BENG 130 Lecture 3: Lecture 03

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29 Oct 2016
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Classical view of the first law (and applications: internal energy: (cid:1847)=(cid:1847)(cid:3033) (cid:1847)=(cid:1843)+(cid:1849) Work done on the system is positive. Work done by the system is negative. Q and w are not state functions, except in special cases (when the. (cid:1847) is a state function: heat: (cid:1843)=((cid:1846)(cid:3033) (cid:1846)) other is 0) To achieve the same temperature differential in wood as in metal, the amount of energy needed is much more in wood. This difference is taken into account as heat capacity (c) C will depend on variable of state. The heat required to change the heat of a system depends on the properties of the system: work. We will compare a reversible and an irreversible process. Imagine we start at state 1, go to state 2, and end at state 1. Net work, change in internal energy, and net heat are 0. I start at p1v1, then go to p2v2: the work is the red area.

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