226 Chapter Six
EXERCISES
To strive, to seek, to find, and not to yield. —Alfred, Lord Tennyson
6.3 Quantum Numbers
- Why is it natural that three quantum numbers are needed to
describe an atomic electron (apart from electron spin)? - Show that
20 () (3 cos^2 1)
is a solution of Eq. (6.13) and that it is normalized.
- Show that
R 10 (r) er^ a^0
is a solution of Eq. (6.14) and that it is normalized.
- Show that
R 21 (r) er^2 a^0
is a solution of Eq. (6.14) and that it is normalized.
- In Exercise 12 of Chap. 5 it was stated that an important
property of the eigenfunctions of a system is that they are
orthogonal to one another, which means that
*nmdV 0 nm
r
a 0
^1
2 6 a 03 2
^2
a 03 2
10
4
Verify that this is true for the azimuthal wave functions (^) mlof
the hydrogen atom by calculating
2
0
*ml (^) mld
for mlml.
- The azimuthal wave function for the hydrogen atom is
()Aeiml
Show that the value of the normalization constant Ais 1 2
by integrating | |^2 over all angles from 0 to 2.
6.4 Principal Quantum Number
6.5 Orbital Quantum Number
- Compare the angular momentum of a ground-state electron in
the Bohr model of the hydrogen atom with its value in the
quantum theory. - (a) What is Schrödinger’s equation for a particle of mass m
that is constrained to move in a circle of radius R, so that
depends only on ? (b) Solve this equation for and evaluate
the normalization constant. (Hint: Review the solution of
Schrödinger’s equation for the hydrogen atom.) (c) Find the
possible energies of the particle. (d) Find the possible angular
momenta of the particle.
Example 6.4
A sample of a certain element is placed in a 0.300-T magnetic field and suitably excited. How
far apart are the Zeeman components of the 450-nm spectral line of this element?
Solution
The separation of the Zeeman components is
Since c , dc d ^2 , and so, disregarding the minus sign,
2.83 10 ^12 m0.00283 nm
(1.60^10 ^19 C)(0.300 T)(4.50^10 ^7 m)^2
(4)(9.11 10 ^31 kg)(3.00 108 m/s)
eB 2
4 mc
2
c
eB
4 m
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