12.14
12.15
The limits are r=1.058 or x=2 and infinity so the probability is
equal to:
0 −(−e−^4 (2 × 42 + 2 × 4 +1)) =0.75
12.16
The limits are r=0.5 Å or x=1 and r=1.058 Å or x=2, so the
probability is:
− 4 e−^4 (2 × 4 + 4 +1) + 4 e−^2 (2 + 2 +1) =−0.44 +0.68 =0.24
12.17 The most probable radial position of the electron is simply the peak
position of this term. We can find the peak by setting the derivative
equal to zero:
12.18
=
3
2
a 0
4
44
0
3
0
2
0
32
0
0
0 2
a
rera r a xex x ae
∞
− −
∞
−
∫∫==
/ ddxx⎛−− − −xxx
⎝
⎜⎜
⎞
⎠
⎟⎟
32 ∞
(^20)
3
4
3
4
3
8
ψψτ
π
*drr π d
a
= errra/
⎛
⎝
⎜
⎜
⎞
⎠
⎟
⎟
− =
∞ ∞
∫∫
1
4
0
2
0 0
0 2 4 /
0
3
0
(^20)
a
rera r
∞
−
∫ d
0
8
1
0
3
2
0
0
=−/^0
⎛
⎝
⎜⎜
⎞
⎠
− ⎟⎟ =
a
er
r
a
ra or ra
04
2 14
0
3
2
0
3
= /^0 (
⎛
⎝
⎜⎜
⎞
⎠
− ⎟⎟=
d
d
d
r d
r
a
e
ar
π ra r
π
(^22) e−^2 ra/ (^0) )
04 = ()^2
d
d
*
r
πψψr
letxra/ then d d
a
== 0 ∫err ex−ra/ −x
0
3
(^4202242) xxex x=− x()+ +
∫
− (^22221)
1
4
4
0
3
2
2
0
3
002 2
π
π
a
err
a
−−ra erra
⎛
⎝
⎜
⎜
⎞
⎠
⎟
⎟
∫ //dd= ∫ dr
letxra/ then / d
a
== 0 ∫err ex−ra −x
0
3
(^4202242) ddxex x=− x()+ +
∫
− (^22221)
1
4
4
0
3
2
2
0
3
0 2 02
π
π
a
err
a
−ra er−ra
⎛
⎝
⎜
⎜
⎞
⎠
⎟
⎟
∫ / dd= ∫ / dr
ψψψpppx=− ()()+−− =xf r
1
2
468 ANSWERS TO PROBLEMS
9781405124362_5_end.qxd 4/29/08 9:17 Page 468