Electromagnetism in the aether
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Here’s the explanation of electromagnetism in the aether lattice model in ASCII format:
ELECTROMAGNETISM IN THE AETHER LATTICE MODEL 1. COULOMB'S LAW (ELECTRIC FORCE) Electric force arises from lattice tension gradients between charges: F_e = k_a * (q1 * q2) / r^2 Where: :F_e = Electric force :q1, q2 = Electric charges (lattice distortions) :r = Distance between charges :k_a = Aether electrostatic constant (depends on lattice properties). 2. BIOT-SAVART LAW (MAGNETIC FIELD) A moving charge creates a magnetic field by aligning distortions in the lattice: B = (mu_a / 4pi) * (q * v * sin(theta)) / r^2 Where: :B = Magnetic field strength :q = Charge (distortion magnitude) :v = Velocity of charge (rate of lattice distortion propagation) :theta = Angle between velocity and observation point :mu_a = Aether magnetic permeability. 3. FARADAY'S LAW (INDUCED ELECTRIC FIELD) Changing magnetic fields induce electric fields: curl(E) = - (dB / dt) Where: :E = Electric field (tension gradient in lattice) :B = Magnetic field (alignment of distortions) :t = Time. 4. AMPÈRE'S LAW WITH MAXWELL'S CORRECTION Changing electric fields induce magnetic fields: curl(B) = mu_a * J + mu_a * epsilon_a * (dE / dt) Where: :B = Magnetic field :J = Current density (rate of charge motion through lattice) :E = Electric field :epsilon_a = Aether permittivity (related to lattice compressibility). 5. ELECTROMAGNETIC WAVE PROPAGATION Electromagnetic waves propagate as coupled lattice oscillations: laplacian(E) = mu_a * epsilon_a * (d^2E / dt^2) laplacian(B) = mu_a * epsilon_a * (d^2B / dt^2) Where the speed of light in the lattice is: c = 1 / sqrt(mu_a * epsilon_a) 6. NOVEL PREDICTIONS :Lattice Quantization: :Electric and magnetic fields might show discrete changes at small scales if the lattice is quantized. :Nonlinear Effects: :Strong fields could modify local lattice properties, leading to deviations from classical predictions. :Variable Constants: :The values of mu_a and epsilon_a depend on lattice density and rigidity, which may vary in high-energy regions.