One of the most fundamental concepts in physical chemistry is the Schrödinger equation, which lies at the heart of quantum mechanics. It provides a mathematical framework to describe the behavior of particles—such as electrons—at the atomic and subatomic level. Understanding this equation is key to explaining chemical bonding, molecular structure, and spectroscopy.
The time-independent Schrödinger equation for a single particle in one dimension is written as: H^ψ=Eψ\hat{H}\psi = E\psiH^ψ=Eψ
Where:
The Hamiltonian typically consists of two parts: H^=T^+V^\hat{H} = \hat{T} + \hat{V}H^=T^+V^
where T^\hat{T}T^ is the kinetic energy operator and V^\hat{V}V^ is the potential energy operator.
The wavefunction ψ(x)\psi(x)ψ(x) contains all the information about a quantum system. While ψ\psiψ itself is not directly observable, its square ∣ψ(x)∣2|\psi(x)|^2∣ψ(x)∣2 gives the probability density of finding a particle at a position xxx. This probabilistic interpretation marks a shift from classical mechanics to quantum mechanics.
One of the simplest and most illustrative problems is the particle-in-a-box (also known as the infinite potential well). In this model:
The allowed wavefunctions are: ψn(x)=2Lsin(nπxL)\psi_n(x) = \sqrt{\frac{2}{L}} \sin\left(\frac{n\pi x}{L}\right)ψn(x)=L2sin(Lnπx)
The corresponding energy levels are quantized: En=n2h28mL2E_n = \frac{n^2 h^2}{8mL^2}En=8mL2n2h2
where n=1,2,3,…n = 1, 2, 3, \ldotsn=1,2,3,… is the quantum number, hhh is Planck’s constant, mmm is the mass of the particle, and LLL is the box length.
This model illustrates that energy is not continuous, but quantized.
In physical chemistry, the Schrödinger equation is used to:
Although exact solutions exist only for simple systems, approximate methods (like Hartree-Fock) rely on the foundation laid by Schrödinger’s work.
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