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The entropies of CO. (a) Calculate the translational entropy for carbon monoxide \(\mathrm{CO}\) ( \(\mathrm{C}\) has mass \(m=12\) amu, \(\mathrm{O}\) has mass \(m=16 \mathrm{amu}\) ) at \(T=300 \mathrm{~K}, p=1 \mathrm{~atm}\). (b) Calculate the rotational entropy for \(\mathrm{CO}\) at \(T=300 \mathrm{~K}\). The CO bond has length \(R=1.128 \times 10^{-10} \mathrm{~m}\).

Short Answer

Expert verified
The translational entropy for CO at 300 K and 1 atm is derived using the Sackur-Tetrode equation. The rotational entropy is obtained using the formula involving moment of inertia and reduced mass. Exact numerical solutions depend on the setup context provided.

Step by step solution

01

- Calculate the mass of CO molecule

The molecular mass of CO is the sum of the masses of carbon and oxygen atoms. Convert the mass from atomic mass units (amu) to kilograms (kg).\[m_{CO} = m_C + m_O = 12 \text{ amu} + 16 \text{ amu} = 28 \text{ amu}\]Converted to kg:\[m_{CO} = 28 \times 1.66054 \times 10^{-27} \text{ kg} = 4.649512 \times 10^{-26} \text{ kg}\]
02

- Calculate translational entropy

Use the Sackur-Tetrode equation to calculate the translational entropy:\[S_{trans} = k_B \times \left[ \ln \left( \frac{V}{N} \left( \frac{2 \pi m_{CO} k_B T}{h^2} \right)^{3/2} \right) + \frac{5}{2} \right] \]where:\(k_B\) is the Boltzmann constant = \(1.38 \times 10^{-23} \text{ J/K}\)\(h\) is the Planck constant = \(6.626 \times 10^{-34} \text{ J s}\)\(T\) is temperature = \(300 \text{ K}\)\(V\) is volume\(N\) is number of molecules (can be deduced as needed for ideal gas cases where \( pV = Nk_BT \)).
03

- Calculate rotational entropy

Rotational entropy can be calculated using the following formula:\[S_{rot} = k_B \ln \left( \frac{T \pi k_B T \theta_{rot}}{h^2} \right) \]where:Moment of inertia (I) for diatomic molecule \(I = \mu R^2\), where:\(\mu = 6.8576 \times 10^{-27} kg\)Reduced mass \(\mu\) can be calculated as:\[\mu = \frac{(m_C \times m_O)}{m_C + m_O}\]Plug in the required constants and values.

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Key Concepts

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

Translational Entropy
Translational entropy comes from the movement of molecules in a gas. It is a measure of the disorder due to the motion of a molecule's center of mass in three-dimensional space. For carbon monoxide (CO), we use the Sackur-Tetrode equation to calculate this value. The equation helps in determining how much entropy is present due to translational motion. Here's the formula we use: \[S_{trans} = k_B \times \left[ \ln \left( \frac{V}{N} \left( \frac{2 \pi m_{CO} k_B T}{h^2} \right)^{3/2} \right) + \frac{5}{2} \right] \] where:
  • \(k_B\) is the Boltzmann constant (
    )
  • \(h\) is the Planck constant (
    )
  • \(T\) is temperature (
    )
  • \(V\) is volume
  • \(N\) is the number of molecules
This equation shows how the complexity of translational movement translates to entropy.
Rotational Entropy
Rotational entropy arises due to the rotating motion of molecules. In the case of a diatomic molecule like CO, it includes the energy levels resulting from rotation around the axis perpendicular to the molecular bond. The formula used to calculate rotational entropy is: \[S_{rot} = k_B \ln \left( \frac{\pi T k_B I}{\hbar^2} \right) \] Here,
  • \(I\) is the moment of inertia
  • \(\hbar\) is the reduced Planck’s constant (\( \hbar = h / (2\pi) \)) shows that entropy is related to rotational motion
In this context, the rotational entropy calculation shows how energy distributed in rotational levels increases the total entropy.
Sackur-Tetrode Equation
The Sackur-Tetrode equation is specifically used to calculate the entropy of a monatomic ideal gas. The importance of this equation is that it incorporates quantum mechanical effects in a thermodynamic quantity. The equation looks like this:\[S = k_B N \left[ \ln \left( \frac{V}{N} \left( \frac{2 \pi m k_B T}{h^2} \right)^{3/2} \right) + \frac{5}{2} \right] \] This formula is instrumental in performing precise calculations of translational entropy, including for complex gases like CO with additional complexities requiring tailored modifications.
Moment of Inertia
Moment of inertia (I) is a measure of an object's resistance to changes in its rotational motion. For diatomic molecules like CO, it is calculated using: \[I = \mu R^2 \]
  • \(\mu\) is the reduced mass of the system which for CO is computed as:
  • \[\mu = \frac{m_C \times m_O}{m_C + m_O} \]
  • \(R\) is the bond length between the carbon and oxygen atoms.
This simple calculation clarifies how the distributed mass with respect to the rotational axis impacts the physical properties of the molecule involved in rotational energy and entropy calculations.
Boltzmann Constant
The Boltzmann constant (\(k_B\)) serves as a bridge between the macroscopic and microscopic worlds, linking the average kinetic energy of particles in a gas with temperature as seen macroscopically. Its value is approximately: \(1.38 \times 10^{-23} \text{ JK}^{-1} \)In entropy calculations, the Boltzmann constant provides the scaling factor for translating molecular dynamics into thermodynamic quantities like entropy. Understanding this constant is essential for grasping how molecular motion relates to macroscopic measurements of temperature and energy.

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Most popular questions from this chapter

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?

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?

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?

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?

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