PHZ3400-09 Problem Set 2: Difference between revisions
(New page: '''Problem 1''' Consider the famous Van der Waals equation describing the liquid-gas transition: <math>(P + \frac {aN^2}{V^2})(V - Nb) = NkT</math>.) |
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<math>(P + \frac {aN^2}{V^2})(V - Nb) = NkT</math>. | <math>(P + \frac {aN^2}{V^2})(V - Nb) = NkT</math>. | ||
a) Show that introducing the average volume per particle <math>v=V/N</math>, this equation can be expressed as a cubic polynomial in <math>v</math>. | |||
b) By looking for extrema (<math>dP/dv = 0</math>) of the <math>P(v)</math> isotherms, show that the pressure is monotonic function of the volume, above a certain critical temperature <math>T_c</math>. Show that: | |||
<math>T_c = \frac{8}{27}\frac{a}{b}\!</math>, <math>V_c = 3Nb\!</math>, and <math>P_c = \frac{1}{27}\frac{a}{b^2}\!</math>. | |||
c) Show that the Van der Waals equation can be written in universal form | |||
<math>(\frac{P}{P_c} + 3(\frac{V_c}{V})^2)(3\frac{V}{V_c} - 1) = 8\frac{T}{T_c}\!</math>, | |||
and that | |||
<math>\frac{P_cV_c}{T_c} = \frac{3}{8}</math>. | |||
d) The isothermal compressibility is defined as: | |||
<math>\Kappa = -\left \frac{dV}{dP}\right_T</math>. |
Revision as of 20:15, 2 February 2011
Problem 1
Consider the famous Van der Waals equation describing the liquid-gas transition:
.
a) Show that introducing the average volume per particle , this equation can be expressed as a cubic polynomial in .
b) By looking for extrema () of the isotherms, show that the pressure is monotonic function of the volume, above a certain critical temperature . Show that:
, , and .
c) Show that the Van der Waals equation can be written in universal form
,
and that
.
d) The isothermal compressibility is defined as: Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \Kappa = -\left \frac{dV}{dP}\right_T} .