Suppose you open a bottle of perfume at one end of a room. Very roughly, how much time would pass before a person at the other end of the room could smell the perfume, if diffusion were the only transport mechanism? Do you think diffusion is the dominant transport mechanism in this situation?

Short Answer

Expert verified

The amount of time it would take for someone on the other end of the room to smell the perfume is

Δt=107s116daysD=105m2s1

Step by step solution

01

Step1:In this case, diffusion is the dominant transport mechanism.

Assume a perfume bottle is opened at one end of a long 10mroom. Schroeder provides D=2×10-5m2·s-1for COAt room temperature and atmospheric pressure, molecules in air Because a perfume molecule is likely larger than a CO molecule, its diffusion constant would be lower, say,localid="1650259068074" D=10-5m2·s-1.We can calculate how far a perfume molecule will diffuse by takingΔx=10mto be the distance that diffusion has occurred over This region's volume is :

V=AΔx

where A denotes the room's cross sectional area If N is the total number of molecules in this region, the particle density is as follows:

n=NV=NAΔx

The flux can be calculated by dividing the time it takestfor the volume to acquire the N molecules by the volume At, yielding:

Jx=NAΔt

02

Step2:Ficks law

Jx=Ddndx

substitute from equationsJx=NAΔtand n=NV=NAΔxinto equationJx=NAΔt, so:

NAΔt=DddxNAΔx=DNA(Δx)2

Δt=(Δx)2D

substitute with,Δx=10mandD=10-5m2·s-1, so:

which is approximately116days Certainly, most odors released at some point in a room (including those embarrassing to the emitter at times) travel much faster than that (often in less than a minute), implying that other processes (typically convection) are responsible for spreading them.

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Problem 1.36. In the course of pumping up a bicycle tire, a liter of air at atmospheric pressure is compressed adiabatically to a pressure of 7 atm. (Air is mostly diatomic nitrogen and oxygen.)

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Even at low density, real gases don’t quite obey the ideal gas law. A systematic way to account for deviations from ideal behavior is the virial

expansion,

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where the functions B(T), C(T), and so on are called the virial coefficients. When the density of the gas is fairly low, so that the volume per mole is large, each term in the series is much smaller than the one before. In many situations, it’s sufficient to omit the third term and concentrate on the second, whose coefficient B(T)is called the second virial coefficient (the first coefficient is 1). Here are some measured values of the second virial coefficient for nitrogen (N2):

T(K)
B(cm3/mol)
100–160
200–35
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4009.0
50016.9
60021.3
  1. For each temperature in the table, compute the second term in the virial equation, B(T)/(V/n), for nitrogen at atmospheric pressure. Discuss the validity of the ideal gas law under these conditions.
  2. Think about the forces between molecules, and explain why we might expect B(T)to be negative at low temperatures but positive at high temperatures.
  3. Any proposed relation between P, V, andT, like the ideal gas law or the virial equation, is called an equation of state. Another famous equation of state, which is qualitatively accurate even for dense fluids, is the van der Waals equation,
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  4. Plot a graph of the van der Waals prediction for B(T), choosing aand bso as to approximately match the data given above for nitrogen. Discuss the accuracy of the van der Waals equation over this range of conditions. (The van der Waals equation is discussed much further in Section 5.3.)
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