The Schrödinger equation describes how the wavefunction evolves over time. In its time-dependent form, it can be written as:
iħ ∂Ψ/∂t = HΨ
Where i is the imaginary unit, ħ is the reduced Planck's constant, ∂Ψ/∂t is the partial derivative of the wavefunction with respect to time, and H is the Hamiltonian operator. The Hamiltonian represents the total energy of the system, including both kinetic and potential energies.
