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Derived Variables

Last time we introduced two different kinds of thermodynamic variables: Extensive and Intensive

Intensive variables can be specified point by point; i.e.

\begin{center}\vbox{\input{tables/fields}
}\end{center}

They do not depend on the size of the body.


Extensive variables depend on the size of the system in question. They are additive.

$\displaystyle \input{equations/ext-examp}$ (04-4)

We can define ``derived quantities'' (or densities) by scaling:1

$\displaystyle \frac{\mbox{some Extensive quantity}} {\mbox{some other Extensive quantity}}$ (04-5)

and size of system drops out and these quantities are not additive.

However, the derived intensive quantities still `act' like extensive quantities regarding where they appear in `work' terms:


Extensive variables can be distinguished from intensive variables by the way they add when you add two systems at equilibrium (See Eq. [*]). Derived quantities don't sum like extensive or intensive quantities, but one can derive a rule for their addition. The trick in involves realizing that the derived quantities are ``extensive variables in hiding.'' One can turn them into extensive variables and then use the appropriate rule to add, for instance, consider the combined density, \bgroup\color{blue}$ \rho_{AB}$\egroup of two bodies with volumes \bgroup\color{blue}$ V_A$\egroup, \bgroup\color{blue}$ V_B$\egroup, and masses \bgroup\color{blue}$ M_A$\egroup, \bgroup\color{blue}$ M_B$\egroup:

\begin{displaymath}\begin{split}\rho_{AB} & = \frac{M_A + M_B}{V_A + V_B} = \fra...
...ac{V_B}{V_A + V_B} \rho_B = f_A \rho_A + f_B \rho_B \end{split}\end{displaymath} (04-6)

where the \bgroup\color{blue}$ f_i$\egroup are volume fractions. The derived quantities or densities have a ``weighted addition'' rule.


Examples of derived intensive quantities are:

$\displaystyle \input{equations/density-examp}$ (04-7)

$\displaystyle \input{equations/dspecies-examp}$ (04-8)


This last equation introduces another derived intensive quantity called a molar quantity:

$\displaystyle \frac{\mbox{Extensive variable}}{\mbox{Total Number of moles}}= \...
...h{{N}^{\mbox{total}}}} \equiv \ensuremath{\overline{\mbox{Extensive variable}}}$ (04-9)

For example, molar species number

$\displaystyle \input{equations/molar-conc-ex}$ (04-10)

This quantity is used so often that it gets its own name--mole fraction and symbol \bgroup\color{blue}$ X_j$\egroup

$\displaystyle \input{equations/molar-U-def}$ (04-11)


\bgroup\color{blue}\fbox{Note on Notation:
we use the over-line as the notation to specify that a quantity is molar.}\egroup


Partial Quantities

For intensive quantities, it is sometimes useful to associate the contributions of each type of existing chemical species to the value of the intensive quantities. Each separate contribution is called a partial quantity, for example for pressure,

$\displaystyle \input{equations/part-press-def}$ (04-12)

\bgroup\color{blue}$ P_j$\egroup is defined as the partial pressure of species \bgroup\color{blue}$ j$\egroup

Question: Does the product of two extensive variables produce a similar extensive variable?

Question: Does the product of two intensive variables produce an intensive variable?

Question: Under what conditions does the product of an intensive variable and an extensive variable produce an extensive variable?


next up previous
Next: Equivalence of heat and Up: Lecture_04_web Previous: Some Example State Functions
W. Craig Carter 2002-09-10