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Quantum Mechanics in Physics

Once a particle has a wavelength, something has to say how that wavelength behaves, and the Schrodinger equation is that something. It is a wave equation, but its solutions are not numbers you measure. They are wave functions, and squaring one gives the odds of finding the particle in a given place. What makes the equation so productive is that it must be obeyed everywhere at once, including at the walls of whatever container the particle sits in, and only certain energies let the wave fit those edges smoothly. Those energies are the quantum levels, and they were not put in by hand. The blocks give the equation in both forms, the well worked through to its allowed energies, tunneling through a barrier, and the harmonic oscillator, which is the one case that comes up again and again in later physics.

The Wave Function
Probability of finding a particle in a range

Given

  • (m)
Normalization condition for a wave function

Given

Expectation value of the position of a particle

Given

  • (m)
Time-dependent Schrodinger equation

Given

  • (kg)
  • (J)

Constant used

Time-independent Schrodinger equation

Given

  • (kg)
  • (J)
  • (J)

Constant used

Allowed energies of a particle in an infinite square well

Given

  • (J s)
  • (kg)
  • (m)

Constants used

Wave function of a particle in an infinite square well

Given

  • (m)
  • (m)
Probability of tunneling through a potential barrier

Given

  • (1/m)
  • (m)
  • (J)
  • (J)

Constant used

Transmission coefficient of a rectangular barrier

Given

  • (1/m)
  • (m)
Allowed energies of a quantum harmonic oscillator

Given

  • (J s)
  • (rad/s)

Constant used

Angular frequency of a harmonic oscillator

Given

  • (N/m)
  • (kg)
A Particle in a Well of Finite Height
Applications of Tunneling