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Particle in a Box
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Class Objectives Introduce the idea of a free particle.
Solve the TISE for the free particle case.
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Particle in a Box The best way to understand Schrödinger’s equation is to solve it for various potentials.
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Particle in a Box The best way to understand Schrödinger’s equation is to solve it for various potentials. The simplest of these involving forces is particle confinement (a particle in a box).
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Particle in a Box Consider a particle confined along the x axis between the points x = 0 and x = L.
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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.
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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.
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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 L
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Particle in a Box U E: total energy of the particle
E: total energy of the particle U: potential containing the particle. The Pd of the walls. E<U
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Particle in a Box Inside the well the particle is free. U
E: total energy of the particle U: potential containing the particle. The Pd of the walls. E<U Inside the well the particle is free.
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Particle in a Box Inside the well the particle is “free”.
U L E: total energy of the particle U: potential containing the particle. The Pd of the walls. E<U Inside the well the particle is “free”. This is because is zero inside the well.
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Particle in a Box Inside the well the particle is “free”.
U L E: total energy of the particle U: potential containing the particle. The Pd of the walls. E<U 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.
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Infinite square potential
L x
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Particle in a Box Classically there is no restriction on the energy or momentum of the particle.
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Particle in a Box Classically there is no restriction on the energy or momentum of the particle. However from QM we have energy quantization.
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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
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Particle in a Box Since we get that, we take,
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Particle in a Box Since we get that, So that we take,
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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)
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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!
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Particle in a Box Therefore the wave must be zero at the boundaries, x=0 and x=L.
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Particle in a Box Therefore the wave must be zero at the boundaries, x=0 and x=L. At x=0,
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Particle in a Box Therefore the wave must be zero at the boundaries, x=0 and x=L. At x=0,
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Particle in a Box Therefore the wave must be zero at the boundaries, x=0 and x=L. At x=0,
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Particle in a Box Therefore the wave must be zero at the boundaries, x=0 and x=L. At x=0, At x=L,
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Particle in a Box Therefore the wave must be zero at the boundaries, x=0 and x=L. At x=0, At x=L, Since , then , Recall:
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Particle in a Box From this we find that particle energy is quantized. The restricted values are
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Particle in a Box From this we find that particle energy is quantized. The restricted values are Note E=0 is not allowed!
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Particle in a Box From this we find that particle energy is quantized. The restricted values are Note E=0 is not allowed! N=1 is ground state and n=2,3… excited states.
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Particle in a Box Finally, given k and B we write the waveform as
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Particle in a Box Finally, given k and B we write the waveform as
We need to determine A.
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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.
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Particle in a Box Normalising,
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Particle in a Box Normalising,
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Particle in a Box Normalising,
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Particle in a Box Normalising,
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Particle in a Box Normalising,
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Particle in a Box Normalising,
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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 .
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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.
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Particle in a Box
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