A physical system can be described by classical physics when it satisfies conditions such that the laws of classical physics are approximately valid.
In practice, physical objects ranging from those larger than atoms and molecules to macroscopic and astronomical objects, can be well-described (understood) with classical mechanics. Beginning at the atomic level and lower, the laws of classical physics break down and generally do not provide a correct description of nature. Electromagnetic fields and forces can be described well by classical electrodynamics at length scales and field strengths large enough that quantum mechanical effects are negligible. Unlike quantum physics, classical physics is generally characterized by the principle of complete determinism, although deterministic interpretations of quantum mechanics do exist.
From the point of view of classical physics as being non-relativistic physics, the predictions of general and special relativity are significantly different from those of classical theories, particularly concerning the passage of time, the geometry of space, the motion of bodies in free fall, and the propagation of light. Historically, light was reconciled with classical mechanics by assuming the existence of a stationary medium through which light propagated, the luminiferous aether, which was later shown not to exist.
Comparison to quantum physics
Decoherence describes how the laws of quantum physics give rise to classical physics through loss of interference.[6]
↑Barut, Asim O. (1980) [1964]. "Introduction to Classical Mechanics". Electrodynamics and Classical Theory of Fields & Particles. New York: Dover Publications. ISBN9780486640389.
12Krane, Kenneth S. (2020). Modern physics (4ed.). Hoboken, New Jersey: John Wiley & Sons, Inc. ISBN978-1-119-49548-2.
↑Bacciagaluppi, Guido (2025). "The Role of Decoherence in Quantum Mechanics,". In Zalta, Edward; Nodelman, Uri (eds.). The Stanford Encyclopedia of Philosophy (Winter 2025ed.). Wetaphysics Research Lab, Stanford University.