Dissipative thermodynamic processes are essentially irreversible because they
produce entropy.
Planck regarded friction as the prime example of an irreversible thermodynamic process. In a process in which the temperature is locally continuously defined, the local density of rate of entropy production times local temperature gives the local density of dissipated power. A particular occurrence of a dissipative process cannot be described by a single individual
Hamiltonian formalism. A dissipative process requires a collection of admissible individual Hamiltonian descriptions, exactly which one describes the actual particular occurrence of the process of interest being unknown. This includes friction and hammering, and all similar forces that result in decoherence of energy—that is, conversion of
coherent or directed energy flow into an indirected or more
isotropic distribution of energy.
Energy "The conversion of mechanical energy into heat is called energy dissipation." –
François Roddier The term is also applied to the loss of energy due to generation of unwanted heat in electric and electronic circuits.
Computational physics In
computational physics, numerical dissipation (also known as "
Numerical diffusion") refers to certain side-effects that may occur as a result of a numerical solution to a differential equation. When the pure
advection equation, which is free of dissipation, is solved by a numerical approximation method, the energy of the initial wave may be reduced in a way analogous to a diffusional process. Such a method is said to contain 'dissipation'. In some cases, "artificial dissipation" is intentionally added to improve the
numerical stability characteristics of the solution.
Mathematics A formal, mathematical definition of dissipation, as commonly used in the mathematical study of
measure-preserving dynamical systems, is given in the article
wandering set. == Examples ==