Chapter 5: Problem 5
Just what is stationary in a stationary state? The particle? Something else?
Short Answer
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Chapter 5: Problem 5
Just what is stationary in a stationary state? The particle? Something else?
These are the key concepts you need to understand to accurately answer the question.
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Get started for freeExercises \(78-88\) refer to a particle of mass \(m\) described by the wave function $$ \psi(x)=\left\\{\begin{array}{ll} 2 \sqrt{a^{3}} x e^{-a x} & x>0 \\ 0 & x<0 \end{array}\right. $$ Verify that the normalization constant \(2 \sqrt{a^{3}}\) is correct.
Exercises \(90-92\) refer to a particle described by the wave function $$ \psi(x)=\sqrt{\frac{2}{\pi}} a^{3 / 2} \frac{1}{x^{2}+a^{2}} $$ Show that the normalization constant is correct.
The term interaction is sometimes used interchangeably with for'e, and (other times interchangeably with potential energy. Although force and potential energy certainly aren't the same thing, what justification is there for using the same term to cover both?
A particle is described by the wave function $$ \psi(x)=\frac{\sqrt{2 / \pi}}{x^{2}-x+1.25} $$ (a) Show that the normalization constant \(\sqrt{2 / \pi}\) is correct. (b) A measurement of the position of the particle is to be made. At what location is it most probable that the particle would be found? (c) What is the probability per unit length of finding the particle at this location?
Whereas an infinite well has an infinite number of bound states, a finite well does not. By relating the well height \(U_{0}\) to the kinetic energy and the kinetic energy (through \(\lambda\) ) to \(n\) and \(L\). show that the number of bound states is given roughly by \(\sqrt{8 m L^{2} U_{0} / h^{2}}\). (Assume that the number is Large.)
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