Chapter 11: Problem 34
Why is \(\Delta H_{\text {vap }}\) usually larger than \(\Delta H_{\text {fusion }}\) ?
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Chapter 11: Problem 34
Why is \(\Delta H_{\text {vap }}\) usually larger than \(\Delta H_{\text {fusion }}\) ?
These are the key concepts you need to understand to accurately answer the question.
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The density of a sample of metal was measured to be \(22.67 \mathrm{~g} / \mathrm{cm}^{3}\). An X-ray diffraction experiment measures the edge of a face- centered cubic cell as \(383.3 \mathrm{pm}\). Calculate the atomic mass of the metal and identify it.
Iodine has \(\mathrm{mp}=113.7^{\circ} \mathrm{C}\) and \(\mathrm{bp}=184.4^{\circ} \mathrm{C}\). What, if any, phase changes take place under the following conditions at \(1.0\) atm pressure? (a) The temperature of a solid sample is held at \(113.7{ }^{\circ} \mathrm{C}\) while heat is added. (b) The temperature of a sample is lowered from \(452 \mathrm{~K}\) to \(389 \mathrm{~K}\).
Bromine has \(T_{\mathrm{t}}=-7.3^{\circ} \mathrm{C}, P_{\mathrm{t}}=44 \mathrm{~mm} \mathrm{Hg}, T_{\mathrm{c}}=315^{\circ} \mathrm{C}\), and \(P_{c}=102 \mathrm{~atm} .\) The density of the liquid is \(3.1 \mathrm{~g} / \mathrm{cm}^{3}\), and the density of the solid is \(3.4 \mathrm{~g} / \mathrm{cm}^{3}\). Sketch a phase diagram for bromine, and label all points of interest.
Use the following data to sketch a phase diagram for krypton: \(T_{\mathrm{t}}=-169{ }^{\circ} \mathrm{C}, P_{\mathrm{t}}=133 \mathrm{~mm} \mathrm{Hg}, T_{\mathrm{c}}=-63{ }^{\circ} \mathrm{C}, P_{\mathrm{c}}=54 \mathrm{~atm}\) \(\mathrm{mp}=-156.6^{\circ} \mathrm{C}, \mathrm{bp}=-152.3^{\circ} \mathrm{C} .\) The density of solid kryp- ton is \(2.8 \mathrm{~g} / \mathrm{cm}^{3}\), and the density of the liquid is \(2.4 \mathrm{~g} / \mathrm{cm}^{3}\). Can a sample of gaseous krypton at room temperature be liquefied by raising the pressure?
The following table gives the vapor pressure of mercury at various temperatures. Fill in the rest of the table, and use the data to plot curves of \(P_{\text {vap }}\) versus \(T\) and \(\ln P_{\text {vap }}\) versus \(1 / T\). $$ \begin{array}{lccc} \hline \text { Temp }(\mathrm{K}) & P_{\text {vap }}(\mathrm{mm} \mathrm{Hg}) & \ln P_{\text {vap }} & 1 / T \\ \hline 500 & 39.3 & ? & ? \\ 520 & 68.5 & ? & ? \\ 540 & 114.4 & ? & ? \\ 560 & 191.6 & ? & ? \\ 580 & 286.4 & ? & ? \\ 600 & 432.3 & ? & ? \end{array} $$
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