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    • https://phys.libretexts.org/Courses/Grand_Rapids_Community_College/PH246_Calculus_Physics_II_(2025)/11%3A_Electromagnetic_Waves/11.02%3A_Maxwells_Equations_and_Electromagnetic_Waves
      James Clerk Maxwell (1831–1879) was one of the major contributors to physics in the nineteenth century. Although he died young, he made major contributions to the development of the kinetic theory of ...James Clerk Maxwell (1831–1879) was one of the major contributors to physics in the nineteenth century. Although he died young, he made major contributions to the development of the kinetic theory of gases, to the understanding of color vision, and to the nature of Saturn’s rings. He is  best known for having combined existing knowledge of the laws of electricity and of magnetism with insights of his own into a complete overarching electromagnetic theory, represented by Maxwell’s equations.
    • https://phys.libretexts.org/Courses/Georgia_State_University/GSU-TM-Physics_II_(2212)/08%3A_Electromagnetic_Waves/8.01%3A_Maxwells_Equations_and_Electromagnetic_Waves
      Then the z-component of the electric field between the plates as a function of time t is Ez(t)=V0d(1et/RC). Therefore, the z-component of the displacemen...Then the z-component of the electric field between the plates as a function of time t is Ez(t)=V0d(1et/RC). Therefore, the z-component of the displacement current Id between the plates is Id(t)=ϵ0AEz(t)t=ϵ0AV0d×1RCet/RC=V0Ret/RC, where we have used C=ϵ0Ad for the capacitance.
    • https://phys.libretexts.org/Courses/Berea_College/Electromagnetics_I/08%3A_Time-Varying_Fields/8.09%3A_Displacement_Current_and_Amperes_Law
      In this section, we generalize Ampere’s Law, previously encountered as a principle of magnetostatics. We shall now demonstrate that this equation is unreliable if the current is not steady; i.e., not ...In this section, we generalize Ampere’s Law, previously encountered as a principle of magnetostatics. We shall now demonstrate that this equation is unreliable if the current is not steady; i.e., not DC.
    • https://phys.libretexts.org/Bookshelves/University_Physics/University_Physics_(OpenStax)/University_Physics_II_-_Thermodynamics_Electricity_and_Magnetism_(OpenStax)/16%3A_Electromagnetic_Waves/16.02%3A_Maxwells_Equations_and_Electromagnetic_Waves
      James Clerk Maxwell (1831–1879) was one of the major contributors to physics in the nineteenth century. Although he died young, he made major contributions to the development of the kinetic theory of ...James Clerk Maxwell (1831–1879) was one of the major contributors to physics in the nineteenth century. Although he died young, he made major contributions to the development of the kinetic theory of gases, to the understanding of color vision, and to the nature of Saturn’s rings. He is  best known for having combined existing knowledge of the laws of electricity and of magnetism with insights of his own into a complete overarching electromagnetic theory, represented by Maxwell’s equations.
    • https://phys.libretexts.org/Courses/Georgia_State_University/GSU-TM-Introductory_Physics_II_(1112)/zz%3A_Back_Matter/10%3A_13.1%3A_Appendix_J-_Physics_Formulas_(Wevers)/1.02%3A_Electricity_and_Magnetism
      Electricity and magnetism from statics to electromagnetic fields as described by Maxwell's equations
    • https://phys.libretexts.org/Courses/Georgia_State_University/GSU-TM-Introductory_Physics_II_(1112)/09%3A_Electromagnetic_Waves/9.02%3A_Maxwells_Equations_and_Electromagnetic_Waves
      Then the z-component of the electric field between the plates as a function of time t is Ez(t)=V0d(1et/RC). Therefore, the z-component of the displacemen...Then the z-component of the electric field between the plates as a function of time t is Ez(t)=V0d(1et/RC). Therefore, the z-component of the displacement current Id between the plates is Id(t)=ϵ0AEz(t)t=ϵ0AV0d×1RCet/RC=V0Ret/RC, where we have used C=ϵ0Ad for the capacitance.
    • https://phys.libretexts.org/Learning_Objects/A_Physics_Formulary/Physics/02%3A_Electricity_and_Magnetism
      Electricity and magnetism from statics to electromagnetic fields as described by Maxwell's equations
    • https://phys.libretexts.org/Courses/Bowdoin_College/Phys1140%3A_Introductory_Physics_II%3A_Part_1/07%3A_Electromagnetic_Waves/7.02%3A_Maxwells_Equations_and_Electromagnetic_Waves
      James Clerk Maxwell (1831–1879) was one of the major contributors to physics in the nineteenth century. Although he died young, he made major contributions to the development of the kinetic theory of ...James Clerk Maxwell (1831–1879) was one of the major contributors to physics in the nineteenth century. Although he died young, he made major contributions to the development of the kinetic theory of gases, to the understanding of color vision, and to the nature of Saturn’s rings. He is  best known for having combined existing knowledge of the laws of electricity and of magnetism with insights of his own into a complete overarching electromagnetic theory, represented by Maxwell’s equations.
    • https://phys.libretexts.org/Courses/Kettering_University/Electricity_and_Magnetism_with_Applications_to_Amateur_Radio_and_Wireless_Technology/20%3A_Maxwell's_Equations/20.05%3A_Maxwells_Equations_and_Electromagnetic_Waves
      James Clerk Maxwell (1831–1879) was one of the major contributors to physics in the nineteenth century. Although he died young, he made major contributions to the development of the kinetic theory of ...James Clerk Maxwell (1831–1879) was one of the major contributors to physics in the nineteenth century. Although he died young, he made major contributions to the development of the kinetic theory of gases, to the understanding of color vision, and to the nature of Saturn’s rings. He is  best known for having combined existing knowledge of the laws of electricity and of magnetism with insights of his own into a complete overarching electromagnetic theory, represented by Maxwell’s equations.
    • https://phys.libretexts.org/Bookshelves/Electricity_and_Magnetism/Electromagnetics_I_(Ellingson)/08%3A_Time-Varying_Fields/8.09%3A_Displacement_Current_and_Amperes_Law
      In this section, we generalize Ampere’s Law, previously encountered as a principle of magnetostatics. We shall now demonstrate that this equation is unreliable if the current is not steady; i.e., not ...In this section, we generalize Ampere’s Law, previously encountered as a principle of magnetostatics. We shall now demonstrate that this equation is unreliable if the current is not steady; i.e., not DC.

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