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A wave function with a non-infinite wavelength-however approximate it might be- has nonzero momentum and thus nonzero kinetic energy. Even a single "bump" has kinetic energy. In either case, we can say that the function has kinetic energy because it has curvature- a second derivative. Indeed, the kinetic energy operator in any coordinate system involves a second derivative. The only function without kinetic energy would be a straight line. As a special case, this includes a constant, which may be thought of as a function with an infinite wavelength. By looking at the curvature in the appropriate dimension(s). answer the following: For a givenn,isthe kinetic energy solely

(a) radial in the state of lowest l- that is, l=0; and

(b) rotational in the state of highest l-that is, l=n-1?

Short Answer

Expert verified
  1. Yes, The kinetic energy is solely radial.
  2. No, Kinetic energy is not solely rotational.

Step by step solution

01

 Given data

Orbital angular momentum, l = 0.

Orbital angular momentum, l = n – 1.

02

 (a) To determine the kinetic energy solely radial in case of l = 0

The only angular solution to the l =0 state is a constant that has no curvature and thus has zero rotational kinetic energy. Hence, for any n, the state of lowest l must have only radial kinetic energy.

Thus, the kinetic energy is solely radial.

03

 To determine the kinetic energy solely rotational in case of l = n – 1

The radial solution, for a given n, to the l = n – 1 state is never constant, involves an exponential part, which has a curvature, and thus has nonzero radial kinetic energy.Hence, for any n, the state of highest l cannot be only rotational kinetic energy.

The wave function for the atom with the highest l still has radial dependence, so the kinetic energy is not solely rotational

No, kinetic energy is not solely rotational.

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Most popular questions from this chapter

Calculate the “series limit” of the Lyman series of spectral lines. This is defined as the shortest wavelength possible of a photon emitted in a transition from a higher initial energy level to the ni=1 final level. (Note: In figure 7.5, the spectral lines of the series “crowd together” at the short-wavelength end of the series).

A spherical infinite well has potential energy

U(r)={0r<a+r>a

Since this is a central force, we may use the Schrodinger equation in the form (7-30)-that is, just before the specific hydrogen atom potential energy is inserted. Show that the following is a solution

R(r)=Asinbrr

Now apply the appropriate boundary conditions. and in so doing, find the allowed angular momenta and energies for solutions of this form.

Classically, what happens when a moving object has a head-on elastic collision with a stationary object of exactly equal mass? What if it strikes an object of smaller mass? Of larger mass? How do these ideas relate to Rutherford’s conclusion about the nature of the atom?

Taking then=3states as representative, explain the relationship between the complexity numbers of nodes and antinodes-of hydrogen's standing waves in the radial direction and their complexity in the angular direction at a given value of n. Is it a direct or inverse relationship, and why?

Knowing precisely all components of a nonzero Lwould violate the uncertainty principle, but knowingthat Lis precisely zerodoes not. Why not?

(Hint:For l=0 states, the momentum vector p is radial.)

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