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Closed system
Closed system
from Wikipedia

A closed system is a natural physical system that does not allow transfer of matter in or out of the system, although the transfer of energy is allowed in the contexts of certain fields (e.g. physics, chemistry, engineering, etc).

Physics

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In classical mechanics

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In nonrelativistic classical mechanics, a closed system is a physical system that does not exchange any matter with its surroundings, and is not subject to any net force whose source is external to the system.[1][2] A closed system in classical mechanics would be equivalent to an isolated system in thermodynamics. Closed systems are often used to limit the factors that can affect the results of a specific problem or experiment.

In thermodynamics

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Properties of isolated, closed, and open systems in exchanging energy and matter

In thermodynamics, a closed system can exchange energy (as heat or work) but not matter, with its surroundings. An isolated system cannot exchange any heat, work, or matter with the surroundings, while an open system can exchange energy and matter.[3][4][5][6][7][8][9] (This scheme of definition of terms is not uniformly used, though it is convenient for some purposes. In particular, some writers use 'closed system' where 'isolated system' is used here.[10][11])

For a simple system, with only one type of particle (atom or molecule), a closed system amounts to a constant number of particles. However, for systems which are undergoing a chemical reaction, there may be all sorts of molecules being generated and destroyed by the reaction process. In this case, the fact that the system is closed is expressed by stating that the total number of each elemental atom is conserved, no matter what kind of molecule it may be a part of. Mathematically:

where is the number of j-type molecules, is the number of atoms of element in molecule and is the total number of atoms of element in the system, which remains constant, since the system is closed. There will be one such equation for each different element in the system.

In thermodynamics, a closed system is important for solving complicated thermodynamic problems. It allows the elimination of some external factors that could alter the results of the experiment or problem thus simplifying it. A closed system can also be used in situations where thermodynamic equilibrium is required to simplify the situation.

In quantum physics

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This equation, called Schrödinger's equation, describes the behavior of an isolated or closed quantum system, that is, by definition, a system which does not interchange information (i.e. energy and/or matter) with another system. So if an isolated system is in some pure state |ψ(t) ∈ H at time t, where H denotes the Hilbert space of the system, the time evolution of this state (between two consecutive measurements).[12]

where i is the imaginary unit, ħ is the Planck constant divided by , the symbol /t indicates a partial derivative with respect to time t, Ψ (the Greek letter psi) is the wave function of the quantum system, and Ĥ is the Hamiltonian operator (which characterizes the total energy of any given wave function and takes different forms depending on the situation).

In chemistry

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In chemistry, a closed system is where no reactants or products can escape, only heat can be exchanged freely (e.g. an ice cooler). A closed system can be used when conducting chemical experiments where temperature is not a factor (i.e. reaching thermal equilibrium).

In engineering

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In an engineering context, a closed system is a bound system, i.e. defined, in which every input is known and every resultant is known (or can be known) within a specific time.

See also

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References

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
In thermodynamics and physics, a closed system is defined as a that exchanges energy—such as or work—with its surroundings but does not allow the transfer of across its boundary. This contrasts with an open system, which permits both energy and exchange, and an , which exchanges neither. The concept is fundamental to analyzing and transformations within bounded quantities of , such as a fixed volume of gas in a piston-cylinder assembly. The first law of , which expresses the , is particularly applied to closed systems through the equation ΔE=QW\Delta E = Q - W, where ΔE\Delta E represents the change in the system's total (including internal, kinetic, and potential components), QQ is the added to the system, and WW is the work done by the system. For many practical cases, such as stationary processes where kinetic and potential energies remain constant, this simplifies to focus on changes in , ΔU=QW\Delta U = Q - W. This formulation underscores that within a closed system is neither created nor destroyed but can convert between forms, enabling precise predictions of state changes independent of the process path. Closed systems are ubiquitous in and physical applications, including the of an , where fuel and oxidizer react without mass loss. In , air parcels are modeled as closed systems to study thermodynamic processes like adiabatic expansion without moisture exchange. These models facilitate the design of efficient heat engines, refrigeration cycles, and chemical reactors, where understanding energy balances ensures optimal performance and compliance with physical laws.

Fundamental Concepts

Basic Definition

A closed system is defined as a that can exchange , such as or work, with its surroundings but does not allow the transfer of across its boundaries. This concept is fundamental in , where the system's mass remains constant while interactions influence its internal state. Key attributes of a closed system include boundaries that are impermeable to but permeable to forms like , mechanical work, or pressure-volume changes. This contrasts with common intuition, where "sealed" or "closed" might suggest no interactions whatsoever; in scientific terms, closure pertains specifically to conservation, permitting controlled flows. Representative examples illustrate these attributes: a sealed -cylinder assembly containing gas, where the piston enables work through volume changes and via the cylinder walls, but no gas escapes. Similarly, a thermos approximates a closed system for short durations, retaining liquid while slowly exchanging minimal with the environment. The boundary is conceptualized as a real or imaginary mathematical surface that delineates the from its surroundings, facilitating of exchanges without crossing. This boundary enables precise modeling of transfers in theoretical and practical contexts.

System Classifications

In and physics, systems are classified into three primary categories based on their exchanges with the surroundings: open systems, which can exchange both and ; closed systems, which exchange but not ; and isolated systems, which exchange neither nor . This typology builds on the of a boundary that delineates interactions with the external environment. Isolated systems represent theoretical idealizations, as achieving complete isolation from all external influences is unattainable in reality; a conceptual example is a perfect vacuum chamber with no , mechanical, or radiative contact with the outside. Closed systems, while also approximations, are more feasible in controlled settings, such as a beaker sealed with a lid to block transfer while permitting exchange through the boundary. The classification into open, closed, and isolated systems is a standard convention in modern thermodynamics, evolving from 19th-century foundational work on energy conservation. To illustrate the distinctions, the following table compares the permissible exchanges across system types:
System TypeMatter ExchangeEnergy Exchange (e.g., heat or work)
OpenYesYes
ClosedNoYes
IsolatedNoNo

Applications in Physics

In Classical Mechanics

In classical mechanics, a closed system is defined as a collection of particles or bodies where no matter enters or leaves the system, and the net external force acting on it is zero, leading to the application of conservation laws for momentum and angular momentum. The conservation of linear momentum is a key principle for such systems, stating that the total linear momentum remains constant over time. This arises from Newton's third law, where internal forces between particles cancel in pairs, producing no net change in the system's momentum. The total linear momentum P\vec{P}
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