michael webb
Another name for a reversible adiabatic process is an isentropic process. This type of process involves no heat exchange with the surroundings and is characterized by constant entropy.
A process where entropy remains the same is an isentropic process. In an isentropic process, there is no net change in the entropy of the system. This typically occurs when there is no heat transfer and the system is adiabatic and reversible.
No. All processes involving heat transfer are not reversible, since they result in an increase in entropy. Isothermal expansion implies heat transfer to maintain the system at a constant temperature. Normally an expanding gas would cool if there were no heat entering the system. Adiabatic processes involve no heat transfer and are reversible. The temperature can (and usually does) change during an adiabatic process.
entropy of system for a reversible adiabatic process is equal to zero. entropy of system for a irreversible adiabatic process (like free expansion) can be achieved by the following formula: Delta S= n Cp ln(V2/V1) + n Cv ln (P2/P1)
"Adiabatic process" refers to processes that take place in a closed system with no heat interaction with it's surroundings. "Isentropic process" refers to processes that take place in a closed system with no heat interaction with the surroundings (adiabatic process) and internally reversible. This is, no internal generation of entropy, entropy stays constant, which is what is meant by "isentropic". We can also say, an isentropic process is one where entropy stays constant, and no heat interaction of the system with the surroundings takes place (adiabatic process). Or, an adiabatic process can be irreversible, or reversible (isentropic).
In thermodynamics, an isentropic process is a reversible and adiabatic process, meaning there is no heat exchange with the surroundings. An adiabatic process, on the other hand, does not necessarily have to be reversible, but it also involves no heat exchange with the surroundings.
A reversible adiabatic process is a thermodynamic process that occurs without any heat exchange with the surroundings and can be reversed without any energy loss. This process is efficient and ideal for theoretical calculations. The implications of a reversible adiabatic process include the conservation of energy and the ability to achieve maximum work output.
because while cooling of gas in adiabatic expansion process , as it is a reversible procces the heat is lost while reversible work
An isoentropic process is a chemical or thermodynamic process in which entropy does not change. An example a reversible adiabatic process is isoentropic.
Another name for a reversible adiabatic process is an isentropic process. This type of process involves no heat exchange with the surroundings and is characterized by constant entropy.
No, a reversible adiabatic system is also known as isentropic.
the value of polytropic exponent "n" in reversible process will vary from 1 to adiabatic constant "gamma"
A process where entropy remains the same is an isentropic process. In an isentropic process, there is no net change in the entropy of the system. This typically occurs when there is no heat transfer and the system is adiabatic and reversible.
An adiabatic reversible process in thermodynamics is when heat transfer is completely prevented and the process is able to be reversed without any energy loss. This type of process is efficient and ideal for theoretical calculations. The implications include the ability to predict the behavior of ideal gases and the efficiency of certain thermodynamic systems.
In thermodynamics, adiabatic processes do not involve heat transfer, while isentropic processes are reversible and adiabatic.
The Carnot power cycle is based on four key principles: reversible isothermal expansion, reversible adiabatic expansion, reversible isothermal compression, and reversible adiabatic compression. The cycle involves transferring heat energy from a high-temperature reservoir to a working fluid, which then performs work by expanding and contracting. The efficiency of the Carnot cycle is determined by the ratio of the temperatures of the hot and cold reservoirs.
During reversible adiabatic expansion, the work done by the system is equal to the change in internal energy.