We have introduced the connection between reversibility and maximum work for the special case of a perfect gas undergoing expansion. Later (in Section 3.5) we shall see that it applies to all substances and to all kinds of work.
We have introduced the connection between reversibility and maximum work forthe special case of a perfect gas undergoing expansion. Later (in Section 3.5) we shallsee that it applies to all substances and to all kinds of work.