Chapter 5: Q. 5.49 (page 185)
Use the result of the previous problem and the approximate values of a and b to find the value of Tc, Pc, Vc/N for N2, H2O and He.
Short Answer
() | role="math" localid="1647074922910" | ||
(Pa) | |||
(K) | 143 | 572 | 21.5 |
Chapter 5: Q. 5.49 (page 185)
Use the result of the previous problem and the approximate values of a and b to find the value of Tc, Pc, Vc/N for N2, H2O and He.
() | role="math" localid="1647074922910" | ||
(Pa) | |||
(K) | 143 | 572 | 21.5 |
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Get started for freeWhen solid quartz "dissolves" in water, it combines with water molecules in the reaction
(a) Use this data in the back of this book to compute the amount of silica dissolved in water in equilibrium with solid quartz, at 25° C
(b) Use the van't Hoff equation (Problem 5.85) to compute the amount of silica dissolved in water in equilibrium with solid quartz at 100°C.
Problem 5.58. In this problem you will model the mixing energy of a mixture in a relatively simple way, in order to relate the existence of a solubility gap to molecular behaviour. Consider a mixture of A and B molecules that is ideal in every way but one: The potential energy due to the interaction of neighbouring molecules depends upon whether the molecules are like or unlike. Let n be the average number of nearest neighbours of any given molecule (perhaps 6 or 8 or 10). Let n be the average potential energy associated with the interaction between neighbouring molecules that are the same (4-A or B-B), and let uAB be the potential energy associated with the interaction of a neighbouring unlike pair (4-B). There are no interactions beyond the range of the nearest neighbours; the values of are independent of the amounts of A and B; and the entropy of mixing is the same as for an ideal solution.
(a) Show that when the system is unmixed, the total potential energy due to neighbor-neighbor interactions is . (Hint: Be sure to count each neighbouring pair only once.)
(b) Find a formula for the total potential energy when the system is mixed, in terms of x, the fraction of B.
(c) Subtract the results of parts (a) and (b) to obtain the change in energy upon mixing. Simplify the result as much as possible; you should obtain an expression proportional to x(1-x). Sketch this function vs. x, for both possible signs of .
(d) Show that the slope of the mixing energy function is finite at both end- points, unlike the slope of the mixing entropy function.
(e) For the case , plot a graph of the Gibbs free energy of this system
vs. x at several temperatures. Discuss the implications.
(f) Find an expression for the maximum temperature at which this system has
a solubility gap.
(g) Make a very rough estimate of for a liquid mixture that has a
solubility gap below 100°C.
(h) Use a computer to plot the phase diagram (T vs. x) for this system.
The standard enthalpy change upon dissolving one mole of oxygen at 25°C is -11.7 kJ. Use this number and the van't Hoff equation (Problem 5.85) to calculate the equilibrium (Henry's law) constant for oxygen in water at 0°C and at 100° C. Discuss the results briefly.
Imagine that you drop a brick on the ground and it lands with a thud. Apparently the energy of this system tends to spontaneously decrease. Explain why.
Assume that the air you exhale is at 35°C, with a relative humidity of 90%. This air immediately mixes with environmental air at 5°C and unknown relative humidity; during the mixing, a variety of intermediate temperatures and water vapour percentages temporarily occur. If you are able to "see your breath" due to the formation of cloud droplets during this mixing, what can you conclude about the relative humidity of your environment? (Refer to the vapour pressure graph drawn in Problem 5.42.)
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