Classical Field Theory

Action, field Lagrangians, field equations, symmetries, and conservation laws.

General idea of the topic

Classical field theory generalizes Lagrangian and Hamiltonian analytical mechanics from discrete systems with finite degrees of freedom to continuous field distributions with infinite degrees of freedom across space and time. It forms the foundational unifying framework of classical physics, allowing the systematic derivation of Maxwell's electrodynamics, continuum mechanics, and relativistic field equations from variational action principles.

This node covers continuous Lagrangian densities, Euler-Lagrange field equations, Noether's theorem, energy-momentum stress tensors, and gauge invariance.

What you will truly understand

You will understand how Noether's theorem maps every continuous symmetry of the Lagrangian density L(ϕ,∂μϕ)\mathcal{L}(\phi, \partial_\mu \phi) to a conserved 4-current ∂μJμ=0\partial_\mu J^\mu = 0 and an invariant conserved charge Q=∫J0d3xQ = \int J^0 d^3x.

You will construct gauge-invariant field actions by coupling matter fields to the electromagnetic potential AμA_\mu through the minimal gauge covariant derivative Dμ=∂μ−iqAμD_\mu = \partial_\mu - i q A_\mu.

Recommended learning route

  1. Action principle for continuum fields: Lagrangian density L\mathcal{L}, Hamilton's principle δS=0\delta S = 0, and covariant Euler-Lagrange equations.
  2. Symmetries and Noether's theorem: spacetime translations, canonical energy-momentum tensor TμνT^{\mu\nu}, and global internal U(1)U(1) phase invariance.
  3. Covariant electromagnetic field: Faraday tensor Fμν=∂μAν−∂νAμF_{\mu\nu} = \partial_\mu A_\nu - \partial_\nu A_\mu, Maxwell Lagrangian density L=−14FμνFμν\mathcal{L} = -\frac{1}{4} F_{\mu\nu} F^{\mu\nu}, and local gauge freedom.
  4. Relativistic scalar and spinor fields: Klein-Gordon real/complex fields, Dirac field Lagrangian, and plane-wave mode expansions.

Physical criterion you must acquire

Recognizing that demanding local gauge invariance fundamentally mandates the introduction of gauge connection fields that mediate physical interactions.

Connection with real problems

  • Covariant electrodynamics and relativistic antenna beam pattern synthesis.
  • Continuum elasticity, acoustic phonon fields, and magnetohydrodynamic wave systems.
  • Indispensable conceptual prerequisite for canonical quantization and Quantum Field Theory (QFT).

Final goal of the topic

Master the variational Lagrangian formulation of classical fields to systematically extract equations of motion, conserved Noether currents, and gauge interactions.

Topics in this section

  • Action and Field Lagrangian

    Introduces action, Lagrangian density, and Euler-Lagrange equations for classical fields.

  • Scalar Fields

    Representation of scalar quantities continuously distributed across space and time.

  • Vector Fields

    Representation of quantities with magnitude and direction distributed across space and time.

  • Euler-Lagrange Equations for Fields

    Derives field dynamics from a local Lagrangian density. Theory, formulas, worked examples and interactive graphs.

  • Noether Theorem in Fields

    Links continuous field symmetries to conserved currents and charges. Theory, formulas, worked examples and interactive graphs.

  • Stress-Energy Tensor

    Describes energy-momentum density, flux, and stresses in fields and matter.

  • Waves and Field Modes

    Describes wave propagation and normal modes of classical fields. Theory, formulas, worked examples and interactive graphs.