LinearRotor(inertia=None, symmetry=1, quantum=False, rotationalConstant=None)¶
A statistical mechanical model of a two-dimensional (linear) rigid rotor. The attributes are:
|inertia||The moment of inertia of the rotor|
|rotationalConstant||The rotational constant of the rotor|
|symmetry||The symmetry number of the rotor|
Note that the moment of inertia and the rotational constant are simply two ways of representing the same quantity; only one of these can be specified independently.
In the majority of chemical applications, the energies involved in the rigid rotor place it very nearly in the classical limit at all relevant temperatures; therefore, the classical model is used by default.
A linear rigid rotor is modeled as a pair of point masses \(m_1\) and \(m_2\) separated by a distance \(R\). Since we are modeling the rotation of this system, we choose to work in spherical coordinates. Following the physics convention – where \(0 \le \theta \le \pi\) is the zenith angle and \(0 \le \phi \le 2\pi\) is the azimuth – the Schrodinger equation for the rotor is given by
where \(I \equiv \mu R^2\) is the moment of inertia of the rotating body, and \(\mu \equiv m_1 m_2 / (m_1 + m_2)\) is the reduced mass. Note that there is no potential term in the above expression; for this reason, a rigid rotor is often referred to as a free rotor. Solving the Schrodinger equation gives the energy levels \(E_J\) and corresponding degeneracies \(g_J\) for the linear rigid rotor as
where \(J\) is the quantum number for the rotor – sometimes called the total angular momentum quantum number – and \(B \equiv \hbar^2/2I\) is the rotational constant.
Using these expressions for the energy levels and corresponding degeneracies, we can evaluate the partition function for the linear rigid rotor:
In many cases the temperature of interest is large relative to the energy spacing; in this limit we can obtain a closed-form analytical expression for the linear rotor partition function in the classical limit:
Above we have also introduced \(\sigma\) as the symmetry number of the rigid rotor.
getDensityOfStates(self, ndarray Elist, ndarray densStates0=None) → ndarray¶
Return the density of states \(\rho(E) \ dE\) at the specified energies Elist in J/mol above the ground state. If an initial density of states densStates0 is given, the rotor density of states will be convoluted into these states.
getEnthalpy(self, double T) → double¶
Return the enthalpy in J/mol for the degree of freedom at the specified temperature T in K.
getEntropy(self, double T) → double¶
Return the entropy in J/mol*K for the degree of freedom at the specified temperature T in K.
getHeatCapacity(self, double T) → double¶
Return the heat capacity in J/mol*K for the degree of freedom at the specified temperature T in K.
getLevelDegeneracy(self, int J) → int¶
Return the degeneracy of level J.
getLevelEnergy(self, int J) → double¶
Return the energy of level J in kJ/mol.
getPartitionFunction(self, double T) → double¶
Return the value of the partition function \(Q(T)\) at the specified temperature T in K.
getSumOfStates(self, ndarray Elist, ndarray sumStates0=None) → ndarray¶
Return the sum of states \(N(E)\) at the specified energies Elist in J/mol above the ground state. If an initial sum of states sumStates0 is given, the rotor sum of states will be convoluted into these states.
The moment of inertia of the rotor.
The rotational constant of the rotor.