1861 paper " On Physical Lines of Force ".
• It is later clarified in his concept of a sea of molecular vortices that appears in his 1861 paper " On Physical Lines of Force ".
• From this, Maxwell concluded that light was a form of electromagnetic radiation : he first stated this result in 1862 in " On Physical Lines of Force ".
• Between 1861 and 1865, James Clerk Maxwell developed and published Maxwell's equations, which explained and united all of On Physical Lines of Force " in 1861.
• Maxwell's contribution to science in producing these equations lies in the correction he made to Amp鑢e's circuital law in his 1861 paper " On Physical Lines of Force ".
• The idea was conceived by James Clerk Maxwell in his 1861 paper " On Physical Lines of Force, Part III " in connection with the displacement of electric particles in a dielectric medium.
• In his 1865 paper titled A Dynamical Theory of the Electromagnetic Field, Maxwell utilized the correction to Amp鑢e's circuital law that he had made in part III of his 1861 paper On Physical Lines of Force.
• James Clerk Maxwell began working on On Physical Lines of Force " he modelled these magnetic lines of force using a sea of molecular vortices that he considered to be partly made of aether and partly made of ordinary matter.
• This amalgamation, which Maxwell himself had actually originally made at equation ( 112 ) in " On Physical Lines of Force ", is the one that modifies Amp鑢e's Circuital Law to include Maxwell's displacement current.
• In Maxwell's 1861 paper " On Physical Lines of Force ", equation ( 77 ) is identical to the Lorentz force equation albeit that it is written in cartesian coordinates and split into x, y, and z components.
• In part VI of " A Dynamical Theory of the Electromagnetic Field ", Maxwell uses the correction to Amp鑢e's Circuital Law made in part III of his 1862 paper, " On Physical Lines of Force ", which is defined as displacement current, to derive the electromagnetic wave equation.
• In Maxwell's 1861 paper'On Physical Lines of Force', magnetic field strength "'H "'was directly equated with pure vorticity ( spin ), whereas "'B "'was a weighted vorticity that was weighted for the density of the vortex sea.
• It is of particular interest to note that Maxwell includes a \ mu ( \ mathbf { v } \ times \ mathbf { H } ) term in his expression for the " electromotive force " at equation " On Physical Lines of Force " " quite some time before Lorentz thought of it.