Prerequisite materialElectromagnetic Induction and Alternating CurrentSimple Harmonic Motion

Electrical Oscillations and Electromagnetic Waves

We first show why the electric charge in an LC circuit oscillates. We then use the laws governing electric and magnetic fields to determine how electromagnetic waves propagate through a vacuum and how fast they travel.

電荷が初めの半分になった瞬間、電流の大きさは最大値の何倍か?

The equations explain the phenomenon

  1. 1The electric potential differences across the coil and capacitor give the circuit equation.L dIdt=⁠−QC……
  2. 2Substituting I = dQ/dt allows comparison with the spring equation.d²Qdt²=⁠−QL C……
  3. 3The initial conditions determine the expressions for electric charge and electric current.Q = Q₀ cos ωt⁠,I = −Q₀ω sin ωt……
  4. 4Multiplying the circuit equation by I gives conservation of energy.½ Q²C+⁠½ L I²=⁠½ Q₀²C……
  5. 5The electric current can be calculated when the electric charge is halved.|I|Imax=⁠√32……
  6. 6Add resistance and check whether the electric charge changes sign.L d²Qdt²+⁠R dQdt+⁠QC=⁠0……
  7. 7Values from a radio circuit give its oscillation frequency.f=⁠12π √(L C)……
  8. 8An additional law connects changing electric and magnetic fields.∮ B · dl=⁠μ₀ I + μ₀ ε₀ dΦEdt……
  9. 9Changes in electric and magnetic fields propagate as waves.E ⊥ B⁠,E ⊥ direction of propagation⁠,B ⊥ direction of propagation……
  10. 10The electromagnetic wave speed is calculated from ε₀ and μ₀.c=⁠1√(ε₀ μ₀)……
  11. Further exploration: wavelengths and familiar electromagnetic waves
  12. 11Electromagnetic waves are arranged by wavelength.λ=⁠cf……