Page 37 - Bruno Linder Elementary Physical Chemistry
P. 37

August 18, 2010 11:36      9in x 6in     b985-ch03     Elementary Physical Chemistry





                               22                   Elementary Physical Chemistry

                               the statement is usually expressed in the form of two equivalent Principles:

                                  Claussius Principle: It is not possible to construct an engine
                                  which has the sole effect of transferring heat from a lower temper-
                                  ature reservoir to a higher one.

                               or,
                                  Kelvin–Planck Principle: It is not possible to construct an
                                  engine which has the sole effect of converting heat entirely into
                                  work.

                               It can be shown that either statement leads to the conclusion that dq rev /T
                               is path-independent and this statement is used to define entropy. It can be
                               shown also rigorously that statements (3.3)–(3.6) are valid.


                               3.2. Carnot Cycle
                               The standard way of proving the foregoing statements is by means of a
                               Carnot cycle. This is a reversible cycle consisting of an isothermal expansion
                               of a gas from a volume V 1 toavolume V 2 at a temperature T 2 , followed
                               by an adiabatic (no heat transfer) expansion of the gas from V 2 to V ,then

                                                                                         2
                               followed by an isothermal compression from V to V at a temperature T 1 ,


                                                                      2     1
                               and finally followed by an adiabatic compression from V to V 1 .

                                                                               1
                                  The system (gas) is connected to an engine, consisting of two heat
                               reservoirs, one at the higher temperature, T 2, and the other at the lower
                               temperature, T 1 (see Figs. 3.1 and 3.2). The heat, q 2 , extracted from the
                               high temperature reservoir T 2 is used to run the Carnot cycle, thereby
                               generating work, −w, and returning the remaining heat q 1 to the reservoir
                               at the lower temperature T 1 .[Note: q 2 and q 1 are symbolic representations:
                               q 2 is positive, and q 1 is negative. Work done on the surrounding has a
                               negative sign because we use the convention that w represents the work
                               done by the surrounding on the system, and thus the work done by the
                               system must be −w.]


                               3.3. Engine Efficiency
                               The efficiency, ξ, is defined as the work done by the system in a complete
                               cycle divided by the heat absorbed at the higher temperature, i.e.

                                                                                           (3.7)
                                                          ξ = −w/q 2
   32   33   34   35   36   37   38   39   40   41   42