Chapter 5: Q82CE (page 193)
Calculate the expectation value of the position of the particle.
Short Answer
The expectation value of the position of the particle is .
Chapter 5: Q82CE (page 193)
Calculate the expectation value of the position of the particle.
The expectation value of the position of the particle is .
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Get started for freeWhen is the temporal part of the wave function ? Why is this important?
The figure shows a potential energy function.
(a) How much energy could a classical particle have and still be bound?
(b) Where would an unbound particle have its maximum kinetic energy?
(c) For what range of energies might a classical particle be bound in either of two different regions?
(d) Do you think that a quantum mechanical particle with energy in the range referred to in part?
(e) Would be bound in one region or the other? Explain.
There are mathematical solutions to the Schrödinger equation for the finite well for any energy, and in fact. They can be made smooth everywhere. Guided by A Closer Look: Solving the Finite Well. Show this as follows:
(a) Don't throw out any mathematical solutions. That is in region Il , assume that , and in region III , assume that. Write the smoothness conditions.
(b) In Section 5.6. the smoothness conditions were combined to eliminate in favor of . In the remaining equation. canceled. leaving an equation involving only and , solvable for only certain values of . Why can't this be done here?
(c) Our solution is smooth. What is still wrong with it physically?
(d) Show that
localid="1660137122940"
and that setting these offending coefficients to 0 reproduces quantization condition (5-22).
For a total energy of 0, the potential energy is given in Exercise 96. (a) Given these, to what region of the x-axis would a classical particle be restricted? Is the quantum-mechanical particle similarly restricted? (b) Write an expression for the probability that the (quantum-mechanical) particle would be found in the classically forbidden region, leaving it in the form of an integral. (The integral cannot be evaluated in closed form.)
A finite potential energy function U(x) allows the solution of the time-independent Schrödinger equation. to penetrate the classically forbidden region. Without assuming any particular function for U(x) show that b(x) must have an inflection point at any value of x where it enters a classically forbidden region.
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