Finding b in Van der Waals Equation?

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SUMMARY

The discussion centers on the application of the Van der Waals equation, specifically the term 'b', which represents the excluded volume per mole of gas. Participants clarify that 'b' is not a constant value but varies depending on the specific gas in question. The correct approach to finding the change in internal energy (ΔU) during an isobaric expansion is highlighted, revealing that 'b' cancels out in the calculations for temperature change, thus not affecting the final result. The equation ΔU = nC_v(T_2 - T_1) is confirmed as the correct formula for this scenario.

PREREQUISITES
  • Understanding the Van der Waals equation for real gases.
  • Knowledge of thermodynamic concepts, including internal energy and heat capacities (C_v and C_p).
  • Familiarity with algebraic manipulation of equations in thermodynamics.
  • Basic principles of isobaric processes in thermodynamics.
NEXT STEPS
  • Research the specific values of 'b' for different gases in the context of the Van der Waals equation.
  • Study the derivation and implications of the internal energy equation ΔU = nC_v(T_2 - T_1).
  • Explore the differences between ideal and non-ideal gases, focusing on their thermodynamic properties.
  • Learn about experimental methods to determine gas constants and excluded volumes in real gases.
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Students and professionals in thermodynamics, chemical engineering, and physical chemistry who are working with real gas behaviors and the Van der Waals equation.

DaynaClarke
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I've got a question that requires me to use the Van der Waals equation in the form:
p(V-b)=nRT
The process is isobaric, the volume changes from 1m3 to 2m3, and there is 1 mole of the unidentified gas.
Ultimately, I need to find initial and final values of T. So I rearranged the formula:
p(V-b)/nR=T

So I need b. I think b is the volume per mole, so that's how I worked it out - as V/n. However, this gave me b as 1m3/mol and 2m3/mol. That gives me initial and final temperatures of 0K, which I'm guessing is wrong.

In short, if someone could point me in the right direction as to what b actually is, I would very much appreciate it. Thank you.
 
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DaynaClarke said:
I've got a question that requires me to use the Van der Waals equation in the form:
p(V-b)=nRT
The process is isobaric, the volume changes from 1m3 to 2m3, and there is 1 mole of the unidentified gas.
Ultimately, I need to find initial and final values of T. So I rearranged the formula:
p(V-b)/nR=T

So I need b. I think b is the volume per mole, so that's how I worked it out - as V/n. However, this gave me b as 1m3/mol and 2m3/mol. That gives me initial and final temperatures of 0K, which I'm guessing is wrong.

In short, if someone could point me in the right direction as to what b actually is, I would very much appreciate it. Thank you.
What is the exact statement of the problem?
 
##b## should be the excluded volume for two particles of the gas (https://en.wikipedia.org/wiki/Van_der_Waals_equation) so it depends on the kind of gas you are working with. And it makes sense because because VdW introduced his formula to take in account for different kind of molecules (Pv=RT handles all gases the same way).
If you don't know anything about the gas I don't know how you can find a correct value for ##b##
 
Chestermiller said:
What is the exact statement of the problem?

"The equation of state of n moles of a gas is p(V-b)=nRT. The molar heat capacities of the gas at constant pressure and constant volume, cp and cv, satisfy cp - cv = R, where R is the gas constant, and γ = cp/cv = 5/3.

Find the change in internal energy of one mole of the gas in an isobaric expansion at a pressure of 1 bar from a volume of 1 m3 to 2 m3."


I have values for cp and cv, and I know that ΔU= Q - W = n⋅cp⋅dT - pdV. However, due to being unable to identify values for b at initial and final volumes, I don't know how to find initial and final temperatures.
 
DaynaClarke said:
"The equation of state of n moles of a gas is p(V-b)=nRT. The molar heat capacities of the gas at constant pressure and constant volume, cp and cv, satisfy cp - cv = R, where R is the gas constant, and γ = cp/cv = 5/3.

Find the change in internal energy of one mole of the gas in an isobaric expansion at a pressure of 1 bar from a volume of 1 m3 to 2 m3."


I have values for cp and cv, and I know that ΔU= Q - W = n⋅cp⋅dT - pdV.
This equation is incorrect. For this equation of state, $$\Delta U=nC_v(T_2-T_1)$$
Do you know how to show that this in the change in internal energy for this equation of state?
However, due to being unable to identify values for b at initial and final volumes, I don't know how to find initial and final temperatures.
Algebraically, in terms of p, ##V_1## and b, what is the initial temperature?
Algebraically, in terms of p, ##V_2##, and b, what is the final temperature?
From these algebraic expressions, what is ##(T_2-T_1)##? Does it involve b?
 
If you have experimental data, you could do a best fit to your data to find b.
 
Dr. Courtney said:
If you have experimental data, you could do a best fit to your data to find b.
That's not necessary. To solve this problem, the value of b is not needed.
 
Chestermiller said:
This equation is incorrect. For this equation of state, $$\Delta U=nC_v(T_2-T_1)$$
Do you know how to show that this in the change in internal energy for this equation of state?

Is it because the gas is ideal, and the internal energy of an ideal gas is purely kinetic, so it only considers the heat? I'll admit I'm not sure why it's Cv and not Cp because volume isn't constant, but pressure is.

Algebraically, in terms of p, ##V_1## and b, what is the initial temperature?
$$\frac{p(V_1-b)}{nR} = T_1$$
Algebraically, in terms of p, ##V_2##, and b, what is the final temperature?
$$\frac{p(V_2-b)}{nR} = T_2$$
From these algebraic expressions, what is ##(T_2-T_1)##? Does it involve b?
$$T_2-T_1 = \frac{p(V_1-V_2)}{nR}$$
So it doesn't contain b at all, it cancels out.
 
DaynaClarke said:
Is it because the gas is ideal, and the internal energy of an ideal gas is purely kinetic, so it only considers the heat? I'll admit I'm not sure why it's Cv and not Cp because volume isn't constant, but pressure is.
No. This gas is not ideal. Are you familiar with the following equation for a general non-ideal gas:
$$dU=nC_vdT-\left[p-T\left(\frac{\partial p}{\partial T}\right)_V\right]dV$$
If not, then your teacher did you a disservice by assigning you this problem. In any event, for the particular equation of state in the present problem, what do you get for the term in brackets?

Regarding Cv and Cp, you are aware of the following definitions, correct?:
$$nC_v=\left(\frac{\partial U}{\partial T}\right)_V$$and $$nC_p=\left(\frac{\partial H}{\partial T}\right)_p$$So, Cp is always associated with H and Cv is always associated with U. And, for this gas, if you did the math above correctly, you know that U is independent of V, and depends only on T.

$$\frac{p(V_1-b)}{nR} = T_1$$

$$\frac{p(V_2-b)}{nR} = T_2$$

$$T_2-T_1 = \frac{p(V_1-V_2)}{nR}$$
So it doesn't contain b at all, it cancels out.
These results are correct. So, what do you get if you substitute this result for the temperature change into the equation for ##\Delta U##?
 
  • #10
DaynaClarke said:
Is it because the gas is ideal, and the internal energy of an ideal gas is purely kinetic, so it only considers the heat? I'll admit I'm not sure why it's Cv and not Cp because volume isn't constant, but pressure is.$$\frac{p(V_1-b)}{nR} = T_1$$

$$\frac{p(V_2-b)}{nR} = T_2$$

$$T_2-T_1 = \frac{p(V_1-V_2)}{nR}$$
So it doesn't contain b at all, it cancels out.

Great job. One thing I often tell students is that if you are not given a value that appears in an equation, and you are not asked for it, and you don't have the information needed to find it, it probably cancels out.
 
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