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Schodinger Equation

  • Tufail Hussain
  • Oct 25, 2024
  • 2 min read



The Schrödinger equation is a fundamental equation in quantum mechanics that describes how the quantum state of a physical system evolves over time. It's named after the Austrian physicist Erwin Schrödinger, who formulated it in 1925. The equation plays a role similar to Newton's laws in classical mechanics but operates within the framework of quantum mechanics, governing the behavior of particles at atomic and subatomic scales.

There are two main forms of the Schrödinger equation:

  1. Time-Dependent Schrödinger Equation (TDSE): This equation describes how the quantum state (represented by the wave function, ψ(x,t)\psi(x,t)ψ(x,t)) of a system evolves over time. It is especially useful for systems where the potential energy depends on time or where the system evolves dynamically.

    iℏ∂∂tψ(r,t)=H^ψ(r,t)i \hbar \frac{\partial}{\partial t} \psi(\mathbf{r}, t) = \hat{H} \psi(\mathbf{r}, t)iℏ∂t∂​ψ(r,t)=H^ψ(r,t)

    Where:

    • iii is the imaginary unit,

    • ℏ\hbarℏ is the reduced Planck constant,

    • ψ(r,t)\psi(\mathbf{r}, t)ψ(r,t) is the wave function,

    • H^\hat{H}H^ is the Hamiltonian operator, which represents the total energy of the system (sum of kinetic and potential energies),

    • r\mathbf{r}r is the position vector, and

    • ttt is time.

  2. Time-Independent Schrödinger Equation (TISE): This is used for systems where the potential energy does not depend on time, such as particles in a stationary state. It's derived from the time-dependent equation under the assumption of a time-independent potential, and it describes the spatial distribution of the wave function.

    H^ψ(r)=Eψ(r)\hat{H} \psi(\mathbf{r}) = E \psi(\mathbf{r})H^ψ(r)=Eψ(r)

    Where:

    • EEE is the energy eigenvalue of the system,

    • The Hamiltonian H^\hat{H}H^ typically includes kinetic energy (involving derivatives with respect to position) and potential energy terms.

Significance of the Schrödinger Equation

  • The wave function ψ(r,t)\psi(\mathbf{r}, t)ψ(r,t) contains all the information about a quantum system, including the probabilities of finding particles in specific states.

  • The equation allows for the calculation of observable quantities such as energy, momentum, and position.

  • It's a core component of quantum mechanics, governing systems ranging from electrons in atoms to quantum fields in advanced theories.

 
 
 

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