Thermodynamics Flashcards
System
A system is specified by a description of the material it contains and the boundaries that contain it. There are two main classifications of systems.
Open System
Material may enter into or exit from the system. Many sources call this type of system a control volume.
Closed System
Material may not enter into or exit from the system. Many sources call this type of system a control mass.
Reversible process
A process for which there exists another process that can return the system to its original state, leaving no net effect on the system’s environment. A true reversible process cannot be achieved in practice.
The utility of investigating reversible processes is that they provide a limit to the change in state that can occur in any process.
Irreversible Process
A process for which there does not exist another process that can return the system to its original state, without changing the state of the environment. All real processes are irreversible.
Adiabatic
A process for which all transfers of energy occur through work interactions
Constant property
A process during which the value of one property remains constant. When such a process occurs, the analysis of the process is usually simplified.
Isometric
Constant-volume process (energy transfer to a closed rigid container)
Isothermal
Constant-temperature process (condensation or evaporation in a heat exchanger)
Isobaric
Constant-pressure process (weighted piston and cylinder)
Isentropic
Constant-entropy process (ideal turbine)
Isenthalpic
Constant-enthalpy process (flow through a valve)
Clausius Statement
It is impossible to devise a cyclic machine that produces, as its only effect, the transfer of energy through a heat interaction from a low-temperature body to a high-temperature body
Kelvin-Planck Statement
It is impossible to devise a cyclic machine that will have no other effect than to extract energy from a reservoir through a heat interaction and to produce an equal amount of energy through a work interaction.
Gyftopolous-Baretta Statement
Among all possible states of system with a given value of energy and with a given set of values of the amounts of constituents and the parameters, there exists one and only one equilibrium state. Moreover, starting from any state of the system, it is possible to reach an equilibrium state with an arbitrarily specified set of values of the amounts of constituents and the parameters.