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The compression factor of a fluid is defined as the ratio PV/NkT; the deviation of this quantity from 1 is a measure of how much the fluid differs from an ideal gas. Calculate the compression factor of a Van der Waals fluid at the critical point, and note that the value is independent of a and b. (Experimental values of compression factors at the critical point are generally lower than the Van der Waals prediction, for instance, 0.227 for H22O, 0.274 for CO22, and 0.305 for He.)

Short Answer

Expert verified

The compression factor of van der Waal fluid at critical point is 38.

Step by step solution

01

Given 

The compression factor of a fluid is given by

Z=PVNkT

where Z is compression factor.

02

van  der Waal's equation

P=NkT(V-Nb)-aN2V2

Partial differentiation of the equation w.r.t V

we get

role="math" localid="1646976952526" δPδV=-NkT(V-Nb)2+2aN2V3

Again differentiating we get

role="math" localid="1646977057779" δ2Pδ2V=NkT(V-Nb)3-6aN2V4

03

At critical point

δPδV=0δ2Pδ2V=0

role="math" localid="1646977123022" ⇒NkTc(Vc-Nb)2=2aN2Vc3andNkTc(Vc-Nb)3=6aN2Vc4

04

Finding Vc, Tc, Pc.

On equating the above equations we get

Vc=3Nb

Substituting the equation in equation

role="math" localid="1646977903462" NkTc(3Nb-Nb)2=2aN2(3Nb)3⇒kTc=327ab

Substituting the above values in equation (2)

Pc=Nk(3a27b)(3Nb-Nb)-aN2(3Nb)2⇒Pc=127ab2

05

Substituting the values in Equation (1)

ZC=PcVcNkTc=127ab2×3Nb×1N×273×ba=38

The value of the compression factor is less than 1

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Most popular questions from this chapter

What happens when you add salt to the ice bath in an ice cream maker? How is it possible for the temperature to spontaneously drop below 0"C? Explain in as much detail as you can.

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.

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.

Check that equations 5.69 and 5.70 satisfy the identityG=NAμA+NBμB (equation 5.37)

By subtracting μNfrom localid="1648229964064" U,H,F,orG,one can obtain four new thermodynamic potentials. Of the four, the most useful is the grand free energy (or grand potential),

Φ≡U-TS-μN.

(a) Derive the thermodynamic identity for Φ, and the related formulas for the partial derivatives ofΦwith respect toT,V, and μN

(b) Prove that, for a system in thermal and diffusive equilibrium (with a reservoir that can supply both energy and particles), Φtends to decrease.

(c) Prove thatϕ=-PV.

(d) As a simple application, let the system be a single proton, which can be "occupied" either by a single electron (making a hydrogen atom, with energy -13.6eV) or by none (with energy zero). Neglect the excited states of the atom and the two spin states of the electron, so that both the occupied and unoccupied states of the proton have zero entropy. Suppose that this proton is in the atmosphere of the sun, a reservoir with a temperature of 5800Kand an electron concentration of about 2×1019per cubic meter. Calculate Φfor both the occupied and unoccupied states, to determine which is more stable under these conditions. To compute the chemical potential of the electrons, treat them as an ideal gas. At about what temperature would the occupied and unoccupied states be equally stable, for this value of the electron concentration? (As in Problem 5.20, the prediction for such a small system is only a probabilistic one.)

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