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11.6: Schrödinger's Equation

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Quantum mechanics is the study of microscopic systems such as electrons or atoms. Calculus of variations and the idea of a Hamiltonian are fundamental ideas of quantum mechanics [136]. In Chapter 13, we apply the ideas of calculus of variations to an individual atom in a semiclassical way.

We can never say with certainty where an electron or other microscopic particle is located or its energy. However, we can discuss the probability of finding it with a specific energy. The probability of finding an electron, for example, in a particular energy state is specified by |ψ|2 where ψ is called the wave function [136]. As with any probability 0|ψ|21.

For example, suppose that as an electron moves, kinetic energy is converted to potential energy. The quantum mechanical Hamiltonian HQM is then the sum of the kinetic energy Ekinetic and potential energy Epotentialenergy.

HQM=Ekinetic+Epotentialenergy

Kinetic energy is expressed as

Ekinetic=12m(MQM)2

where m is the mass of an electron. In the expression above, MQM is the quantum mechanical momentum operator, and

(MQM)2=MQMMQM.

The quantum mechanical momentum operator is defined by

MQM=j

where the quantity is the Planck constant divided by 2π. The del operator, , was introduced in Sec. 1.6.1, and it represents the spatial derivative of a function. The quantities HQM, MQM, and are all operators, not just values. An operator, such as the derivative operator d dt, acts on a function. It itself is not a function or value.

Using the of momentum definition of Equation ??? and the vector identity of Equation 1.6.8, we can rewrite the Hamiltonian.

HQM=22m2+Epotentialenergy

In quantum mechanics, the Hamiltonian is related to the total energy.

HQMψ=Etotalψ

The above two equations can be combined algebraically.

(22m2+Epotentialenergy)ψ=Etotalψ

With some more algebra, Equation ??? can be rewritten.

2ψ+2m2(EtotalEpotentialenergy)ψ=0

Equation ??? is the time independent Schrödinger equation, and it is one of the most fundamental equations in quantum mechanics. Energy level diagrams were introduced in Section 6.2. Allowed energies illustrated by energy level diagrams satisfy the Schrödinger equation. At least for simple atoms and ground state energies, energy level diagrams can be derived by solving Schrödinger equation.


This page titled 11.6: Schrödinger's Equation is shared under a CC BY-NC 4.0 license and was authored, remixed, and/or curated by Andrea M. Mitofsky via source content that was edited to the style and standards of the LibreTexts platform.

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