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- https://phys.libretexts.org/Bookshelves/Electricity_and_Magnetism/Electromagnetics_and_Applications_(Staelin)/01%3A_Introduction_to_electromagnetics_and_electromagnetic_fields/1.01%3A_Review_of_FoundationsThis page introduces electromagnetics, covering the behavior of electric charges through laws like the Lorentz force and Maxwell's equations. It highlights significant advancements in electrical engin...This page introduces electromagnetics, covering the behavior of electric charges through laws like the Lorentz force and Maxwell's equations. It highlights significant advancements in electrical engineering and discusses conservation laws in physics, including momentum and charge. Key aspects include the interplay of electric charge, current, and photon energy, alongside relationships between frequency, wavelength, and light speed.
- https://phys.libretexts.org/Bookshelves/Electricity_and_Magnetism/Electromagnetics_and_Applications_(Staelin)/05%3A_Electromagnetic_Forces/5.03%3A_Forces_on_bound_charges_within_materialsThis page explores the calculation of forces on materials through Lorentz force law, Kelvin polarization, and magnetization forces, highlighting their dependence on electric and magnetic fields. It de...This page explores the calculation of forces on materials through Lorentz force law, Kelvin polarization, and magnetization forces, highlighting their dependence on electric and magnetic fields. It details the effects of electric field gradients on dielectrics and the implications of magnetic dipoles for current loops, presenting expressions for force density.
- https://phys.libretexts.org/Bookshelves/Quantum_Mechanics/Quantum_Mechanics_(Fowler)/06%3A_Charged_Particle_in_Magnetic_Field/6.01%3A_Charged_Particle_in_a_Magnetic_FieldClassically, the force on a charged particle in electric and magnetic fields is given by the Lorentz force law and is quite different from the conservative forces from potentials that we have dealt wi...Classically, the force on a charged particle in electric and magnetic fields is given by the Lorentz force law and is quite different from the conservative forces from potentials that we have dealt with so far, and the recipe for going from classical to quantum mechanics—replacing momenta with the appropriate derivative operators—has to be carried out with more care. We begin by demonstrating how the Lorentz force law arises classically in the Lagrangian and Hamiltonian formulations.
