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Particle in a Box

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Particle in a Box Class Objectives Introduce the idea of a free particle. Solve the TISE for the free particle case. Particle in a Box The best way to understand ... – PowerPoint PPT presentation

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Title: Particle in a Box


1
Particle in a Box
2
Class Objectives
  • Introduce the idea of a free particle.
  • Solve the TISE for the free particle case.

3
Particle in a Box
  • The best way to understand Schrödingers equation
    is to solve it for various potentials.

4
Particle in a Box
  • The best way to understand Schrödingers equation
    is to solve it for various potentials.
  • The simplest of these involving forces is
    particle confinement (a particle in a box).

5
Particle in a Box
  • Consider a particle confined along the x axis
    between the points x 0 and x L.

6
Particle in a Box
  • Consider a particle confined along the x axis
    between the points x 0 and x L.
  • Inside the box it free but at the edges it
    experiences strong forces which keep it confined.

7
Particle in a Box
  • Consider a particle confined along the x axis
    between the points x 0 and x L.
  • Inside the box it free but at the edges it
    experiences strong forces which keep it confined.
    Eg. A ball bouncing between 2 impenetrable walls.

8
Particle in a Box
  • Consider a particle confined along the x axis
    between the points x 0 and x L.
  • Inside the box it free but at the edges it
    experiences strong forces which keep it confined.
    Eg. A ball bouncing between 2 impenetrable walls.

U
E
0
L
9
Particle in a Box
10
Particle in a Box
  • Inside the well the particle is free.

11
Particle in a Box
  • Inside the well the particle is free.
  • This is because is zero inside the well.

12
Particle in a Box
  • Inside the well the particle is free.
  • This is because is zero inside the well.
  • Increasing to infinity as the width is
    reduced to zero, we have the idealization of an
    infinite potential square well.

13
Infinite square potential
U
L
0
x
14
Particle in a Box
  • Classically there is no restriction on the energy
    or momentum of the particle.

15
Particle in a Box
  • Classically there is no restriction on the energy
    or momentum of the particle.
  • However from QM we have energy quantization.

16
Particle in a Box
  • We are interested in the time independent
    waveform of the particle.
  • The particle can never be found outside the well.
    Ie. in the region

17
Particle in a Box
  • Since we get that,

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Particle in a Box
  • Since we get that,
  • So that

19
Particle in a Box
  • The solutions to this equation are of the form
    for
    (a linear combination of cosine and sine waves of
    wave number k)

20
Particle in a Box
  • The solutions to this equation are of the form
    for
    (a linear combination of cosine and sine waves of
    wave number k)
  • The interior wave must match the exterior wave at
    the boundaries of the well. Ie. To be continuous!

21
Particle in a Box
  • Therefore the wave must be zero at the
    boundaries, x0 and xL.

22
Particle in a Box
  • Therefore the wave must be zero at the
    boundaries, x0 and xL.
  • At x0,

23
Particle in a Box
  • Therefore the wave must be zero at the
    boundaries, x0 and xL.
  • At x0,

24
Particle in a Box
  • Therefore the wave must be zero at the
    boundaries, x0 and xL.
  • At x0,

25
Particle in a Box
  • Therefore the wave must be zero at the
    boundaries, x0 and xL.
  • At x0,
  • At xL,

26
Particle in a Box
  • Therefore the wave must be zero at the
    boundaries, x0 and xL.
  • At x0,
  • At xL,
  • Since , then
  • ,
  • Recall

27
Particle in a Box
  • From this we find that particle energy is
    quantized. The restricted values are

28
Particle in a Box
  • From this we find that particle energy is
    quantized. The restricted values are
  • Note E0 is not allowed!

29
Particle in a Box
  • From this we find that particle energy is
    quantized. The restricted values are
  • Note E0 is not allowed!
  • N1 is ground state and n2,3 excited states.

30
Particle in a Box
  • Finally, given k and B we write the waveform as

31
Particle in a Box
  • Finally, given k and B we write the waveform as
  • We need to determine A.

32
Particle in a Box
  • Finally, given k and B we write the waveform as
  • We need to determine A.
  • To do this we need to normalise.

33
Particle in a Box
  • Normalising,

34
Particle in a Box
  • Normalising,

35
Particle in a Box
  • Normalising,

36
Particle in a Box
  • Normalising,

37
Particle in a Box
  • Normalising,

38
Particle in a Box
  • Normalising,

39
Particle in a Box
  • For each value of the quantum number n there is a
    specific waveform describing the state of a
    particle with energy .

40
Particle in a Box
  • For each value of the quantum number n there is a
    specific waveform describing the state of a
    particle with energy .
  • The following are plots of vs x and the
    probability density vs x.

41
Particle in a Box
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