8.3 Solutions 451
ThereforeJ=
2 ER
ω
=
2 × 537. 5 × 1. 6 × 10 −^13
2. 6 × 1023
= 6. 61 × 10 −^34 Js=h
8.10 (a) IfJbe the electronic angular momentum andIthe nuclear spin, the mul-
tiplicity is given by (2J+1) or (2I+1), whichever is smaller.
Now, 2J+ 1 = 2 ×
5
2
+ 1 =6. But only four terms are found. Therefore,
the multiplicity is given by 2I+ 1 =4, whenceI= 3 /2.
(b) The magnetic field produced by the electron interacts with the nuclear
magnetic moment resulting in the energy shift in hyperfine structure.
ΔE≈ 2 I.J=F(F+1)−I(I+1)−J(J+1)
where,F=I+Jtakes on integral values from 4 to 1.
F= 4 ,ΔE= 20 − 25 / 2
F= 3 ,ΔE= 12 − 25 / 2
F= 2 ,ΔE= 6 − 25 / 2
F= 1 ,ΔE= 2 − 25 / 2
The intervals are 8, 6 and 4 in the ratio 4:3:2
8.11 The resonance frequencyνis given by
ν=
μβ
Ih
whereμis the magnetic moment, B the magnetic induction,Ithe nuclear spin
in units of. A nuclear magnetonμN= 5. 05 × 10 −^27 JT−^1.
B=
νIh
μ
=
60 × 106 ×(1/2)× 6. 625 × 10 −^34
2. 79 × 5. 05 × 10 −^27
= 1 .4T
8.12 f=
μB
Jh
=
3. 46 × 3. 15 × 10 −^14 × 1. 6 × 10 −^13 × 0. 8
(
7
2
)
× 6. 63 × 10 −^34
= 6. 012 × 106 Hz
= 6 .012 MHz
8.3.4 Electric Quadrupole Moment........................
8.13 Quadrupole Moment
Assume that the charge is uniformly distributed over an ellipsoid of revolution,
with the axis of symmetry along thez/-axis, the semi-major axis of lengtha,
and the other two semi-axes of lengthb. The charge densityρis
ρ=
Ze
volume
=
Ze
4 π
3 ab
2