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Heat capacity for \(\mathrm{Cl}_{2} .\) What is \(C_{V}\) at \(800 \mathrm{~K}\) for \(\mathrm{Cl}_{2}\) treated as an ideal diatomic gas in the high-temperature limit?

Short Answer

Expert verified
At 800 K, the heat capacity at constant volume for \[\mathrm{Cl}_2\] as an ideal diatomic gas is approximately 29.1 J/mol K.

Step by step solution

01

Understand the problem

Determine the heat capacity at constant volume (\(C_V\)) for chlorine gas (\reviews evaluating the limiting behavior of a high-temperature ideal diatomic gas.
02

Recall the formula for heat capacity of a diatomic gas

For a diatomic gas, in the high-temperature limit, the total degrees of freedom (including translational, rotational, and vibrational) contribute to the heat capacity. The formula is given by: \[ C_V = \frac{f}{2} R \]where \( f \) is the degrees of freedom, and \( R \) is the gas constant.
03

Identify the degrees of freedom for \(\mathrm{Cl}_2\)

A diatomic gas has 3 translational, 2 rotational, and 2 vibrational degrees of freedom. The total degrees of freedom at high temperature are: \[ f = 3 + 2 + 2 = 7 \]
04

Substitute the values into the formula

Plug in \( f = 7 \) and \( R = 8.314 \; \mathrm{J/mol \, K} \) into the formula: \[ C_V = \frac{7}{2} R = \frac{7}{2} \times 8.314 \approx 29.1 \; \mathrm{J/mol \, K} \]

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Ideal Gas Law
The ideal gas law is a fundamental principle used in thermodynamics to describe the behavior of ideal gases. It is represented by the equation:
\( PV = nRT \).

In this equation:
  • \( P \): Pressure of the gas
  • \( V \): Volume of the gas
  • \( n \): Amount of substance (in moles)
  • \( R \): Ideal gas constant \( (8.314 \, \text{J/mol K}) \)
  • \( T \): Absolute temperature in Kelvin

The ideal gas law helps us understand how gases expand and contract depending on temperature, pressure, and volume changes.
Degrees of Freedom
In thermodynamics, degrees of freedom refer to the number of independent ways in which a system can store energy. For a diatomic gas like chlorine gas (\( \text{Cl}_2 \)), we consider translational, rotational, and vibrational movements.

  • Translational: The gas molecules move in three-dimensional space (x, y, z directions). Thus, there are three translational degrees of freedom.
  • Rotational: For a diatomic molecule, rotation can occur around two axes perpendicular to the bond axis. Hence, there are two rotational degrees.
  • Vibrational: Diatomic molecules have one vibrational mode. Each mode counts as two degrees (one for kinetic and one for potential energy). Thus, there are two vibrational degrees of freedom.

This summation gives a total of seven degrees of freedom for diatomic gases at high temperatures (
\(3 + 2 + 2 = 7\)).
High-Temperature Limit
At high temperatures, the vibrational modes of diatomic molecules are fully excited along with the translational and rotational modes. This is why we consider all seven degrees of freedom (3 translational, 2 rotational, and 2 vibrational) for calculating heat capacity.

Normally, at room temperature, vibrational modes contribute very little because their energy levels are not accessible. However, as temperature increases, these modes get populated and contribute significantly to heat capacity calculations.
Heat Capacity Calculation
Heat capacity is a property that describes how much energy a substance can absorb per unit temperature increase. For a diatomic gas at constant volume (\(C_V\)), it can be calculated using degrees of freedom.

The formula is:
\[ C_V = \frac{f}{2} R \]
where:
  • \( f \): Degrees of freedom (which is 7 for diatomic gases at high temperatures)
  • \( R \): Ideal gas constant (\( 8.314 \, \text{J/mol·K} \))

So, for chlorine gas (\( \text{Cl}_2 \)) at 800 K:
\[ C_V = \frac{7}{2} \times 8.314 \, \text{J/mol·K} \ C_V \ \approx 29.1 \, \text{J/mol·K} \]
Diatomic Molecules
Diatomic molecules are molecules composed of only two atoms. Examples include chlorine gas (\( \text{Cl}_2 \)), oxygen gas (\( \text{O}_2 \)), and hydrogen gas (\( \text{H}_2 \)).

For diatomic gases, we consider:
  • Movements: The atoms can move translationally and rotate.
  • Bond Vibration: The bond between the two atoms can stretch and compress (vibrational modes).

Understanding these properties is essential for computing thermal properties such as the heat capacity in different thermodynamic conditions.

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Most popular questions from this chapter

Electron in benzene. Consider an electron that can move freely throughout the aromatic orbitals of benzene. Model the electron as a particle in a two- dimensional box \(4 \AA \times 4 \AA\). (a) Compute \(\Delta \varepsilon\), the energy change from the ground state to the excited state, \(n_{x}=n_{y}=2\). (b) Compute the wavelength \(\lambda\) of light that would be absorbed in this transition, if \(\Delta \varepsilon=h c / \lambda\), where \(h\) is Planck's constant and \(c\) is the speed of light. (c) Will this transition be in the visible part of the electromagnetic spectrum (i.e., is liquid benzene colored or transparent), according to this simple model?

Heat capacities of liquids. (a) \(C_{V}\) for liquid argon (at \(T=100 \mathrm{~K}\) ) is \(18.7 \mathrm{JK}^{-1} \mathrm{~mol}^{-1}\). How much of this heat capacity can you rationalize on the basis of your knowledge of gases? (b) \(C_{V}\) for liquid water at \(T=10^{\circ} \mathrm{C}\) is about \(75 \mathrm{JK}^{-1} \mathrm{~mol}^{-1}\). Assuming water has three vibrations, how much of this heat capacity can you rationalize on the basis of gases? What is responsible for the rest?

Conjugated polymers: why the absorption wavelength increases with chain length. Polyenes are linear double-bonded polymer molecules \((\mathrm{C}=\mathrm{C}-\mathrm{C})_{N}\), where \(N\) is the number of \(\mathrm{C}=\mathrm{C}-\mathrm{C}\) monomers. Model a polyene chain as a box in which \(\pi\)-electrons are particles that can move freely. If there are \(2 N\) carbon atoms each separated by bond length \(d=1.4 \AA\), and if the ends of the box are a distance \(d\) past the end \(\mathrm{C}\) atoms, then the length of the box is \(\ell=(2 N+1) d\). An energy level is occupied by two paired electrons. Suppose the \(N\) lowest levels are occupied by electrons, so the wavelength absorption of interest involves the excitation from level \(N\) to level \(N+1\). Compute the absorption energy \(\Delta \varepsilon=\varepsilon_{N+1}-\varepsilon_{N}=h c / \lambda\), where \(c\) is the speed of light and \(\lambda\) is the wavelength of absorbed radiation, using the particle-in-a-box model.

The translational partition function in two dimensions. When molecules adsorb on a two-dimensional surface, they have one less degree of freedom than in three dimensions. Write the two-dimensional translational partition function for an otherwise structureless particle.

Electron in a quantum-dot box. An electron moving through the lattice of a semiconductor has less inertia than when it is in a gas. Assume that the effective mass of the electron is only \(10 \%\) of its actual mass at rest. Calculate the translational partition function of the electron at room temperature \((273 \mathrm{~K})\) in a small semiconductor particle of a cubic shape with a side (a) \(1 \mathrm{~mm}\left(10^{-3} \mathrm{~m}\right)\), (b) \(100 \AA\left(100 \cdot 10^{-10} \mathrm{~m}\right)\); (c) To which particle would the term 'quantum dot,' i.e., a system with quantum mechanical behavior, be applied, and why?

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