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Physics theorems

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Noether's theorem
physical law that differentiable symmetries correspond to conservation laws
Stokes' theorem
theorem in vector calculus
parallel axis theorem
theorem in planar dynamics
virial theorem
general equation that relates the time-averaged total kinetic energy of a stable system consisting of N particles, bound by potential forces, with that of the time-averaged total potential energy
equipartition theorem
theorem
spin-statistics theorem
theorem that, in a Lorenz-invariant local quantum field theory, particles with integer spins are bosons, while particles with half-integer spins are fermions
Carnot's theorem
in thermodynamics, the principle that any heat engine operating between the same two thermal reservoirs cannot have an efficiency greater than a reversible heat engine operating between the same reservoirs
Clausius theorem
theorem that for a thermodynamic system undergoing a thermodynamic cycle, the following inequality holds: ∮ δ𝑄/𝑇 ≤ 0, where δ𝑄 is heat absorbed by the system and 𝑇 is the temperature
Poynting's theorem
theorem in physics, showing the conservation of energy for the electromagnetic field, expressed in the form of a partial differential equation developed by British physicist John Henry Poynting
Bertrand's theorem
theorem that, among central-force potentials with bound orbits, there are only 2 types of central-force scalar potentials such that all bound orbits are closed: inverse square and radial harmonic
Buckingham π theorem
dimensional analysis theorem
Earnshaw's theorem
Mathematical demonstration applied in electro-magnetism
Kutta–Joukowski theorem
theorem
tennis racket theorem
theorem that, in a 3d rigid body with 3 principal axes, rotation around 1st and 3rd principal axes is stable, but rotation around 2nd principal axis is not
H-theorem
In classical statistical mechanics, the ' H-theorem', introduced by Ludwig Boltzmann in 1872, describes the tendency of the quantity H (defined below) to decrease in a nearly-ideal gas of molecules. As this quantity H was meant to represent the entropy of thermodynamics, the H-theorem was an early demonstration of the power of statistical mechanics as it claimed to derive the second law of thermodynamics—a statement about fundamentally irreversible processes—from reversible microscopic mechanics. It is thought to prove the second law of thermodynamics, albeit under the assumption of low-entrop
Varignon's theorem (mechanics)
theorem
Shell theorem
Simplified gravity models for objects inside or outside a spherically symmetrical body
Lami's theorem
equation relating the magnitudes of three coplanar, concurrent and non-collinear vectors, which keeps an object in static equilibrium, with the angles directly opposite to the corresponding vectors
Goldstone boson
massless boson that must be present in a quantum system with spontaneously broken symmetry
fluctuation-dissipation theorem
theorem
König's theorem
named after Samuel König
perpendicular axis theorem
Mathematical theorem
Mermin–Wagner theorem
theorem about the impossibility of spontaneous symmetry breaking in two-dimensional systems at finite temperature
Bohr–Van Leeuwen theorem
theorem
Clairaut's theorem
formula for the surface gravity on a viscous rotating ellipsoid in hydrostatic equilibrium under the action of its gravitational field and centrifugal force
Wick's theorem
theorem transforming derivatives into combinatorics problems applied in quantum field theory
Betti's theorem
Reciprocal work theorem in engineering
optical theorem
theorem in physics
Taylor–Proudman theorem
free will theorem
quantum physics theorem that, given relativitistic causality, quantized spin and entanglement, if 2 experimenters each having one of a pair of entanged particles can freely decide what to measure, the measured results aren’t determined by prior state
Homoeoid
shell bounded by two concentric, similar ellipses or ellipsoids