1. Solve the Schrodinger equation for a particle of mass, m, in a box. The box is modeled as an infinite potential well that is V, inside the region from 0 < x < L and there is an infinite amount of potential energy outside this region. Remark: The only difference between this problem and the one we worked out in a previous lecture is that now the constant potential energy inside the box can be any value, whereas, in the previous lecture, we considered the special case that V, = 0.
1. Solve the Schrodinger equation for a particle of mass, m, in a box. The box is modeled as an infinite potential well that is V, inside the region from 0 < x < L and there is an infinite amount of potential energy outside this region. Remark: The only difference between this problem and the one we worked out in a previous lecture is that now the constant potential energy inside the box can be any value, whereas, in the previous lecture, we considered the special case that V, = 0.
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