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Classical mechanics is a branch of physics which studies the deterministic motion of objects. It includes several different branches which represent specialised forms or stages of development:

Most of the above are in some way equivalent, either exactly equivalent or equivalent under special circumstances. For example, Lagrangian mechanics is exactly equivalent to Newtonian mechanics, always, but in its simplest form, Hamiltonian mechanics is only equivalent to the prior two when no frictional or drag forces are present. In other cases, an abovementioned branch of mechanics is a convenient specialised form: Newtonian mechanics can be used to deduce statistical mechanics, and statistical mechanics directly produces, more accurately, all of the results of thermodynamics.

Classical mechanics excludes any physics which involves the uncertainty principle, so quantum mechanics is not "classical", and is sometimes called modern physics by contrast. Some sources also exclude so-called "relativistic physics" from that category. However, a number of sources do include Einstein's mechanics, which in their view represents classical mechanics in its most developed and most accurate form.

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Journal of Mathematical Physics: All Topics

Symmetry, full symmetry groups, and some exact solutions to a generalized Davey--Stewartson system
Biao Li, Wang-Chuan Ye, and Yong Chen The Lie symmetry algebra of a generalized DaveyStewartson (GDS) system is obtained. The general element of this algebra depends on eight arbitrary functions of time, which has a KacMoodyVirasoro loop algebra structure and is isomorphic to that of the standard integrable DaveyStewartson equations und ... [J. Math. Phys. 49, 103503 (2008)] published Thu Oct 9, 2008.
On the classification of Darboux integrable chains
Ismagil Habibullin, Natalya Zheltukhina, and Asli Pekcan We study a differential-difference equation of the form t(n+1)=f(t(n),t(n+1),t(n)) with unknown t=t(n,x) depending on x and n. The equation is called a Darboux integrable if there exist functions F (called an x-integral) and I (called an n-integral), both of a finite number of variables x,t(n),t(n1) ... [J. Math. Phys. 49, 102702 (2008)] published Thu Oct 9, 2008.
Stochastic quantization for complex actions
G. Menezes and N. F. Svaiter We use the stochastic quantization method to study systems with complex valued path integral weights. We assume a Langevin equation with a memory kernel and Einstein's relations with colored noise. The equilibrium solution of this non-Markovian Langevin equation is analyzed. We show that for a large ... [J. Math. Phys. 49, 102301 (2008)] published Thu Oct 9, 2008.

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