Chapter 5: Q62E (page 191)
What is the product of uncertainties determined in Exercise 60 and 61? Explain.
Short Answer
The product of uncertainty in position and momentum is , which is in accordance with the uncertainty principle.
Chapter 5: Q62E (page 191)
What is the product of uncertainties determined in Exercise 60 and 61? Explain.
The product of uncertainty in position and momentum is , which is in accordance with the uncertainty principle.
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Get started for freeSketch . Would you expect this wave function to be the ground state? Why or why not?
It is possible to take the finite well wave functions further than (21) without approximation, eliminating all but one normalization constant . First, use the continuity/smoothness conditions to eliminate , , and in favor of in (21). Then make the change of variables and use the trigonometric relations
and
on the
functions in region I, . The change of variables shifts the problem so that it is symmetric about , which requires that the probability density be symmetric and thus that be either an odd or even function of . By comparing the region II and region III functions, argue that this in turn demands that must be either +1 (even) or -1 (odd). Next, show that these conditions can be expressed, respectively, as and . Finally, plug these separately back into the region I solutions and show that
or
Note that is now a standard multiplicative normalization constant. Setting the integral of over all space to 1 would give it in terms of and , but because we can’t solve (22) exactly for k(or E), neither can we obtain an exact value for .
Write out the total wave function.For an electron in the n=3 state of a 10nm wide infinite well. Other than the symbols a and t, the function should include only numerical values?
Where would a particle in the first excited state (first above ground) of an infinite well most likely be found?
Show that the uncertainty in the momentum of a ground state harmonic oscillator is .
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