Page 237 - Instant notes
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The wave nature of matter     223


        and remembering that ħ=h/2π gives:





        The final result is de Broglie’s equation, i.e. the Schrödinger equation reproduces the
        experimental observation that a freely moving particle can be described as a sine wave of
        wavelength inversely proportional to the particle momentum.


                                   Boundary conditions

        In principle, there are an infinite number of solutions to the Schrödinger equation. If
        sin(kx) is a solution then so is asin(bkx) for all values of a and b. However, only a sub-set
        of solutions are allowed physically and these are determined by the boundary conditions
        imposed by the physical situation which the Schrödinger equation describes. Examples
        are shown for a particle in a box or an electron in the hydrogen atom (Topic G5). The
        fact that only certain values of E and ψ are allowed solutions of a particular Schrödinger
        equation is the origin of the quantization of energy (Topic G3).


                             Heisenberg’s uncertainty principle

        The wavefunction description of a moving particle replaces the classical concept that the
        particle moves with known velocity along a precisely defined trajectory. Combination of
        the Schrödinger and de Broglie equations shows that the wavefunction of a particle of
        momentum p moving freely in the x direction is:



        with wavelength  λ=h/p.  The  wavefunction  has constant wavelength and peak-to-peak
        amplitude at all positions, corresponding to equal probability of finding the particle at any
        of an infinite number of points in the x direction. Therefore, although the momentum of
        the particle is known exactly, its position is uncertain. The converse situation, in which
        the position of the particle in space is known exactly, requires a wavefunction which has
        zero amplitude everywhere except at the particle’s position (Fig. 1a), and can only be
        achieved through the superposition of an infinite number of wavefunctions of different
        wavelengths, corresponding to an infinite range in particle momentum (Fig. 1b). These
        outcomes are encapsulated in Heisenberg’s Uncertainty Principle:

              It is impossible to specify simultaneously both the position and momentum
              of a particle exactly.
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