An approximation of the ideal gas law for real gases

Click For Summary
SUMMARY

The discussion focuses on the virial expansion as a systematic method to account for deviations from the ideal gas law for real gases. The virial equation is expressed as PV=nRT(1+B(T)/(V/n) + C(T)/(V/n)^2+...), where B(T) and C(T) are the second and third virial coefficients, respectively. The van der Waals equation, (P+an^2/V^2)(V-nb)=nRT, is also highlighted as a notable equation of state for dense fluids. The coefficients are derived as B(T)=(b-a/RT) and C(T)=ab/RT, confirming their dependence on the constants a and b.

PREREQUISITES
  • Understanding of the ideal gas law and its limitations
  • Familiarity with the van der Waals equation
  • Knowledge of virial coefficients and their significance
  • Basic calculus and algebra for manipulating equations
NEXT STEPS
  • Study the derivation of the virial expansion in detail
  • Learn about the physical significance of virial coefficients in thermodynamics
  • Explore applications of the van der Waals equation in real gas behavior
  • Investigate other equations of state for gases, such as the Redlich-Kwong equation
USEFUL FOR

Students and professionals in chemistry and physics, particularly those studying thermodynamics and gas behavior, will benefit from this discussion. It is also valuable for researchers working on real gas modeling and related applications.

pentazoid
Messages
142
Reaction score
0

Homework Statement



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,

PV=nRT(1+B(T)/(V/n) + C(T)/(V/n)^2+...)

where functions B(T), C(T) and so on are called the virial coefficients.

Any proposed relation between P,V, and T , like the ideal gas law or the virial equationm is called an equation of state. Another famous equation of state , which is qualitative accurate even for dense fluids, is the van der waals equations

(P+an^2/V^2)(V-nb)=nRT

where a and b are constants that depend on the type of gas. Calculate the second and third virial coefficients(B and C) for a gas obeying the van der waals equation , and terms of a and b. (hint: The binomial expansion says that (1+x)^p=1+px+1/2p(p-1)x^2, provided that abs(px)<<1. Apply this approximation to the quantity [1-nb/V]^-1.)

Homework Equations





The Attempt at a Solution


(P+an^2/V^2)(V-nb)=nRT==> PV-Pnb-an^3b/V^2+an^2/V=nRT==> PV=nRT+Pnb+an^3/V^2-an^2/V ==> PV=nRT(1+Pnb/nRT-an/RTV+an^3b/nRTV^2) ==> PV=nRT(1+Pnb/PV-an/RTV+an^3b/nRTV^2)==> PV=nRT(1+nb/(V/n)-(a/RT)/(V/n)+(ab/RT)V^2/n^2). Therefore the coefficients of B and C are:

B(T)=(b-a/RT) and C(T)=ab/RT right?
 
Physics news on Phys.org
pentazoid said:

Homework Statement



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,

PV=nRT(1+B(T)/(V/n) + C(T)/(V/n)^2+...)

where functions B(T), C(T) and so on are called the virial coefficients.

Any proposed relation between P,V, and T , like the ideal gas law or the virial equationm is called an equation of state. Another famous equation of state , which is qualitative accurate even for dense fluids, is the van der waals equations

(P+an^2/V^2)(V-nb)=nRT

where a and b are constants that depend on the type of gas. Calculate the second and third virial coefficients(B and C) for a gas obeying the van der waals equation , and terms of a and b. (hint: The binomial expansion says that (1+x)^p=1+px+1/2p(p-1)x^2, provided that abs(px)<<1. Apply this approximation to the quantity [1-nb/V]^-1.)

Homework Equations


The Attempt at a Solution


(P+an^2/V^2)(V-nb)=nRT==> PV-Pnb-an^3b/V^2+an^2/V=nRT==> PV=nRT+Pnb+an^3/V^2-an^2/V ==> PV=nRT(1+Pnb/nRT-an/RTV+an^3b/nRTV^2) ==> PV=nRT(1+Pnb/PV-an/RTV+an^3b/nRTV^2)==> PV=nRT(1+nb/(V/n)-(a/RT)/(V/n)+(ab/RT)V^2/n^2). Therefore the coefficients of B and C are:

B(T)=(b-a/RT) and C(T)=ab/RT right?

Instead ofmultiplying out like you I wrote (as suggested)
(V-nb) = V(1-\frac{nb}{V} )\\
and took the bracket to the other side, then:
nRT(1-\frac{nb}{V} )^-^1 = nRT(1 + \frac{nb}{V} +\frac{n^2b^2}{V^2} + ...) = PV +\frac {an^2}{V} = PV + \frac{n}{V}. \frac {a}{RT}.nRT
Giving
<br /> B = b - \frac{a}{RT} , C = b^2<br />
 

Similar threads

Replies
1
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
Replies
3
Views
2K
Replies
30
Views
4K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 23 ·
Replies
23
Views
3K
Replies
3
Views
2K