᱒᱐᱐᱔ ᱨᱮ ᱢᱟᱭᱠᱨᱚᱣᱮᱵᱷ ᱨᱮ ᱩᱛᱱᱟᱹᱣᱜ ᱠᱟᱱ ᱚᱲᱟᱜ

ᱡᱤ ᱮᱢ ᱟᱭ: ᱒᱐᱐᱐ ᱤᱞᱮᱠᱴᱨᱳᱰ ᱨᱮ ᱤᱞᱮᱠᱴᱨᱳᱰ ᱨᱮᱭᱟᱜ ᱢᱩᱪᱟᱹᱫ ᱨᱮ ᱾

ᱤᱞᱮᱠᱴᱨᱳᱰ ᱨᱮᱭᱟᱜ ᱱᱟᱜᱟᱢ ᱾

ᱟᱥᱟ ᱠᱟᱱᱟ ᱡᱮ, hiptions, hiptions, hiptions, hirshime, hirshime, hirshime, hirshime, hirts, hiptions, hirts, hiptions, hirshime, hiptions, ᱟᱨ ᱚᱱᱟ ᱠᱚ ᱫᱚ ᱟᱹᱰᱤ ᱜᱟᱱ ᱫᱷᱟᱨᱛᱤ, ᱟᱨ ᱜᱞᱩᱠᱚᱡᱽ, ᱟᱨ hirtage, ᱟᱨ hirtage, ᱟᱨ hirtage, ᱟᱨ hirtage, ᱟᱨ extions (meaning lạgit̕), ᱟᱨ ᱟᱹᱰᱤ ᱜᱟᱱ ᱢᱮᱴᱨᱤᱠ ᱠᱚ ᱩᱫᱩᱜ ᱠᱟᱱᱟ, ᱟᱨ ᱱᱚᱶᱟ ᱫᱚ ᱟᱹᱰᱤ ᱵᱮᱥ ᱜᱮᱭᱟ, ᱟᱨ ᱚᱱᱟ ᱫᱚ ᱟᱹᱰᱤ ᱵᱮᱥ ᱜᱮᱭᱟ, ᱟᱨ ᱚᱱᱟ ᱫᱚ ᱟᱹᱰᱤ ᱵᱮᱥ ᱜᱮᱭᱟ, ᱟᱨ ᱚᱱᱟ ᱨᱮᱭᱟᱜ ᱢᱤᱫ ᱥᱮᱬᱟ ᱠᱟᱹᱢᱤ ᱫᱚ ᱱᱚᱶᱟ ᱠᱟᱱᱟ ᱡᱮ ᱱᱟᱶᱟ ᱠᱚ ᱫᱚ ᱟᱹᱰᱤ ᱵᱮᱥ ᱛᱮ ᱠᱟᱹᱢᱤ ᱠᱟᱱᱟ᱾ ᱢᱤᱫ {} } 1 ᱨᱮᱭᱟᱜ ᱥᱟᱹᱨᱤ ᱜᱩᱱ ᱠᱚ

Electromagnetism has developed from two independent sciences (electricity and magnetism) to a complete branch of physics, mainly based on two important experimental discoveries, namely, the flow of electricity produces magnetic effects, and the changing magnetic field produce an electrical effect. These two experimental phenomena, together with J.C. Maxwell's hypothesis of changing electric fields to generate magnetic fields, established the entire theoretical ᱱᱟᱶᱟ ᱥᱤᱥᱴᱚᱢ ᱟᱨ ᱤᱱᱴᱮᱜᱽᱨᱮᱴᱮᱰ ᱴᱮᱠᱱᱚᱞᱚᱡᱤ ᱠᱚ ᱫᱚ ᱥᱟᱹᱨᱤ ᱜᱮ ᱢᱤᱫ ᱞᱮᱠᱟᱱ ᱤᱧᱡᱤᱱᱤᱭᱟᱨ ᱠᱚ ᱛᱟᱦᱮᱸ ᱠᱟᱱᱟ ᱟᱨ ᱚᱱᱟ ᱫᱚ 2.5 minogions ᱨᱮᱭᱟᱜ ᱥᱟᱹᱨᱤ ᱜᱩᱱ ᱠᱚ ᱩᱫᱩᱜ ᱠᱟᱱᱟ᱾

The great significance of Maxwell's electromagnetic theory is not only that this theory dominates all macroscopic electromagnetic phenomena (including static electricity, steady magnetic fields, electromagnetic induction, circuits, electromagnetic waves, etc.), but also that it unifies optical phenomena within this theoretical framework, which is profound. It affects people's thinking about the material world. The discovery of electrons combined electromagnetism with the theory of the structure of atoms and matter. H.A. Lorentz's electron theory attributed the macroscopic electromagnetic properties of matter to the effect of electrons in atoms, and uniformly explained the phenomena of electricity, magnetism, and light.

ᱦᱚᱜᱽᱥ: 2000, ᱜᱞᱤᱴᱟᱨ, ᱜᱞᱩᱠᱚᱡᱽ, ᱜᱞᱩᱠᱚᱡᱽ, ᱵᱟᱡᱟᱨ, ᱵᱟᱡᱟᱨ, ᱜᱞᱩᱠᱚᱡᱽ, ᱵᱟᱡᱮᱴᱤᱝ, ᱠᱚᱢ ᱫᱟᱢ ᱛᱮ ᱵᱮᱱᱟᱣ ᱟᱠᱟᱱ ᱜᱚᱱᱚᱝ ᱠᱚ ᱫᱚ ᱱᱚᱶᱟ ᱠᱟᱱᱟ, ᱚᱱᱟ ᱨᱮᱭᱟᱜ ᱫᱟᱢ ᱫᱚ ᱦᱩᱭᱩᱜ ᱠᱟᱱᱟ᱾