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.)

Short Answer

Expert verified

The relative humidity required to produce cloud droplets is around 25%.

Step by step solution

01

Given information

Consider the initial water vapour pressure of air mixed at temperatures of 10°C and 35°C. When the air particles have the same mass, the air mixture should have a half-temperature of between 10 and 35 degrees Celsius.

The reason for this is that air's heat capacity is independent of its temperature. In the same way, the water partial pressure is half way between the air particle starting pressures. The air mixture temperature and water partial pressure lie on the straight line in the figure for any value of the initial mass ratio.

02

Explanation

Use the vapour pressure graph from problem 5.42 to graph the compositions of exhaled air at 35° and 90% relative humidity, as well as the composition of outside air, as illustrated in the diagram below.

P is the partial pressure of water in bar, and T is the temperature in degrees Celsius. In the diagram above, the lower dot represents the external air temperature (10°C) and the top dot represents the exhaled air temperature (35°C).

03

Conclusion

Cloud droplets are formed when the state of the mixture is above the equilibrium curve, as indicated in the diagram. Because both initial states are below the curve, this is conceivable.

When the outdoor air dot goes vertically downward, the vapour pressure curve may be crossed. The minimal partial pressure in this situation is 0.003 bar, while the relative humidity is around 25%, according to the graph.

As a result, the relative humidity required to produce cloud droplets is around 25%.

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Most popular questions from this chapter

The partial-derivative relations derived in Problems 1.46,3.33, and 5.12, plus a bit more partial-derivative trickery, can be used to derive a completely general relation between CPandCV.

(a) With the heat capacity expressions from Problem 3.33 in mind, first considerSto be a function of TandV.Expand dSin terms of the partial derivatives (S/T)Vand (S/V)T. Note that one of these derivatives is related toCV

(b) To bring in CP, considerlocalid="1648430264419" Vto be a function ofTand P and expand dV in terms of partial derivatives in a similar way. Plug this expression for dV into the result of part (a), then set dP=0and note that you have derived a nontrivial expression for (S/T)P. This derivative is related to CP, so you now have a formula for the difference CP-CV

(c) Write the remaining partial derivatives in terms of measurable quantities using a Maxwell relation and the result of Problem 1.46. Your final result should be

CP=CV+TVβ2κT

(d) Check that this formula gives the correct value of CP-CVfor an ideal gas.

(e) Use this formula to argue that CPcannot be less than CV.

(f) Use the data in Problem 1.46 to evaluateCP-CVfor water and for mercury at room temperature. By what percentage do the two heat capacities differ?

(g) Figure 1.14 shows measured values of CPfor three elemental solids, compared to predicted values of CV. It turns out that a graph of βvs.T for a solid has same general appearance as a graph of heat capacity. Use this fact to explain why CPand CVagree at low temperatures but diverge in the way they do at higher temperatures.

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.

When carbon dioxide "dissolves" in water, essentially all of it reacts to form carbonic acid, H2CO3:

CO2(g)+H2O(l)H2CO3(aq)

The carbonic acid can then dissociate into H* and bicarbonate ions,

H2CO3(aq)H+(aq)+HCO3-(aq)

(The table at the back of this book gives thermodynamic data for both of these reactions.) Consider a body of otherwise pure water (or perhaps a raindrop) that is in equilibrium with the atmosphere near sea level, where the partial pressure of carbon dioxide is 3.4 x 10-4 bar (or 340 parts per million). Calculate the molality of carbonic acid and of bicarbonate ions in the water, and determine the pH of the solution. Note that even "natural" precipitation is somewhat acidic.

The enthalpy and Gibbs free energy, as defined in this section, give special treatment to mechanical (compression-expansion) work, -PdV. Analogous quantities can be defined for other kinds of work, for instance, magnetic work." Consider the situation shown in Figure 5.7, where a long solenoid ( Nturns, total length N) surrounds a magnetic specimen (perhaps a paramagnetic solid). If the magnetic field inside the specimen is Band its total magnetic moment is M, then we define an auxilliary field H(often called simply the magnetic field) by the relation

H1μ0B-MV,

where μ0is the "permeability of free space," 4π×10-7N/A2. Assuming cylindrical symmetry, all vectors must point either left or right, so we can drop the -symbols and agree that rightward is positive, leftward negative. From Ampere's law, one can also show that when the current in the wire is I, the Hfield inside the solenoid is NI/L, whether or not the specimen is present.

(a) Imagine making an infinitesimal change in the current in the wire, resulting in infinitesimal changes in B, M, and H. Use Faraday's law to show that the work required (from the power supply) to accomplish this change is Wtotal=VHdB. (Neglect the resistance of the wire.)

(b) Rewrite the result of part (a) in terms of Hand M, then subtract off the work that would be required even if the specimen were not present. If we define W, the work done on the system, to be what's left, show that W=μ0HdM.

(c) What is the thermodynamic identity for this system? (Include magnetic work but not mechanical work or particle flow.)

(d) How would you define analogues of the enthalpy and Gibbs free energy for a magnetic system? (The Helmholtz free energy is defined in the same way as for a mechanical system.) Derive the thermodynamic identities for each of these quantities, and discuss their interpretations.

Go through the arithmetic to verify that diamond becomes more stable than graphite at approximately 15 kbar.

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