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  2. Irreversible process - Wikipedia

    en.wikipedia.org/wiki/Irreversible_process

    An irreversible process increases the total entropy of the system and its surroundings. The second law of thermodynamics can be used to determine whether a hypothetical process is reversible or not. Intuitively, a process is reversible if there is no dissipation. For example, Joule expansion is irreversible because initially the system is not ...

  3. Gibbs–Helmholtz equation - Wikipedia

    en.wikipedia.org/wiki/Gibbs–Helmholtz_equation

    The definition of the Gibbs function is = + where H is the enthalpy defined by: = +. Taking differentials of each definition to find dH and dG, then using the fundamental thermodynamic relation (always true for reversible or irreversible processes): = where S is the entropy, V is volume, (minus sign due to reversibility, in which dU = 0: work other than pressure-volume may be done and is equal ...

  4. Adiabatic process - Wikipedia

    en.wikipedia.org/wiki/Adiabatic_process

    An adiabatic process (adiabatic from Ancient Greek ἀδιάβατος (adiábatos) 'impassable') is a type of thermodynamic process that occurs without transferring heat between the thermodynamic system and its environment. Unlike an isothermal process, an adiabatic process transfers energy to the surroundings only as work and/or mass flow.

  5. Fanno flow - Wikipedia

    en.wikipedia.org/wiki/Fanno_flow

    In fluid dynamics, Fanno flow (after Italian engineer Gino Girolamo Fanno) is the adiabatic flow through a constant area duct where the effect of friction is considered. [1] Compressibility effects often come into consideration, although the Fanno flow model certainly also applies to incompressible flow. For this model, the duct area remains ...

  6. Thermodynamic process - Wikipedia

    en.wikipedia.org/wiki/Thermodynamic_process

    An adiabatic process is a process in which there is no matter or heat transfer, because a thermally insulating wall separates the system from its surroundings. For the process to be natural, either (a) work must be done on the system at a finite rate, so that the internal energy of the system increases; the entropy of the system increases even ...

  7. Adiabatic accessibility - Wikipedia

    en.wikipedia.org/wiki/Adiabatic_accessibility

    Lieb and Yngvason's definition of adiabatic accessibility is: A state is adiabatically accessible from a state , in symbols (pronounced X 'precedes' Y), if it is possible to transform into in such a way that the only net effect of the process on the surroundings is that a weight has been raised or lowered (or a spring is stretched/compressed ...

  8. Gouy–Stodola theorem - Wikipedia

    en.wikipedia.org/wiki/Gouy–Stodola_theorem

    An irreversible process produces some work , which is less than . The lost work is then W l o s t = W r e v − W a c t u a l {\displaystyle W_{lost}=W_{rev}-W_{actual}} ; in other words, W l o s t {\displaystyle W_{lost}} is the work which was lost or not exploited during the process due to irreversibilities.

  9. List of adiabatic concepts - Wikipedia

    en.wikipedia.org/wiki/List_of_adiabatic_concepts

    Adiabatic (from Gr. ἀ negative + διάβασις passage; transference) refers to any process that occurs without heat transfer. This concept is used in many areas of physics and engineering. Notable examples are listed below.