Answers to drylab-II-The postulates - Cobalt
Answers to drylab-II-The postulates - Cobalt
Answers to drylab-II-The postulates - Cobalt
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CHEMISTRY 373 - DRY LAB <strong>II</strong><br />
PRACTICE FOR THE QUANTUM MECHANICAL POSTULATES<br />
Practice Problems for January<br />
A. Questions on Postulate 1.<br />
1. Which of the following mathematical functions is a well-behaved wave function:<br />
(a) e kx2 ,K < x < +K, k > 0, (b) e kx2 ,K < x < +K, k > 0<br />
(c) e imx ,K < x < +K, m a real number<br />
(Answer: (a) This is a well behaved function. It is continuous, single-valued, and vanishes as<br />
x ¸ ±K. (b) Blows up as x ¸ ±K. (c) This function is continuous and single-valued but is not<br />
defined in the limit asx ¸ ±K.Þ<br />
2. Show that the wave functions<br />
1<br />
f 1 ÝxÞ = 2 2 sin ^x<br />
L L<br />
1<br />
, f 2 ÝxÞ = 2 2 sin 2^x<br />
L L<br />
for the first two levels of a particle in a 1-dimensional box are orthonormal.<br />
B. Questions on Postulate 2 and commuta<strong>to</strong>rs.<br />
1. Find the quantum mechanical opera<strong>to</strong>rs corresponding <strong>to</strong> the following classical quantities:<br />
xp x , p 2 x + x 2 , p 2 x + p 2 y + g 2 Ýx 2 + y 2 Þ + Ux.<br />
(<strong>Answers</strong>:<br />
xp x ¸ åx å p x + å å<br />
p xx = i¥ x<br />
/<br />
+ / x , Tricky. Later we will learn that xp /x /x x is a classical<br />
observable and must correspond <strong>to</strong> a Hermitian opera<strong>to</strong>r in quantum mechanics. <strong>The</strong> opera<strong>to</strong>r<br />
åå xp x is not Hermitian (next question) but å x å p x + å å<br />
p xx is.<br />
p x 2 + x 2 ¸ åp<br />
x 2 + å x 2 = ¥ 2 /2<br />
/x 2 + x 2 ,<br />
p x 2 + p y 2 + g 2 Ýx 2 + y 2 Þ + Ux ¸ åp<br />
x 2 + å p y 2 + g 2 Ý å x 2 + å y 2 Þ + U å x<br />
= ¥ 2 /2<br />
/x 2 + /2<br />
/y 2 + g 2 Ýx 2 + y 2 Þ + Ux.<br />
)<br />
2. Which of the following opera<strong>to</strong>rs are self-adjoint or Hermitian:<br />
å p 2 z ,<br />
åå xp y å y å p x ,<br />
åå xp x <br />
3. What is the adjoint of the opera<strong>to</strong>r å x å p x <br />
(Answer:<br />
å å p xx + i¥.<br />
)<br />
4. Evaluate the following commuta<strong>to</strong>r brackets:<br />
where the Hamil<strong>to</strong>nian, H = ¥2<br />
2m<br />
ß å x, å p x 2 à, ß å x å p y å y å p x , å y å p z å z å p y à, ßH, å xà.<br />
/ 2<br />
/x 2 + VÝxÞ, is for a 1-dimensional system only.<br />
(<strong>Answers</strong>: Use the fact that ß å x, å p x à = ß å y, å p y à = ß å z, å p z à = i¥ and ß å x, å p y à = 0, etc., as well as the<br />
commuta<strong>to</strong>r identities ßAB,Cà = AßB,Cà + ßA,CàB andßA,BCà = BßA,Cà + ßA,BàC.<br />
ß å x, å p x 2 à = 2i¥ å p x ,ß å x å p y å y å p x , å y å p z å z å p y à = i¥Ý å z å p x å x å p z Þ,<br />
ßH, å xà = ß px 2<br />
2m + VÝå xÞ, å xà = 1<br />
2m ßå x, å p x 2 à = i m ¥ å p x<br />
,
)<br />
C. Questions on Postulate 3.<br />
1. Which of the following functions are eigenfunctions of d2<br />
dx 2<br />
2. Solve the following eigenvalue equation:<br />
(Answer:<br />
iJ<br />
Af = Jf ö xf x = f ö f = Nx iJ ¥ .<br />
¥<br />
)<br />
3. Show that the two opera<strong>to</strong>rs<br />
A = x / /x<br />
e kx2 ,x 2 ,coskx + sinkx.<br />
Af = Jf, A = å x å p x .<br />
/2<br />
+ K, B = x2 + ÝJ KÞ<br />
2<br />
/x<br />
and identify the eigenvalues:<br />
(with J,K constant) commute. Suppose that fÝxÞ is an eigenfunction of A with eigenvalue J, i.e.,<br />
Af = Jf.<br />
<strong>The</strong>n, find f. Also, show that f is simultaneously an eigenfunction of the opera<strong>to</strong>r B with<br />
eigenvalue ÝJ KÞ 2 .<br />
(Answer:<br />
fÝxÞ = Nx JK , then compute Bf.<br />
)<br />
D. Questions on Postulate 5.<br />
1. For a particle in a 1-dimensional box, calculate the expectation values < å x å p x > and < å p x<br />
å x > for<br />
the ground state. Are they real Are they equal Explain. Are the expectation values the same<br />
for all states of the particle in a 1-dimensional box<br />
(Answer:<br />
i¥ 2 L<br />
X<br />
L sin<br />
n^x d<br />
x sin n^x<br />
0 L dx L<br />
dx = 1 2 i¥ 2n^cos2 n^n^cosn^sinn^<br />
n^ = 1 2 i¥<br />
i¥ 2 L<br />
X<br />
L sin<br />
n^x d<br />
x sin n^x dx = 1 i¥ cosn^sinn^3n^+2n^cos2 n^<br />
0 L dx L<br />
2 n^ = 1 i¥ 2<br />
<strong>The</strong> opera<strong>to</strong>rs for å x å p x and for å å<br />
p xx are not self-adjoint.)