Search results
Results From The WOW.Com Content Network
In thermodynamics, an isobaric process is a type of thermodynamic process in which the pressure of the system stays constant: ΔP = 0. The heat transferred to the system does work, but also changes the internal energy (U) of the system. This article uses the physics sign convention for work, where positive work is work done by the system.
The work done in a process is the area beneath the process path on a P-V diagram. Figure 2 If the process is isobaric, then the work done on the piston is easily calculated. For example, if the gas expands slowly against the piston, the work done by the gas to raise the piston is the force F times the distance d .
Isobaric; Isochoric; Isothermal; Adiabatic; ... An isentropic process is an idealized thermodynamic process that is both ... The reversible work done on a system by ...
Thermodynamic work is one of the principal kinds of process by which a thermodynamic system can interact with and transfer energy to its surroundings. This results in externally measurable macroscopic forces on the system's surroundings, which can cause mechanical work, to lift a weight, for example, [1] or cause changes in electromagnetic, [2] [3] [4] or gravitational [5] variables.
The net work equals the area inside because it is (a) the Riemann sum of work done on the substance due to expansion, minus (b) the work done to re-compress. Because the net variation in state properties during a thermodynamic cycle is zero, it forms a closed loop on a P-V diagram.
When a system expands in an isobaric process, the thermodynamic work, , done by the system on the surroundings is the product, , of system pressure, , and system volume change, , whereas is said to be the thermodynamic work done on the system by the surroundings. The change in internal energy of the system is:
Isobaric process: p 1 = p 2, p = constant ... Work done by an expanding gas Process = ... Net work done in cyclic processes = = Kinetic theory ...
An isentropic process is customarily defined as an idealized quasi-static reversible adiabatic process, of transfer of energy as work. Otherwise, for a constant-entropy process, if work is done irreversibly, heat transfer is necessary, so that the process is not adiabatic, and an accurate artificial control mechanism is necessary; such is ...