Problem 11
Question
For a van der Waals gas, plot the isotherms in the \(\bar{P}-\bar{V}\) plane \((\bar{P}\) and \(\bar{V}\) are the reduced pressure and volume) for reduced temperatures \(\bar{T}=0.5, \bar{T}=1.0\), and \(\bar{T}=1.5\). For \(\bar{T}=0.5\), is \(\bar{P}=0.1\) the equilibrium pressure of the liquid-gas coexistence region?
Step-by-Step Solution
Verified Answer
Plot isotherms for \bar{T}=0.5, 1.0, 1.5; equilibrium pressure is determined from the critical point data.
1Step 1 - Understand the van der Waals equation in reduced terms
The van der Waals equation in reduced form describes the behavior of a real gas. The equation is given by: The reduced form equation is then expressed as where: where
2Step 2 - Plot the isotherms for given reduced temperatures
For reduced temperatures plot the reduced pressure in plane. Use the van der Waals equation in reduced form. get the curves.
Key Concepts
isothermsreduced pressurereduced temperaturevan der Waals equation
isotherms
Isotherms are curves on a graph that represent the relationship between pressure and volume at constant temperature. For a van der Waals gas, this relationship is more complex compared to an ideal gas because it considers molecular size and interactions.
In the \(\bar{P} - \bar{V}\) plane, we plot the reduced pressure \(\bar{P}\) against the reduced volume \(\bar{V}\) for different reduced temperatures \(\bar{T}\).
Each curve on the plot corresponds to a specific temperature.
In the \(\bar{P} - \bar{V}\) plane, we plot the reduced pressure \(\bar{P}\) against the reduced volume \(\bar{V}\) for different reduced temperatures \(\bar{T}\).
Each curve on the plot corresponds to a specific temperature.
- For higher temperatures, the isotherms resemble the hyperbolic shape typical of an ideal gas.
- For lower temperatures, the isotherms show regions where liquid and gas coexist, known as the phase transition region.
reduced pressure
Reduced pressure \(\bar{P}\) is a dimensionless form of pressure, scaled by a characteristic pressure of the substance. It is given by:
\[\bar{P} = \frac{P}{P_c} \]
where:
Plotting \(\bar{P}\) versus reduced volume simplifies the analysis of phase transitions and other properties, revealing insights that would be obscured by using raw pressure values alone.
\[\bar{P} = \frac{P}{P_c} \]
where:
- \(P\) is the actual pressure of the gas.
- \(P_c\) is the critical pressure of the gas.
Plotting \(\bar{P}\) versus reduced volume simplifies the analysis of phase transitions and other properties, revealing insights that would be obscured by using raw pressure values alone.
reduced temperature
Reduced temperature \(\bar{T}\) is another dimensionless quantity, which scales the actual temperature with the critical temperature of the gas. It is given by:
\[\bar{T} = \frac{T}{T_c} \]
where:
For \(\bar{T} < 1.0\), the gas can exhibit phase transitions from gas to liquid.
For \(\bar{T} > 1.0\), the gas behaves more like an ideal gas, with less deviation seen in the van der Waals isotherms.
Understanding reduced temperature is crucial in predicting the behavior of gases under different thermal conditions.
\[\bar{T} = \frac{T}{T_c} \]
where:
- \(T\) is the actual temperature of the gas.
- \(T_c\) is the critical temperature of the gas.
For \(\bar{T} < 1.0\), the gas can exhibit phase transitions from gas to liquid.
For \(\bar{T} > 1.0\), the gas behaves more like an ideal gas, with less deviation seen in the van der Waals isotherms.
Understanding reduced temperature is crucial in predicting the behavior of gases under different thermal conditions.
van der Waals equation
The van der Waals equation accounts for real gas behavior by modifying the ideal gas law. It incorporates two factors:
\[ ( \bar{P} + \frac{3} { \bar{V}^2 } ) ( 3\bar{V} - 1 ) = 8\bar{T} \]
Here, each variable is scaled by its critical value:
- Molecular volume: It adjusts the volume available to gas molecules.
- Intermolecular forces: It accounts for the attraction between gas molecules.
\[ ( \bar{P} + \frac{3} { \bar{V}^2 } ) ( 3\bar{V} - 1 ) = 8\bar{T} \]
Here, each variable is scaled by its critical value:
- \(\bar{P} = \frac{P}{P_c}\)
- \(\bar{T} = \frac{T}{T_c}\)
- \(\bar{V} = \frac{V}{V_c}\)
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