You have 3 free guides left 😟
Unlock your guides
You have 3 free guides left 😟
Unlock your guides

The is a key concept in molecular structure. It separates the motion of electrons and nuclei in molecules, simplifying calculations. This approximation allows us to understand molecular geometry, vibrations, and reactions.

By treating electrons and nuclei separately, we can construct potential energy surfaces. These surfaces show how molecular energy changes with nuclear positions, giving insights into stability and reactivity. The approximation has limitations but remains fundamental in quantum chemistry.

Separating Electronic and Nuclear Motions

The Born-Oppenheimer Approximation

Top images from around the web for The Born-Oppenheimer Approximation
Top images from around the web for The Born-Oppenheimer Approximation
  • The Born-Oppenheimer approximation separates the motion of atomic nuclei and electrons in a molecule due to the significant difference in their masses
  • Electrons move much faster than nuclei, allowing the electronic motion to rapidly adjust to any change in nuclear positions ()
  • The total molecular wave function is approximated as a product of electronic and nuclear wave functions
    • The depends parametrically on the nuclear coordinates
    • The nuclear wave function describes the motion of the nuclei on the created by the electrons
  • The separation of electronic and nuclear motions simplifies the for molecules, making it more tractable to solve
    • The electronic Schrödinger equation is solved first, keeping the nuclear coordinates fixed (clamped-nuclei approximation)
    • The resulting electronic energy is then used as a potential energy term in the nuclear Schrödinger equation

Consequences of the Born-Oppenheimer Approximation

  • The Born-Oppenheimer approximation is a fundamental concept in quantum chemistry and is widely used in the study of molecular structure and dynamics
  • It allows for the construction of potential energy surfaces, which represent the electronic energy as a function of nuclear coordinates
    • Potential energy surfaces provide valuable information about the equilibrium geometry, vibrational frequencies, and reaction pathways of molecules
  • The approximation enables the separation of electronic and vibrational spectra in molecules
    • Electronic transitions occur on a much faster timescale than vibrational transitions (Franck-Condon principle)
  • The Born-Oppenheimer approximation forms the basis for the adiabatic and diabatic representations of molecular states
    • Adiabatic states are eigenstates of the electronic Hamiltonian at fixed nuclear coordinates
    • Diabatic states are constructed to minimize the between electronic states during

Born-Oppenheimer Approximation for Molecular Wave Functions

Separating the Molecular Wave Function

  • The molecular wave function is separated into an electronic wave function and a nuclear wave function under the Born-Oppenheimer approximation
    • Ψtotal(r,R)Ψelec(r;R)Ψnuc(R)\Psi_{total}(\vec{r},\vec{R}) \approx \Psi_{elec}(\vec{r};\vec{R}) \Psi_{nuc}(\vec{R})
    • r\vec{r} represents the electronic coordinates, and R\vec{R} represents the nuclear coordinates
  • The electronic wave function is obtained by solving the electronic Schrödinger equation, which depends on the nuclear coordinates as parameters
    • H^elecΨelec(r;R)=Eelec(R)Ψelec(r;R)\hat{H}_{elec} \Psi_{elec}(\vec{r};\vec{R}) = E_{elec}(\vec{R}) \Psi_{elec}(\vec{r};\vec{R})
    • H^elec\hat{H}_{elec} is the electronic Hamiltonian, and Eelec(R)E_{elec}(\vec{R}) is the electronic energy
  • The nuclear wave function is obtained by solving the nuclear Schrödinger equation, which includes the electronic energy as a potential energy term
    • [T^nuc+Eelec(R)]Ψnuc(R)=EtotalΨnuc(R)[\hat{T}_{nuc} + E_{elec}(\vec{R})] \Psi_{nuc}(\vec{R}) = E_{total} \Psi_{nuc}(\vec{R})
    • T^nuc\hat{T}_{nuc} is the nuclear kinetic energy operator, and EtotalE_{total} is the total energy of the molecule

Constructing Potential Energy Surfaces

  • The Born-Oppenheimer approximation allows for the construction of potential energy surfaces, which represent the electronic energy as a function of nuclear coordinates
  • Potential energy surfaces are obtained by solving the electronic Schrödinger equation at various nuclear configurations and plotting the resulting electronic energies
  • The shape of the potential energy surface determines many properties of the molecule, such as:
    • Equilibrium geometry: the nuclear configuration that minimizes the electronic energy
    • Vibrational frequencies: the curvature of the potential energy surface near the equilibrium geometry
    • Reaction pathways: the minimum energy path connecting reactants and products on the potential energy surface
  • Potential energy surfaces provide a visual representation of the energy landscape of a molecule and are essential for understanding its structure, stability, and reactivity

Validity and Limitations of the Born-Oppenheimer Approximation

Conditions for the Validity of the Born-Oppenheimer Approximation

  • The Born-Oppenheimer approximation is valid when the energy separation between electronic states is much larger than the energy of nuclear motion
    • This condition ensures that the electronic motion can quickly adapt to changes in nuclear positions without significant mixing between electronic states
  • The approximation is most accurate for ground-state molecules near their equilibrium geometry, where the potential energy surface is well-separated from other electronic states
  • The Born-Oppenheimer approximation is less reliable for excited states, where the energy separation between electronic states is smaller and the potential for is greater

Limitations and Breakdown of the Born-Oppenheimer Approximation

  • The Born-Oppenheimer approximation breaks down when there is a strong coupling between electronic and nuclear motions, such as:
    • Conical intersections: points on the potential energy surface where two or more electronic states become degenerate and strongly interact
    • Jahn-Teller distortions: symmetry-breaking distortions of the nuclear framework that lift the degeneracy of electronic states
  • Non-adiabatic effects, where the electronic state changes during nuclear motion, cannot be described within the Born-Oppenheimer framework
    • These effects are important in processes such as photochemistry, energy transfer, and electron transfer
  • The Born-Oppenheimer approximation neglects the coupling between different electronic states, which can be important in some cases
    • Examples include spin-orbit coupling, which mixes electronic states with different spin multiplicities, and , which mixes electronic and vibrational states
  • Despite its limitations, the Born-Oppenheimer approximation remains a powerful tool in quantum chemistry and provides a good starting point for more advanced treatments of molecular systems
    • Post-Born-Oppenheimer methods, such as the adiabatic and diabatic representations, can be used to incorporate non-adiabatic effects and electronic state couplings
    • Multireference methods, such as CASSCF and MRCI, can describe systems with strong electronic correlations and near-degeneracies that are challenging for the Born-Oppenheimer approximation
© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.


© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.

© 2024 Fiveable Inc. All rights reserved.
AP® and SAT® are trademarks registered by the College Board, which is not affiliated with, and does not endorse this website.
Glossary
Glossary