serway1 (1)

Nuclear Structure 551

Section 44.5 The Decay Processes

P44.28 (a) A gamma ray has zero charge and it contains no protons or neutrons. So for a gamma

ray Z = 0 and A = 0. Keeping the total values of Z and A for the system conserved then

requires Z = 28 and A = 65 for X. With this atomic number it must be nickel, and the

nucleus must be in an exited state, so it is 65 Ni* .
28

(b) α = 4 He has Z=2 and A=4
2

so for X we require Z = 84 − 2 = 82

for Pb and A = 215 − 4 = 211, X = 211 Pb
82

(c) A positron e+ = 0 e has charge the same as a nucleus with Z = 1. A neutrino 00ν has
1

no charge. Neither contains any protons or neutrons. So X must have by conservation

Z = 26 +1= 27. It is Co. And A = 55 + 0 = 55. It is 55 Co.
27

Similar reasoning about balancing the sums of Z and A across the reaction reveals:

(d) 0 e
−1

(e) 1 H (or p). Note that this process is a nuclear reaction, rather than radioactive decay. We
1

can solve it from the same principles, which are fundamentally conservation of charge and

conservation of baryon number.

P44.29 ( )( )Q = M U-238 − M Th-234 − M He-4 931.5 MeV u

Q = (238.050 783 − 234.043 596 − 4.002 603) u(931.5 MeV u) = 4.27 MeV

⎛ 0.021 0g ⎞
⎜⎝ 12.0 g mol ⎠⎟
( )P44.30
NC = 6.02 × 1023 molecules mol

( )NC = 1.05 × 1021 carbon atoms of which 1 in 7.70 × 1011 is a 14C atom

( )N0 = 1.37 × 109, λC-14 = ln 2 = 1.21 × 10−4 yr −1 = 3.83 × 10−12 s−1
5 730 yr
C-14

R = λN = λN0e−λt

( )( )R0 = λ N0 = 3.83 × 10−12 s−1 ⎡ 7(86 400 s) ⎤
At t = 0, 1.37 × 109
⎣⎢ 1 week ⎥⎦

= 3.17 × 103 decays week

At time t, R = 837 = 951 decays week
0.88

Taking logarithms, ln R = −λ t so t = −1 ln ⎛ R ⎞
R0 λ ⎝⎜ R0 ⎠⎟

t = −1 yr −1 ⎛ 951 ⎞ = 9.96 × 103 yr
1.21 × 10−4 ln ⎝⎜ 3.17 × 103 ⎟⎠

552 Chapter 44

*P44.31 (a) The decay constant is λ = ln 2/10 h = 0.0693/h.
The number of parent nuclei is given by 106 e−0.0693 t where t is in hours.
The number of daughter nuclei is equal to the number of missing parent nuclei,

Nd = 106 − 106 e−0.0693t Nd = 106(1 − e )−0.0693t where t is in hours .

(b) The number of daughter nuclei starts from zero at t = 0. The number of stable product
nuclei always increases with time and asymptotically approaches 1.00 × 106 as t increases
without limit.
Its rate of increase is dNd = 106 (0 + 0.0693 e−0.0693t ) = 6.93 × 104 1 e−0.0693t .
dt h

The number of daughter nuclei first increases most rapidly, at 6.93 × 104/h, and then more
and more slowly. Its rate of change approaches zero in the far future.

P44.32 3 H nucleus → 3 He nucleus + e− + ν
1 2

becomes 3 H nucleus + e− → 3 He nucleus + 2e− +ν
1 2

Ignoring the slight difference in ionization energies,

we have 3 H atom → 3 He atom +ν
1 2

3.016 049 u = 3.016 029 u + 0 + Q
c2

Q = (3.016 049 u − 3.016 029 u)(931.5 MeV u) = 0.018 6 MeV = 18.6 keV

P44.33 (a) e− + p → n + ν

(b) For nuclei, 15 O + e− → 15 N + ν 15 O atom → 15 N atom + ν
Add seven electrons to both sides to obtain 8 7

( ) ( )m Q
(c) From the table of isotopic masses in the chapter text, 15 O =m 15 N + c2
∆m = 15.003 065 u − 15.000 109 u = 0.002 956 u

Q = (931.5 MeV u)(0.002 956 u) = 2.75 MeV

P44.34 (a) For e+ decay,

Q = (M X − MY − 2me )c2 = ⎡⎣39.962 591 u − 39.963 999 u − 2(0.000 549 u)⎤⎦(931.5 MeV u)

Q = −2.33 MeV
Since Q < 0, the decay cannot occur spontaneously.

(b) For alpha decay,

Q = (M X − Mα − )MY c2 = [97.905 287 u − 4.002 603 u − 93.905 088 u](931.5 MeV u)

Q = −2.24 MeV
Since Q < 0, the decay cannot occur spontaneously.

(c) For alpha decay,

Q = (M X − Mα − )MY c2 = [143.910 083 u − 4.002 603 u − 139.905 434 u](931.5 MeV u)

Q = 1.91 MeV

Since Q > 0, the decay can occur spontaneously.

Nuclear Structure 553

Section 44.6 Natural Radioactivity
P44.35

FIG. P44.35

P44.36 (a) Let N be the number of 238 U nuclei and N ′ be 206 Pb nuclei.

Then N = N0e−λ t and N0 = N + N′ so N = (N + N ′)e−λt or eλ t =1+ N′.
N

Taking logarithms, λ t = ln ⎛⎜⎝1 + N′ ⎠⎞⎟ where λ = ln 2
N T1 2

Thus, t = ⎛ T1 2 ⎞ ln ⎜⎛⎝1+ N′ ⎟⎠⎞
⎜⎝ ln 2⎠⎟ N

If N = 1.164 for the 238 U → 206 Pb chain with T1 2 = 4.47 × 109 yr, the age is:
N′

t = ⎛ 4.47 × 109 yr ⎞ ln ⎝⎛1 + 1 ⎞ = 4.00 × 109 yr
⎝⎜ ln 2 ⎟⎠ 1.164 ⎠

(b) From above, eλt = 1 + N ′ . Solving for N gives N = e−λ t .
N N′ N′ 1 − e−λt

With t = 4.00 × 109 yr and T1 2 = 7.04 × 108 yr for the 235 U → 207 Pb chain,

( )λ
t = ⎛ ln 2⎞ t = (ln 2) 4.00 × 109 yr = 3.938 and N = 0.019 9
⎜⎝ T1 2 ⎠⎟ N′
7.04 × 108 yr

With t = 4.00 × 109 yr and T1 2 = 1.41 × 1010 yr for the 232 Th → 208 Pb chain,

( )(ln 2) 4.00 × 109 yr N = 4.60
N′
λ t = 1.41 × 1010 yr = 0.196 6 and

554 Chapter 44

P44.37 (a) 4.00 pCi L = ⎛ 4.00 × 10−12 Ci⎞ ⎛ 3.70 × 1010 Bq⎞ ⎛ 1.00 × 103 L⎞ = 148 Bq m3
⎜⎝ 1L ⎠⎟ ⎜⎝ 1 Ci ⎟⎠ ⎜⎝ 1 m3 ⎟⎠

( )(b) = R = ⎛ T1 2 ⎞ = Bq m3 ⎜⎛⎝ 3.82 d ⎟⎞⎠ ⎝⎜⎛ 86 400 s ⎟⎞⎠ = 7.05 × 107 atoms m3
N λ R ⎜⎝ ln 2⎠⎟ 148 ln2 1d

( )(c) m3 ⎛⎝⎜ 1 mol ⎞⎠⎟ ⎝⎛⎜ 122m2ogl ⎠⎟⎞ × 10−14 m3
mass = 7.05 × 107 atoms 6.02 × 1023 atoms = 2.60 g

Since air has a density of 1.20 kg m3, the fraction consisting of radon is

fraction = 2.60 × 10−14 g m3 = 2.17 × 10−17
1 200 g m3
.

P44.38 Number remaining: N = N0e−(ln 2)t T1 2
Fraction remaining: N = e−λ t = e−(ln 2)t T1 2
N0

(a) With T1 2 = 3.82 d and t = 7.00 d, N = e =−(ln 2)(7.00) (3.82) 0.281
N0

(b) When t = 1.00 yr = 365.25 d, N = e =−(ln 2)(365.25) (3.82) 1.65 × 10−29
N0

(c) Radon is continuously created as one daughter in the series of decays starting from the
long-lived isotope 238 U.

Section 44.7 Nuclear Reactions

P44.39 (a) For X, A = 24 + 1− 4 = 21 so X is 21 Ne
and Z = 12 + 0 − 2 = 10, 10

(b) A = 235 + 1− 90 − 2 = 144

and Z = 92 + 0 − 38 − 0 = 54, so X is 144 Xe
54

(c) A = 2 − 2 = 0 so X must be a positron.
and Z = 2 − 1 = +1,
As it is ejected, so is a neutrino: X = 0 e + and X′ = 00ν
1

Nuclear Structure 555

P44.40 (a) Add two electrons to both sides of the reaction to have it in neutral-atom terms:

4 1 H atom → 4 He atom +Q Q = ∆mc2 = ⎡⎣4 M − M ⎤⎦ c 2
1 2
1 H 4 He
1 2

Q = ⎣⎡4(1.007 825 u) − 4.002 603 u ⎦⎤ (931.5 MeV u ) ⎛ 1.60 × 10−13 J⎞ = 4.28 × 10−12 J
⎜⎝ 1 MeV ⎟⎠

(b) N = 1.99 × 1030 kg = 1.19 × 1057 atoms = 1.19 × 1057 protons
1.67 × 10−27 kg atom

(c) The energy that could be created by this many protons in this reaction is:

( )1.19 × 1057 ⎛ 4.28 × 10−12 J⎞ = 1.27 × 1045
protons ⎝⎜ 4 protons ⎟⎠ J

P= E so ∆t = E = 1.27 × 1045 J = 3.31 × 1018 s = 105 billion years
3.85 × 1026 W
∆t P

P44.41 (a) 197 Au + 1 n → 198 Au* → 198 Hg + 0 e +ν
79 0 79 80 −1

(b) Consider adding 79 electrons:

197 Au atom + 1 n → 198 Hg atom +ν + Q
79 0 80

Q = ⎣⎡M 197 Au + mn − M 198 Hg ⎤⎦ c2

Q = [196.966 552 + 1.008 665 − 197.966 752] u(931.5 MeV u) = 7.89 MeV

P44.42 Neglect recoil of product nucleus (i.e., do not require momentum conservation for the system of
colliding particles). The energy balance gives Kemerging = Kincident + Q. To find Q:

Q = ⎡⎣(M H + M Al ) − (MSi + mn )⎦⎤ c2

Q = ⎡⎣(1.007 825 + 26.981 539) − (26.986 705 + 1.008 665)⎦⎤ u(931.5 MeV u) = −5.59 MeV

Thus, Kemerging = 6.61 MeV − 5.59 MeV = 1.02 MeV .

P44.43 9 Be + 1.665 MeV → 8 Be + 1 n, so M8 Be = M 9 Be − Q − mn
4 4 0 4 c2
4

M 8 Be = 9.012 182 u − (−1.665 MeV) − 1.008 665 u = 8.005 3 u
4
931.5 MeV u

9 Be + 1 n → 10 Be + 6.812 MeV, so M 10 Be = M 9 Be + mn − Q
4 0 4 4 c2
4

M 10 Be = 9.012 182 u + 1.008 665 u − 6.812 MeV = 10.013 5 u
931.5 MeV u
4

P44.44 (a) 10 B + 4 He → 13 C + 1 H
5 2 6 1

The product nucleus is 13 C .
6

(b) 13 C + 1 H → 10 B + 4 He
6 1 5 2

The product nucleus is 10 B .
5

556 Chapter 44

Section 44.8 Nuclear Magnetic Resonance and Magnetic Resonance Imagining

( )P44.45 (a)
2µB 2(1.913 5) 5.05 × 10−27 J T (1.00 T)
fn = h = = 29.2 MHz
6.626 × 10−34 J ⋅ s

(b) fp = )(2(2.792 8) 5.05 × 10−27 J T (1.00 T) = 42.6 MHz

6.626 × 10−34 J ⋅ s

(c) In the Earth’s magnetic field,

) )( (2(2.792 8) 5.05 × 10−27 50.0 × 10−6

fp = 6.626 × 10−34 = 2.13 kHz

P44.46

FIG. P44.46

Additional Problems

P44.47 (a) Q = ⎣⎡M 9 Be + M 4 He − M 12 C − mn ⎦⎤ c2

Q = [9.012 182 u + 4.002 603 u − 12.000 000 u − 1.008 665 u](931.5 MeV u) = 5.70 MeV

(b) Q = ⎣⎡2M 2 H − M 3He − mn ⎤⎦

Q = ⎣⎡2(2.014 102) − 3.016 029 − 1.008 665⎤⎦ u(931.5 MeV u) = 3.27 MeV (exothermic)

P44.48 (a) With mn and vn as the mass and speed of the neutrons, Equation 9.24 of the text becomes,

after making appropriate notational changes, for the two collisions v1 = ⎛ 2 mn ⎞ vn , and
⎝⎜ mn + m1 ⎠⎟

v2 = ⎛ 2mn ⎞ vn
⎜⎝ mn + m2 ⎠⎟

∴(mn + m2 )v2 = (mn + )m1 v1 = 2mnvn

( )∴ mn v2 − v1 = m1v1 − m2v2

∴ mn = m1v1 − m2v2
v2 − v1

(b) mn = (1 u)(3.30 × 107 m s) − (14 u)(4.70 × 106 m s) = 1.16 u

4.70 × 106 m s − 3.30 × 107 m s

Nuclear Structure 557

P44.49 (a) At threshold, the particles have no kinetic energy relative to each other. That is, they move
like two particles that have suffered a perfectly inelastic collision. Therefore, in order
to calculate the reaction threshold energy, we can use the results of a perfectly inelastic
collision. Initially, the projectile M a moves with velocity va while the target M X is at rest.
We have from momentum conservation for the projectile-target system:

( )M ava = M a + M X vc

The initial energy is: Ei = 1 M a va2
2

The final kinetic energy is:

( ) ( )Ef 1 vc2 = 1 ⎡ M ava ⎤2 ⎡ Ma ⎤
= 2 Ma + MX 2 Ma + MX ⎢ Ma + MX ⎥ = ⎢ Ma + MX ⎥ Ei
⎣ ⎦ ⎣ ⎦

From this, we see that Ef is always less than Ei and the change in energy, E f − Ei , is given by

Ef − Ei = ⎡ M M a − ⎤ Ei = − ⎡ M MX ⎤
⎢ a+ 1⎥ ⎢ a+M ⎥ Ei
⎣ M ⎦ ⎣ ⎦
X X

This loss of kinetic energy in the isolated system corresponds to an increase in mass-energy
during the reaction. Thus, the absolute value of this kinetic energy change is equal to −Q

(remember that Q is negative in an endothermic reaction). The initial kinetic energy Ei is
the threshold energy Eth.

Therefore, −Q = ⎡ MX ⎤ Eth
⎢ Ma + M ⎥
⎣ X ⎦

or Eth = −Q ⎡ M X +M a ⎤ = −Q ⎡ + Ma ⎤
⎢ MX ⎥ ⎢1 MX ⎥
⎣ ⎦ ⎣ ⎦

[ ](b) First, calculate the Q-value for the reaction: Q = M N-14 + M He-4 − MO-17 − M H-1 c2

Q = [14.003 074 + 4.002 603 − 16.999 132 − 1.007 825]u(931.5 MeV u) = −1.19 MeV

Then, Eth = −Q ⎡ M X +M a ⎤ = − (−1.19 MeV) ⎡⎣⎢1 + 4.002 603 ⎤ = 1.53 MeV .
⎢ MX ⎥ 14.003 074 ⎥⎦
⎣ ⎦

*P44.50 (a) The system of a separated proton and electron puts out energy 13.606 eV to become
a hydrogen atom in its ground state. This decrease in its rest energy appears also as a
decrease in mass: the mass is smaller .

∆m = E = 13.6 eV ⎛ 1.6 × 10−19 J⎞ = 2.42 × 10−35
c2 3 × 108 ms ⎜⎝ 1 eV ⎟⎠
( )(b) 2 kg

= 2.42 × 10−35 kg ⎛ 1.66 1u ⎞ = 1.46 × 10−8 u
⎜⎝ × 10−27 kg ⎟⎠

(c) 1.46 × 10−8 u = 1.45 × 10−8 = 1.45 × 10−6%
1.007 825 u

(d) The textbook table lists 1.007 825 u as the atomic mass of hydrogen. This correction of
0.000 000 01 u is on the order of 100 times too small to affect the values listed.

558 Chapter 44

*P44.51 The problem statement can be: Find the reaction energy (Q value) of the reaction

10 B + 4 He → 13 C + 1 H.
5 2 6 1
Solving gives Q = (14.015 54 − 14.011 18) u c2(931.5 MeV/u c2) = 4.06 MeV for the energy

released by the reaction as it is converted from rest energy into other forms.

N0 = mass = 1.00 kg = 2.52 × 1024
mass per atom 1.66 × 10−27
( )P44.52 (a) u)
(239.05 kg u

λ = ln 2 = ln 2 = 9.106 × 10−13 s−1
T1 2 2.412 × 104 yr 3.156 × 107
( )( )(b)
s yr

( )( )R0 = λ N0 = 9.106 × 10−13 s−1 2.52 × 1024 = 2.29 × 1012 Bq

(c) R= R0e−λ t , so t = −1 ln ⎛ R⎞ = 1 ln ⎜⎝⎛ R0 ⎠⎟⎞
λ ⎜⎝ R0 ⎠⎟ λ R

t = 1 s−1 ln ⎛ 2.29 × 1012 Bq ⎞ = 3.38 × 1013 s ⎝⎛⎜ 1 yr 7 s ⎠⎞⎟ = 1.07 × 106 yr
9.106 × 10−13 ⎜⎝ 0.100 Bq ⎟⎠ 3.156 × 10

P44.53 (a) 57 Co → 57 Fe + 0 e + 00ν
27 26 +1

The Q-value for this positron emission is Q = ⎣⎡M 57 Co − M 57 Fe − 2me ⎤⎦ c2 .

Q = ⎣⎡56.936 296 − 56.935 399 − 2(0.000 549)⎤⎦ u(931.5 MeV u) = −0.187 MeV

Since Q < 0, this reaction cannot spontaneously occur .

(b) 14 C → 14 N + 0 e + 00ν
6 7 −1

The Q-value for this e− decay is Q = ⎡⎣M 14 C − M 14 N ⎦⎤ c2 .

Q = [14.003 242 − 14.003 074]u(931.5 MeV u) = 0.156 MeV = 156 keV

Since Q > 0, the decay can spontaneously occur .

(c) The energy released in the reaction of (b) is shared by the electron and neutrino. Thus,
Ke can range from zero to 156 keV .

P44.54 (a) r = r0 A1 3 = 1.20 × 10−15 A1 3 m

When A = 12, r = 2.75 × 10−15 m

C2 (Z − 1) 1.60 × 10−19 C 2

r2
( ) ( )(b)
F = ke (Z − 1)e2 = 8.99 × 109 N ⋅ m2

r2

When Z = 6 and r = 2.75 × 10−15 m, F = 152 N

( ) ( )(c) U = keq1q2 = ke (Z − 1)e2 = 8.99 × 109 (Z − 1) 1.6 × 10−19 2
rr r

When Z = 6 and r = 2.75 × 10−15 m, U = 4.19 × 10−13 J = 2.62 MeV

(d) A = 238; Z = 92, r = 7.44 × 10−15 m F = 379 N
and U = 2.82 × 10−12 J = 17.6 MeV

Nuclear Structure 559

P44.55 (a) Because the reaction p → n + e+ + ν would violate the law of conservation of energy

mp = 1.007 276 u mn = 1.008 665 u me+ = 5.49 × 10−4 u
mn + me+ > mp
Note that

(b) The required energy can come from the electrostatic repulsion of protons in the parent

nucleus.

(c) Add seven electrons to both sides of the reaction for nuclei 13 N → 13 C + e+ +ν
7 6

to obtain the reaction for neutral atoms 13 N atom → 13 C atom + e+ + e− +ν
7 6

( ) ( )Q = c2 ⎡⎣m 13 N − m 13 C − me+ − me− − mν ⎤⎦

( )Q = (931.5 MeV u) ⎡⎣13.005 739 − 13.003 355 − 2 5.49 × 10−4 − 0⎤⎦ u

( )Q = (931.5 MeV u) 1.286 × 10−3 u = 1.20 MeV

P44.56 (a) A least-square fit to the graph yields:

( )λ = −slope = − −0.250 h−1 = 0.250 h−1

and

ln(cpm) = intercept = 8.30
t=0

(b) λ = 0.250 h−1 ⎜⎛⎝ 1 hmin ⎠⎟⎞ = 4.17 × 10−3 min−1
60.0

T1 2 = ln 2 = ln 2 min−1
λ 4.17 × 10−3

= 166 min = 2.77 h FIG. P44.56

(c) From (a), intercept = ln(cpm)0 = 8.30
Thus, (cpm)0 = e8.30 counts min = 4.02 × 103 counts min

N0 = R0 = 1 ( cpm )0 = 4.02 × 103 counts min = 9.65 × 106 atoms
λ λ 4.17 × 10−3
Eff min−1 (0.100)
( )(d)

P44.57 (a) One liter of milk contains this many 40 K nuclei:

N = (2.00 g ) ⎛ 6.02 × 1023 nuclei mol ⎞ ⎝⎜⎛ 0.011 7 ⎠⎞⎟ = 3.60 × 1018 nuclei
⎜⎝ 39.1 g mol ⎠⎟ 100

λ = ln 2 = ln 2 yr ⎛⎜⎝ 1 yr 7 s ⎟⎞⎠ = 1.72 × 10−17 s−1
T1 2 1.28 × 109 3.156 × 10

( )( )R = λ N = 1.72 × 10−17 s−1 3.60 × 1018 = 61.8 Bq

(b) For the iodine, R = R0e−λ t with λ = ln 2
8.04 d

t = 1 ln ⎛⎝⎜ R0 ⎟⎞⎠ = 8.04 d ln ⎛⎜⎝ 26010.80 ⎠⎞⎟ = 40.3 d
λ R ln 2

560 Chapter 44

P44.58 (a) If ∆E is the energy difference between the excited and ground states of the nucleus of mass
M, and hf is the energy of the emitted photon, conservation of energy for the
nucleus-photon system gives

∆E = hf + Er (1)

Where Er is the recoil energy of the nucleus, which can be expressed as

Er = M v2 = (M v)2 (2)
2
2M

Since system momentum must also be conserved, we have

M v = hf (3)
c

Hence, Er can be expresses as Er = (hf )2

When 2Mc2
we can make the approximation that
hf << Mc2

hf ≈ ∆E

so Er ≈ ( ∆E )2

2Mc2

(b) Er = ( ∆E )2 where ∆E = 0.014 4 MeV

2 Mc 2

and Mc2 = (57 u)(931.5 MeV u) = 5.31 × 104 MeV

Therefore, ( )1.44 × 10−2 MeV 2 1.94 × 10−3 eV
( )Er = 2 5.31 × 104 MeV =

P44.59 We have N = N e−λ235t
and 235 0,235

N = N e−λ238t
238 0,238

N235 = 0.007 25 = e(−(ln 2)t Th,235+(ln 2)t )Th, 238
N 238

Taking logarithms,

−4.93 = ⎛ − ln 2 yr + ln 2 yr ⎞ t
⎝⎜ 0.704 × 109 4.47 × 109 ⎠⎟

or −4.93 = ⎛ − 1 yr + 1 yr ⎞ (ln 2)t
⎜⎝ 0.704 × 109 4.47 × 109 ⎟⎠

−4.93 = 5.94 × 109 yr
−1.20 × 10−9 yr−1 ln 2
( )t =

Nuclear Structure 561

P44.60 (a) For cobalt-56,

λ = ln 2 = ln 2 ⎛ 365.25 d⎞ = 3.28 yr −1
T1 2 77.1 d ⎜⎝ 1 yr ⎟⎠

The elapsed time from July 1054 to July 2007 is 953 yr.

R = R0e−λ t

R )(= e = e = e =− 3.28 yr−1 (953 yr)
implies = e−λ t −3 129 −(ln10)1 359 ~10−1 359

R0

(b) For carbon-14,
λ = ln 2 = 1.21 × 10−4 yr−1
5 730 yr
( )R = e = e = e =−λ t − 1.21×10−4 yr−1 (953 yr) −0.115 0.891
R0

P44.61 E = −µ ⋅ B so the energies are E1 = +µB and E2 = −µB
µ = 2.792 8µn and µn = 5.05 × 10−27 J T

( )∆E = 2µB = 2(2.792 8) 5.05 × 10−27 J T (12.5 T) = 3.53 × 10−25 J = 2.20 × 10−6 eV

P44.62 R = R0 exp(−λ t ) lets us write ln R = ln R0 − λ t

which is the equation of a straight line with
slope = λ. The logarithmic plot shown in

Figure P44.62 is fitted by ln R = 8.44 − 0.262t.
If t is measured in minutes, then decay constant λ is
0.262 per minute. The half−life is

T1 2 = ln 2 = ln 2 = 2.64 min .
λ 0.262 min

The reported half−life of 137 Ba is 2.55 min. The
difference reflects experimental uncertainties.

FIG. P44.62

562 Chapter 44

( )K = 1 mv2 ,
2
P44.63 so v = 2K = 2(0.040 0 eV) 1.60 × 10−19 J eV = 2.77 × 103 ms
m
1.67 × 10−27 kg

The time for the trip is t = x = 1.00 × 104 m = 3.61 s.
v 2.77 × 103 m s

The number of neutrons finishing the trip is given by N = N0e−λt .

The fraction decaying is 1 − N = 1 − e−(ln2)t T1 2 = 1 − e−(ln2)(3.61 s 624 s) = 0.004 00 = 0.400% .
N0

P44.64 For an electric charge density ρ = (4 Ze R3 .

3)π

Using Gauss’s Law inside the sphere,

E ⋅ 4π r2 = (4 3)π r3 Ze : E = 1 Zer (r ≤ R)
4π ∈0 R3
∈0 (4 3)π R3

E = 1 Ze (r ≥ R)
4π ∈0 r2

We now find the electrostatic energy: ∫U = ∞ 1 ∈0 E2 4π r2dr
r=0 2

1 R⎛ 1 ⎞2 Z 2e2r2 4π r2dr + 1 ϱ⎛ 1 ⎞2 Z 2e2 4π r2dr Z 2e2 ⎡ R5 1⎤
2 0 ⎜⎝ 4π ∈0 ⎟⎠ R6 2 R ⎝⎜ 4π ∈0 ⎟⎠ r4 8π ∈0 ⎣⎢ 5R6 R ⎦⎥
∫ ∫U= ∈0 ∈0 = +

= 3 Z 2e2
20 π ∈0 R

P44.65 (a) If we assume all the 87Sr came from 87 Rb,

then N = N0e−λt

yields t = −1 ln ⎛ N ⎞ = T1 2 ln ⎜⎛⎝ N0 ⎟⎠⎞
λ ⎜⎝ N0 ⎟⎠ ln 2 N

where N = NRb-87

and N0 = NSr-87 + NRb-87

( )t =
4.75 × 1010 yr ln ⎛ 1.82 × 1010 + 1.07 × 109 ⎞ = 3.91 × 109 yr
ln 2 ⎝⎜ 1.82 × 1010 ⎠⎟

(b) It could be no older . The rock could be younger if some 87Sr were originally present.
We must make some assumption about the original quantity of radioactive material. In
part (a) we assumed that the rock originally contained no strontium.

Nuclear Structure 563

P44.66 (a) For the electron capture, 9433Tc + 0 e → 93 Mo + γ
−1 42

The disintegration energy is Q = ⎣⎡M 93Tc − M 93Mo ⎤⎦ c2 .

Q = [92.910 2 − 92.906 8]u(931.5 MeV u) = 3.17 MeV > 2.44 MeV

Electron capture is allowed to all specified excited states in 93 Mo.
42

For positron emission, 9433Tc → 93 Mo + 0 e +γ
42 +1

The disintegration energy is Q′ = ⎡⎣M 93Tc − M 93Mo − 2me ⎤⎦ c2 .

Q′ = ⎡⎣92.910 2 − 92.906 8 − 2(0.000 549)⎤⎦ u(931.5 MeV u) = 2.14 MeV

Positron emission can reach

the 1.35, 1.48, and 2.03 MeV states

but there is insufficient energy to reach
the 2.44 MeV state.

(b) The daughter nucleus in both forms of

decay is 93 Mo .
42

FIG. P44.66

ANSWERS TO EVEN PROBLEMS

P44.2 (a) 7.89 cm and 8.21 cm (b) See the solution.

P44.4 (a) 29.5 fm (b) 5.18 fm (c) See the solution.

P44.6 (a) 1.90 fm (b) 7.44 fm

P44.8 6.11 PN toward the other ball

P44.10 They agree with the figure.

P44.12 0.210 MeV greater for 23 Na because it has less proton repulsion

P44.14 (a) 84.1 MeV (b) 342 MeV (c) The nuclear force of attraction dominates over electrical
repulsion.

P44.16 RR
P44.18 (a) See the solution. (b) and ; see the solution.

36
(a) 491 MeV (b) 179%, −53.0%, −24.6%, −1.37%

P44.20 0.200 mCi

P44.22 See the solution.
P44.24
( )R T 2 − 20 1 2 −t1 T1 2
−t2 T1 2

ln 2

564 Chapter 44

P44.26 (a) See the solution. (b) See the solution. (c) See the solution;10.9 min.

(d) tm = ln (λ1 λ2 ) yes
λ2
λ1 − ;

P44.28 (a) 65 Ni* (b) 211 Pb (c) 55 Co (d) 0 e (e) 1 H
28 82 27 −1 1

P44.30 9.96 × 103 yr

P44.32 3 H atom → 3 He atom + ν ; 18.6 keV
1 2

P44.34 (a) cannot occur (b) cannot occur (c) can occur

P44.36 (a) 4.00 Gyr (b) 0.019 9 and 4.60
P44.38 (a) 0.281 (b) 1.65 × 10−29 (c) See the solution.

P44.40 (a) 4.28 pJ (b) 1.19 × 1057 atoms (c) 105 Gyr

P44.42 1.02 MeV

P44.44 (a) 13 C (b) 10 B
6 5

P44.46 See the solution.

P44.48 (a) See the solution. (b) 1.16 u

P44.50 (a) smaller (b) 1.46 × 10−8 u (c) 1.45 × 10−6 % (d) no

P44.52 (a) 2.52 × 1024 (b) 2.29 TBq (c) 1.07 Myr

P44.54 (a) 2.75 fm (b) 152 N (c) 2.62 MeV (d) 7.44 fm, 379 N, 17.6 MeV

P44.56 (a) See the solution. (b) 4.17 × 10−3 min−1; 2.77 h (c) 4.02 × 103 counts min
(d) 9.65 × 106 atoms

P44.58 (a) See the solution. (b) 1.94 meV
P44.60 (a) ~10−1 359 (b) 0.891

P44.62 2.64 min

P44.64 See the solution.

P44.66 (a) electron capture to all; positron emission to the 1.35 MeV, 1.48 MeV, and 2.03 MeV states

(b) 93 Mo; see the solution.
42

45

Applications of Nuclear Physics

CHAPTER OUTLINE ANSWERS TO QUESTIONS

45.1 Interactions Involving Neutrons Q45.1 The hydrogen nuclei in water molecules have mass
45.2 Nuclear Fission
45.3 Nuclear Reactors similar to that of a neutron, so that they can efficiently
45.4 Nuclear Fusion
45.5 Radiation Damage rob a fast-moving neutron of kinetic energy as they
45.6 Radiation Detectors
45.7 Uses of Radiation scatter it. Once the neutron is slowed down, a hydrogen

nucleus can absorb it in the reaction n+ 1 H → 2 H.
1 1

Q45.2 The excitation energy comes from the binding energy of
the extra nucleon.

*Q45.3 Answer (c). The function of the moderator is to slow
down the neutrons released by one fission so that they
can efficiently cause more fissions.

Q45.4 The advantage of a fission reaction is that it can generate much more electrical energy per
gram of fuel compared to fossil fuels. Also, fission reactors do not emit greenhouse gases as
combustion byproducts like fossil fuels—the only necessary environmental discharge is heat.
The cost involved in producing fissile material is comparable to the cost of pumping, transporting
and refining fossil fuel.

The disadvantage is that some of the products of a fission reaction are radioactive—and some
of those have long half-lives. The other problem is that there will be a point at which enough
fuel is spent that the fuel rods do not supply power economically and need to be replaced.
The fuel rods are still radioactive after removal. Both the waste and the “spent” fuel rods present
serious health and environmental hazards that can last for tens of thousands of years. Accidents
and sabotage involving nuclear reactors can be very serious, as can accidents and sabotage
involving fossil fuels.

*Q45.5 Answer (b). In m = E/c2 we estimate 5 × 1013 J/9 × 1016 m2/s2 ≈ 6 × 10–4 kg = 0.6 g.

*Q45.6 Answer (d). We compute 235 + 1 – 137 – 96 = 3. All the protons that start out in the uranium
nucleus end up in the fission product nuclei.

Q45.7 The products of fusion reactors are generally not themselves unstable, while fission reactions
result in a chain of reactions which almost all have some unstable products.

Q45.8 For the deuterium nuclei to fuse, they must be close enough to each other for the nuclear forces to
overcome the Coulomb repulsion of the protons—this is why the ion density is a factor. The more
time that the nuclei in a sample spend in close proximity, the more nuclei will fuse—hence the
confinement time is a factor.

Q45.9 Fusion of light nuclei to a heavier nucleus releases energy. Fission of a heavy nucleus to lighter
nuclei releases energy. Both processes are steps towards greater stability on the curve of binding
energy, Figure 44.5. The energy release per nucleon is typically greater for fusion, and this
process is harder to control.

565

566 Chapter 45

Q45.10 Advantages of fusion: high energy yield, no emission of greenhouse gases, fuel very easy to
obtain, reactor cannot go supercritical like a fission reactor, low amounts of radioactive waste.
Disadvantages: requires high energy input to sustain reaction, lithium and helium are scarce,
neutrons released by reaction cause structural damage to reactor housing.

*Q45.11 Answer Q1 > Q2 > Q3 > 0. Because all of the reactions involve 108 nucleons, we can look just at
the change in binding-energy-per-nucleon as shown on the curve of binding energy. The jump
from lithium to carbon is the biggest jump, and next the jump from A = 27 to A = 54, which is near
the peak of the curve. The step up for fission from A = 108 to A = 54 is smallest. Both of the fusion
reactions described and the fission reaction put out energy, so Q is positive for all. Imagine turning
the curve of binding energy upside down so that it bends down like a cross-section of a bathtub.
On such a curve of total energy per nucleon versus mass number it is easy to identify the fusion
of small nuclei, the fission of large nuclei, and even the alpha decay of uranium, as exoenergetic
processes. The most stable nucleus is at the drain of the bathtub, with minimum energy.

*Q45.12 Answer (d). The particles lose energy by collisions with nuclei in the bubble chamber to make
their speed and their cyclotron radii r = mv/qB decrease.

*Q45.13 Answer (d) only. The Geiger counter responds to an individual particle with a pulse whose size is
determined by the tube power supply.

Q45.14 For each additional dynode, a larger applied voltage is needed, and hence a larger output from
a power supply—“infinite” amplification would not be practical. Nor would it be desirable: the
goal is to connect the tube output to a simple counter, so a massive pulse amplitude is not needed.
If you made the detector sensitive to weaker and weaker signals, you would make it more and
more sensitive to background noise.

*Q45.15 Answer (b). The cyclotron radius is given by r = mv/qB = 2 1 m2v2 /qB = 2mK /qB. With the
2

same K, | q |, and B for both particles, the electron with much smaller mass has smaller radius and

is deflected more.

*Q45.16 Answer b > c > a > d. Dose (a) is 1 rem. Dose (b) is 10 rem. Doses (c) and (d) are 4 to 5 rem.
If we assume that (a) and (b) as well as (c) were whole-body doses to many kilograms of tissue,
we find the ranking stated.

Q45.17 Sometimes the references are indeed oblique. Some can serve for more than one form of energy
or mode of transfer. Here is one list:

kinetic: ocean currents
rotational kinetic: Earth turning
gravitational: water lifted up; you on the perilous bridge
elastic: Elastic energy is necessary for sound, listed below.
Vibrational energy could be separately exemplified by the swaying bridge of land.
internal: lava in and from infernal volcanoes; or in forging a chain
chemical: corrosive smoke
sound: thunder
electrical transmission: lightning
electromagnetic radiation: heavens blazing; lightning
atomic electronic: In the blazing heavens, stars have different colors because of different

predominant energy losses by atoms at their surfaces.
nuclear: The blaze of the heavens is produced by nuclear reactions in the cores of stars.

Remarkably, the word “energy” in this translation is an anachronism. Goethe wrote the song a
few years before Thomas Young coined the term.

Applications of Nuclear Physics 567

SOLUTIONS TO PROBLEMS

Section 45.1 Interactions Involving Neutrons

Section 45.2 Nuclear Fission

P45.1 The energy is

3.30 ×1010 J ⎝⎛⎜ 1.601×e1V0−19 J ⎠⎞⎟ ⎜⎝⎛1 U-235 nucleus ⎞⎠⎟ ⎝⎛⎜ 6.02 × 235 g ⎞⎟⎠ ⎝⎜⎛1M06 ⎠⎞⎟
208 MeV 1023 nucleus

= 0.387 g of U-235

P45.2 ) )( (∆m = mn + M U − M Zr + M Te + 3mn
∆m = (1.008 665 u + 235.043 923 u) − (97.912 7 u + 134.916 5 u + 3(1.008 665 u))

∆m = 0.197 39 u = 3.28 × 10−28 kg so Q = ∆mc2 = 2.95 × 10−11 J = 184 MeV

P45.3 Three different fission reactions are possible: 1 n + U235 → 90 Sr + 144 Xe + 2 1 n 144 Xe
0 38 54 0 54
92

1 n + U235 → 90 Sr + 143 Xe + 3 1 n 143 Xe 1 n + U235 → 90 Sr + 142 Xe + 4 1 n 142 Xe
0 38 54 0 54 0 38 54 0 54
92 92

P45.4 [ ](a) Q = (∆m) c2 = mn + M U235 − M Ba141 − M Kr92 − 3mn c2

P45.5 ∆m = ⎣⎡(1.008 665 + 235.043 923) − (140.914 4 + 91.926 2 + 3 × 1.008 665)⎦⎤ u = 0.185 993 u
P45.6 Q = (0.185 993 u)(931.5 MeV u) = 173 MeV

(b) f = ∆m = 0.185993 u = 7.88 × 10−4 = 0.078 8%
mi 236.05 u

1 n + 23920Th → 23930Th → 233 Pa + e− +ν 233 Pa → 233 U + e− +ν
0 91 91 92

(a) The initial mass is 1.007 825 u + 11.009 306 u = 12.017 131 u. The final mass is

3(4.002 603 u) = 12.007 809 u. The rest mass annihilated is ∆m = 0.009 322 u. The

energy created is Q = ∆mc2 = 0.009 322 u ⎛ 931.5 MeV ⎞ = 8.68 MeV .
⎝ 1 u ⎠

(b) The proton and the boron nucleus have positive charges. The colliding particles must have
enough kinetic energy to approach very closely in spite of their electric repulsion.

P45.7 The available energy to do work is 0.200 times the energy content of the fuel.

( ) ( ) ( )(1.00 ⎛ ⎞
kg fuel) 0.034 0 235 U fuel ⎛1 000 g ⎞ ⎛1 mol ⎞ 6.02 ×1023 mol ⎜⎜⎝ (208) 1.60 ×10−13 J ⎟⎠⎟
⎜ ⎟⎜ ⎟ fission
⎝ 1 kg ⎠ ⎝ 235 g ⎠

= 2.90 ×1012 J

( ) ( )2.90 ×1012 J (0.200) = 5.80 ×1011 J = 1.00 ×105 N ∆r

∆r = 5.80 ×106 m = 5.80 Mm

568 Chapter 45

P45.8 If the electrical power output of 1 000 MW is 40.0% of the power derived from fission reactions,
the power output of the fission process is

) )( (1 000 MW = 2.50 × 109 J s 8.64 × 104 s d = 2.16 × 1014 J d
0.400
The number of fissions per day is

( )2.16 × 1014 ⎛ 1 fission ⎞ ⎛ 1 eV ⎞ = × 1024 d−1
Jd ⎝ 200 × 106 eV ⎠ ⎝ 1.60 × 10−19 J⎠ 6.74

This also is the number of 235 U nuclei used, so the mass of 235 U used per day is

( )6.74 × 1024 d ⎛ 235 g mol ⎞ = 2.63 × 103 g d= 2.63 kg d
nuclei ⎜⎝ 6.02 × 1023 nuclei mol ⎠⎟

In contrast, a coal-burning steam plant producing the same electrical power uses more than
6 × 106 kg d of coal.

Section 45.3 Nuclear Reactors

( )Mass of ⎛ 106 g ⎞
P45.9 235 U available ≈ (0.007) 109 metric tons ⎜ ⎟ = 7 ×1012 g
⎝1 metric ton ⎠

⎛ 7× 1012 g ⎞
⎝⎜ 235 g mol ⎠⎟
( )number
of nuclei ≈ 6.02 × 1023 nuclei mol = 1.8 × 1034 nuclei

The energy available from fission (at 208 MeV/event) is

( ) ( )E ≈ 1.8 × 1034 events (208 MeV event) 1.60 × 10−13 J MeV = 6.0 × 1023 J

This would last for a time interval of

E 6.0 × 1023 J ⎛ 1 yr ⎞
7.0 × 1012 J s ⎝ 3.16 × 107 s⎠
( )∆tP
= ≈ = 8.6 × 1010 s ≈ 3 000 yr

V = 4 πr3 ⎛ 3V ⎞1 3 A 4π r2
3 ⎝ 4π ⎠ V
*P45.10 (a) For a sphere: and r = so = (4 3)πr3 = 4.84V −1 3

(b) For a cube: V= 3 and = V 1 3 so A = 6 2 = 6V −1 3
V 3

( )and 1 3
⎛ V ⎞ A= 2a2 + 8a2
(c) For a parallelepiped: V = 2a3 a = ⎝ 2 ⎠ so V 2a3 = 6.30V −1 3

(d) The answers show that the sphere has the smallest surface area for a given volume and the
brick has the greatest surface area of the three. Therefore, the sphere has the least leakage
and the parallelepiped has the greatest leakage .

Applications of Nuclear Physics 569

P45.11 In one minute there are 60.0 s = 5.00 ×104 fissions.
1.20 ms

So the rate increases by a factor of (1.000 )25 50 000 = 2.68 × 105 .

P45.12 P = 10.0 MW = 1.00 ×107 J s. If each decay delivers 1.00 MeV = 1.60 × 10−13 J, then the

number of decays/s = 107 J/s J = 6.25 × 1019 Bq .
1.6 × 10Ϫ13

*P45.13 (a) Since K = p2/2m, we have

p= 2mK = 2m 3 kBT = 3(1.67 ×10−27 kg)(1.38 ×10−23 J/K) 300 K
2

= 4.55 × 10–24 kg ⋅ m/s

(b) l = h/p = 6.63 × 10–34 J ⋅ s/4.55 × 10–24 kg ⋅ m/s = 0.146 nm . This size has the same order
of magnitude as an atom’s outer electron cloud, and is vastly larger than a nucleus.

*P45.14 We take the radii of the helium and gold nuclei as 1.20 fm 41/3 = 1.90 fm and 1.20 fm 1971/3 =
6.98 fm. The center to center distance is then 8.89 fm and the electric potential energy is

U = qV = keq1q2 = 8.99 ×109 N ⋅ m2 2 ×1.6 ×10−19 C 79 e = 25.6 MeV
r C2 8.89 ×10−15 m

Section 45.4 Nuclear Fusion

P45.15 (a) The Q value for the D-T reaction is 17.59 MeV.

Specific energy content in fuel for D-T reaction:

( )(17.59 MeV) 1.60 × 10−13 J MeV = 3.39 × 1014 J kg
( )(5 u) 1.66 × 10−27 kg u

(3.00 × 109 J s)(3 600 s hr)
( )( )rDT = 3.39 × 1014 J kg 10−3 kg g = 31.9 g h burning of D and T

(b) Specific energy content in fuel for D-D reaction: Q = 1 (3.27 + 4.03) = 3.65 MeV average
2
of two Q values

( )(3.65 MeV) 1.60 × 10−13 J MeV = 8.80 × 1013 J kg
( )(4 u) 1.66 × 10−27 kg u

(3.00 × 109 J s)(3 600 s hr)
( )( )rDD = 8.80 × 1013 J kg 10−3 kg g = 122 g h burning of D

570 Chapter 45

*P45.16 (a) We assume that the nuclei are stationary at closest approach, so that the electrostatic
(b) potential energy equals the total energy E.

Uf = ke (Z1e)(Z2e) =E

rmin

( )( ) ( )E =
8.99 × 109 N ⋅ m2 C2 1.6 × 10−19 C 2 Z1Z2 = 2.30 × 10−14 J Z1Z2 = (144 keV) Z1Z2
1.00 × 10−14 m

The energy is proportional to each atomic number.

(c) Take Z1 = 1 and Z2 = 59 or vice versa. This choice minimizes the product Z1 Z2. If extra
cleverness is allowed, take Z1 = 0 and Z2 = 60: use neutrons as the bombarding particles.
A neutron is a nucleon but not an atomic nucleus.

(d) For both the D-D and the D-T reactions, Z1 = Z2 = 1. Thus, the minimum energy required
in both cases is

( )E = ⎛ 1 MeV ⎞
2.30 × 10−14 J ⎝ 1.60 × 10−13 J⎠ = 144 keV

Section 45.4 in the text gives more accurate values for the critical ignition temperatures, of
about 52 keV for D-D fusion and 6 keV for D-T fusion. The nuclei can fuse by tunneling.
A triton moves more slowly than a deuteron at a given temperature. Then D-T collisions
last longer than D-D collisions and have much greater tunneling probabilities.

( )P45.17 (a) rf = rD + rT = 1.20 × 10−15 m ⎡⎣(2)1 3 + (3)1 3 ⎦⎤ = 3.24 × 10−15 m

( )( )(b) 2
kee2 8.99 ×109 N ⋅ m2 C2 1.60 ×10−19 C
Uf = rf = 3.24 ×10−15 m = 7.10 ×10−14 J= 444 keV

(c) Conserving momentum, mDvi = (mD + mT ) v f or vf = ⎛ mD ⎞ vi = 2 vi
⎜ mD + mT ⎟ 5
⎝ ⎠

(d) Ki +Ui = K f +U f : Ki + 0 = 1 (mD + )mT v2f +Uf = 1 (mD + mT ⎛ mD ⎞2 vi2 +Uf
2 2 mD + mT ⎟
)⎜ ⎠

⎝

K i + 0 = ⎛ mD ⎞ ⎛ 1 mD vi2 ⎞ + Uf = ⎛ mD ⎞ Ki +U f
⎜ mD + mT ⎟ ⎜⎝ 2 ⎟⎠ ⎜ mD + mT ⎟
⎝ ⎠ ⎝ ⎠

⎛ mD ⎞ K =Uf : Ki = Uf ⎛ mD + mT ⎞ 5 (444 keV) = 740 keV
⎜1 − mD + mT ⎟ ⎜ ⎟=
⎝ ⎠ i ⎝ mT ⎠ 3

(e) The nuclei can fuse by tunneling through the potential-energy barrier.

Applications of Nuclear Physics 571

( )P45.18 (a) ⎛ 1 609 m ⎞ 3 = 1.32 × 1018
V= 317 × 106 mi3 ⎝ 1 mi ⎠ m3

( )( )mwater = ρV = 103 kg m3 1.32 × 1018 m3 = 1.32 × 1021 kg

⎛ M H2 ⎞ ⎛ 2.016 ⎞
⎜⎝ M H2O ⎟⎠ ⎝ 18.015⎠
( )mH2 = 1.48 × 1020
= mH2O = 1.32 × 1021 kg kg

( )( ))(m =Deuterium 0.030 0% mH2 = 0.030 0 × 10−2 1.48 × 1020 kg = 4.43 × 1016 kg

The number of deuterium nuclei in this mass is

= mDeuterium = 4.43 × 1016 kg = 1.33 × 1043
mDeuteron
u) 1.66 × 10−27
( )N
(2.014 kg u

Since two deuterium nuclei are used per fusion, 2 H + 2 H → 4 He + Q / c2 , the number of
1 1 2

events is N = 6.63 × 1042.
2

The energy released per event is

Q = ⎣⎡M2H + M2H − M4 He ⎦⎤ c2 = ⎣⎡2(2.014 102) − 4.002 603⎤⎦ u(931.5 MeV u) = 23.8 MeV

The total energy available is then

( )E⎛ N ⎞ ) ⎛ 1.60 × 10−13 J⎞ 2.53 × 1031 J
= ⎝ 2 ⎠ Q = 6.63 × 1042 (23.8 MeV ⎝⎜ 1 MeV ⎟⎠ =

(b) The time this energy could possibly meet world requirements is

( )∆ t = E = 2.53×1031 J ⎛ 1 yr ⎞
( )P 100 7.00 ×1012 J s ⎝⎜ 3.16 ×10 s ⎟⎠
= 3.61 × 1016 s 7

= 1.14 ×109 yr ~ 1 billion years

P45.19 (a) Average KE per particle is 3 kBT = 1 mv2.
2 2

( ( )( ) )Therefore, vrms =
3kBT = 3 1.38 × 10−23 J K 4.00 × 108 K = 2.22 × 106 m s
m 2.014 1.661 × 10−27 kg

(b) t = x ~ 0.1 m = ~10−7 s
v 106 m s

572 Chapter 45

P45.20 (a) Including both ions and electrons, the number of particles in the plasma is N = 2nV where
n is the ion density and V is the volume of the container. Application of Equation 21.6 gives
the total energy as

E = 3 NkBT = 3nVkBT
2

⎡ ⎛ 106 cm3 ⎞ ⎤
( ) ( ) ( )( )= 3 ⎢
2.0 × 1013 cm −3 ⎣ 50 m3 ⎝⎜ 1 m3 ⎠⎟ ⎥ 1.38 × 10−23 JK 4.0 × 108 K
⎦

E = 1.7 × 107 J

(b) From Table 20.2, the heat of vaporization of water is Lv = 2.26 × 106 J kg. The mass of
water that could be boiled away is

m = E = 1.7 × 107 J = 7.3 kg
Lv 2.26 × 106 J kg

P45.21 (a) Lawson’s criterion for the D-T reaction is nτ ≥ 1014 s cm3. For a confinement time of
τ = 1.00 s, this requires a minimum ion density of n = 1014 cm−3 .

(b) At the ignition temperature of T = 4.5 × 107 K and the ion density found above, the plasma
pressure is

⎡ ⎛ 106 cm3 ⎞ ⎤
( ) ( )( )P = 2nkBT = 2⎢
1014 cm −3 ⎜⎝ 1 m3 ⎠⎟ ⎥ 1.38 × 10−23 JK 4.5 × 107 K
⎣ ⎦

= 1.24 × 105 J m3

(c) The required magnetic energy density is then

( )uB B2 = 1.24 × 106
= 2µ0 ≥ 10P = 10 1.24 × 105 J m3 J m3

( )( )B ≥ 2 4π × 10−7 N A2 1.24 × 106 J m3 = 1.77 T This is a very strong field.

P45.22 The number of nuclei in 1.00 metric ton of trash is

N = 1 000 kg(1 000 g kg) 6.02 × 1023 nuclei mol = 1.08 × 1028 nuclei

56.0 g mol

( ) ( )At an average charge of 26.0 e/nucleus, q = 1.08 × 1028 (26.0) 1.60 × 10−19 = 4.47 × 1010 C

Therefore t = q = 4.47 × 1010 = 4.47 × 104 s = 12.4 h
I 1.00 × 106

Applications of Nuclear Physics 573

Section 45.5 Radiation Damage

mass present 5.00 kg = 3.35 × 1025 nuclei
mass of nucleus
u) 1.66 × 10−27
( )P45.23N0 = =
(89.907 7 kg u

λ = ln 2 = ln 2 = 2.38 × 10−2 yr−1 = 4.53 × 10−8 min−1
T1 2 29.1 yr

( )( )R0 = λ N0 = 4.53 × 10−8 min−1 3.35 × 1025 = 1.52 × 1018 counts min

R = e−λ t = 10.0 counts min = 6.59 × 10−18
R0 1.52 × 1018 counts min

( )and λ t = − ln 6.59 × 10−18 = 39.6

giving t = 39.6 = 39.6 yr −1 = 1.66 × 103 yr
λ 2.38 × 10−2

P45.24 The source delivers 100 mrad of 2-MeV γ-rays/h at a 1.00-m distance.

(a) For γ-rays, dose in rem = dose in rad.
Thus a person would have to stand there 10.0 hours to receive 1.00 rem from a
100-mrad/h source.

(b) If the γ-radiation is emitted isotropically, the dosage rate falls off as 1
r2 .

Thus a dosage 10.0 mrad/h would be received at a distance r = 10.0 m = 3.16 m .

P45.25 (a) The number of x-ray images made per year is

n = (8 x-ray d)(5 d wk)(50 wk yr) = 2.0 × 103 x-ray yr

The average dose per photograph is 5.0 rem yr yr = 2.5 × 10−3 rem x-ray image
2.0 × 103 x-ray

(b) The technician receives low-level background radiation at a rate of 0.13 rem yr . The dose
of 5.0 rem yr received as a result of the job is

5.0 rem yr = 38 times the assumed background level . The technician’s occupational
0.13 rem yr

exposure is high compared to background radiation.

P45.26 (a) I = I0e−µ x , so x = 1 ln ⎛ I0 ⎞
µ ⎝ I ⎠

With µ = 1.59 cm−1, the thickness when I = I0 is x = 1 ln (2) = 0.436 cm .
2 1.59 cm−1

When I0 = 1.00 × 104 , 1
I 1.59 cm−1
( )(b)
x = ln 1.00 × 104 = 5.79 cm .

574 Chapter 45

P45.27 1 rad = 10−2 J kg Q = mc∆T P ∆ t = mc∆T

mc∆T m (4 186 J kg ⋅°C)(50.0°C) = 2.09 ×106 s ≈ 24 days!
(10) 10−2 J kg ⋅ s (m)
P
( )∆t= =

Note that power is the product of dose rate and mass.

P45.28 Q = absorbed energy = (1 000 rad) 10−2 J kg = 10.0 J kg
m unit mass 1 rad

The rise in body temperature is calculated from Q = mc∆T where c = 4 186 J kg for water and
the human body

∆T = Q = (10.0 J kg) 1 = 2.39 ×10−3°C The temperature change is

mc 4 186 J kg ⋅°C
negligible.

P45.29 If half of the 0.140-MeV gamma rays are absorbed by the patient, the total energy absorbed is

E = (0.140 MeV) ⎡⎛ 1.00 × 10−8 g⎞ ⎛ 6.02 × 1023 nuclei ⎞ ⎤ = 4.26 × 1012 MeV
⎢⎣⎜⎝ 98.9 g mol ⎠⎟ ⎝⎜ ⎠⎟ ⎥
2 1 mol ⎦

( )( )E = 4.26 × 1012 MeV 1.60 × 10−13 J MeV = 0.682 J

Thus, the dose received is Dose = 0.682 J ⎛ 1 rad ⎞ = 1.14 rad
60.0 kg ⎜⎝ 10−2 J kg⎠⎟

*P45.30 The decay constant is λ = ln 2 = ln 2 = 0.040 8 d . The number of nuclei remaining
T1 2 17 d

after 30 d is N = N 0 e− λT = N e−0.040 8(30) = 0.294N0 . The number decayed is
0

N0 − N = N0 (1 − 0.294) = 0.706N0 . Then the energy release is

( )2.12 J = 0.706N0 ⎛ 1.6 × 10−19 J⎞
21.0 × 103 eV ⎝⎜ 1 eV ⎟⎠

N0 = 2.12 J J = 8.94 × 1014
2.37 × 10−15

0.040 8 ⎛ 1d ⎞
d ⎜⎝ 86 400 s ⎟⎠
( )(a) 4.22 × 108 Bq
R0 = λN0 = 8.94 × 1014 =

(b) original sample mass = m = N moriginal one atom = 8.94 × 1014 (103 u ) ⎛ 1.66 × 10−27 kg ⎞
⎜⎝ 1u ⎟⎠

= 1.53 × 10−10 kg = 1.53 × 10−7 g = 153 ng

Applications of Nuclear Physics 575

( )P45.31 The nuclei initially absorbed are ⎛ 6.02 × 1023 nuclei mol ⎞
N0 = 1.00 × 10−9 g ⎝⎜ 89.9 g mol ⎠⎟ = 6.70 × 1012

( ) ( )The number of decays in time t is ∆N = N0 − N = N0 1 − e−λ t = N0 1 − e−(ln2)t T1 2

At the end of 1 year, t = 1.00 yr = 0.034 4
and T1 2 29.1 yr

( )( )∆N = N0 − N = 6.70 × 1012 1 − e−0.023 8 = 1.58 × 1011

The energy deposited is ) )( (E = 1.58 × 1011 (1.10 MeV) 1.60 × 10−13 J MeV = 0.027 7 J

Thus, the dose received is Dose = ⎛ 0.027 7 J⎞ = 3.96 × 10−4 J kg = 0.039 6 rad
⎝⎜ 70.0 kg ⎠⎟

Section 45.6 Radiation Detectors

P45.32 (a) EI = 10.0 eV is the energy required to liberate an electron from a dynode. Let ni be the

number of electrons incident upon a dynode, each having gained energy e(∆V ) as it was

accelerated to this dynode. The number of electrons that will be freed from this dynode is

Ni = ni e ∆V :
EI
(1)e(100 V)
At the first dynode, ni = 1 and N1 = = 101 electrons
10.0 eV

(b) For the second dynode, ni = N1 = 101, so N2 = (101 )e (100 V) = 102

10.0 eV

At the third dynode, ni = N2 = 102 and N3 = (102 )e(100 V) = 103

10.0 eV

Observing the developing pattern, we see that the number of electrons incident on the

seventh and last dynode is n7 = N6 = 106 .

(c) The number of electrons incident on the last dynode is n7 = 106. The total energy these
electrons deliver to that dynode is given by

E = nie(∆V ) = 106 e(700 V − 600 V) = 108 eV

576 Chapter 45

) )( (E
)(Eβ
P45.33 (a) = (1 2)C (∆V )2 = (1 2) 5.00 × 10−12 F 1.00 × 103 V 2 = 3.12 × 107
(b)
0.500 MeV (0.500 MeV) 1.60 × 10−13 J MeV

( )( )N = Q = C (∆V ) =
ee
5.00 × 10−12 F 1.00 × 103 V = 3.12 × 1010 electrons
1.60 × 10−19 C

P45.34 (a) The average time between slams is 60 min 38 = 1.6 min. Sometimes, the actual interval
is nearly zero. Perhaps about equally as often, it is 2 × 1.6 min. Perhaps about half as often,
it is 4 × 1.6 min. Somewhere around 5 × 1.6 min = 8.0 min , the chances of randomness

producing so long a wait get slim, so such a long delay might likely be due to mischief.

(b) The midpoints of the time intervals are separated by 5.00 minutes. We use R = R0e−λt.
Subtracting the background counts,

[ ]337 − 5(15) = 372 − 5(15) e ( )− ln 2 T1 2 (5.00 min)

or ln ⎛ 262 ⎞ = ln (0.882) = − 3.47 min T1 2 which yields T1 2 = 27.6 min
⎝ 297 ⎠

(c) As in the random events in part (a), we imagine a ±5 count counting uncertainty. The
smallest likely value for the half-life is then given by

( )⎛ 262 − 5 ⎞
297 + 5 ⎟⎠
ln ⎝⎜
= − 3.47 min T1 2, or T1 2 min = 21.1 min

The largest credible value is found from

( )ln⎛ 262 + 5⎞
⎝ 297 − 5⎠ = − 3.47 min T1 2, yielding T1 2 max = 38.8 min

Thus, T1 2 = ⎛ 38.8 + 21.1⎞ ± ⎛ 38.8 − 21.1⎞ min = (30 ± 9) min = 30 min ± 30%
⎝ 2 ⎠ ⎝ 2 ⎠

Section 45.7 Uses of Radiation

P45.35 The initial specific activity of 59 Fe in the steel,

(R m)0 = 20.0 µCi = 100 µCi ⎛ 3.70 × 104 Bq ⎞ = 3.70 × 106 Bq kg
0.200 kg kg ⎝⎜ 1 µCi ⎠⎟

( )R ⎛ R⎞ e−λ t e (− 6.40×10−4 )h−1 (1 000 h) = 1.95 × 106
⎝ m⎠0
m
After 1 000 h, = = 3.70 × 106 Bq kg Bq kg

The activity of the oil is Roil = ⎛ 800 Bq liter⎞⎠ (6.50 liters) = 86.7 Bq
⎝ 60.0

Therefore min oil = Roil = 86.7 Bq kg = 4.45 × 10−5 kg
1.95 × 106 Bq
(R m)

So that wear rate is 4.45 × 10−5 kg = 4.45 × 10−8 kg h
1 000 h

Applications of Nuclear Physics 577

P45.36 (a) The number of photons is 104 MeV = 9.62 × 103. Since only 50% of the photons are
1.04 MeV

detected, the number of 65 Cu nuclei decaying is twice this value, or 1.92 × 104. In two

half-lives, three-fourths of the original nuclei decay, so 3 N0 = 1.92 × 104 and
4

N0 = 2.56 × 104. This is 1% of the 65 Cu, so the number of 65 Cu is 2.56 ×106 ~ 106 .

(b) Natural copper is 69.17% 63 Cu and 30.83% 63 Cu . Thus, if the sample contains NCu
copper atoms, the number of atoms of each isotope is

N63 = 0.691 7NCu and N65 = 0.308 3NCu

N63 0.691 7 ⎛ 0.6917 ⎞ ⎛ 0.6917 ⎞
N65 0.308 3 ⎝ 0.3083⎠ ⎝ 0.3083⎠
( )Therefore, = 5.75 × 106.
= or N63 = N65 = 2.56 × 106

The total mass of copper present is then mCu = (62.93 u) N63 + (64.93 u) N65 :

( ) ( ) ( )mCu = ⎣⎡(62.93) 5.75 ×106 + (64.93) 2.56 ×106 ⎤⎦u 1.66 ×10−24 g u

= 8.77 ×10−16 g ~ 10−15 g

P45.37 (a) Starting with N = 0 radioactive atoms at t = 0, the rate of increase is (production – decay)

dN = R − λ N so dN = (R − λ N ) dt
dt
The variables are separable.

∫ ∫N dN t − 1 ln ⎛ R −λ N ⎞ = t
λ ⎜⎝ R ⎠⎟
= dt:
0 R−λN 0

so ln ⎛ R − λN ⎞ = −λ t and ⎛ R − λN ⎞ = e−λ t
⎝⎜ R ⎟⎠ ⎝⎜ R ⎠⎟

Therefore 1 − λ N = e−λ t ( )N = R 1 − e−λt
R λ

R
(b) The maximum number of radioactive nuclei would be .

λ

578 Chapter 45

*P45.38 (a) With I (x) = 1 I0 , I (x) = I0e−µx becomes
2

1 I0 = I 0 e−0.72x mm 2 = e+0.72x mm
2 x = ln 2 mm = 0.963 mm

ln 2 = 0.72 x mm 0.72

(b) I (0.8 mm) = I e−0.72(0.8) = 0.562I0
0

I (0.7 mm) = I e−0.72(0.7) = 0.604 I 0
0

fractional change = 0.604I0 − 0.562I0 = 0.074 7 = 7.47%
0.562I0

Additional Problems

P45.39 (a) At 6 × 108 K, the average kinetic energy of a carbon atom is

) )( (3

2 kBT
= (1.5) 8.62 × 10−5 eV K 6 × 108 K = 8 × 104 eV

Note that 6 × 108 K is about 62 = 36 times larger than 1.5 × 107 K, the core temperature
of the Sun. This factor corresponds to the higher potential-energy barrier to carbon fusion

compared to hydrogen fusion. It could be misleading to compare it to the temperature
~108 K required for fusion in a low-density plasma in a fusion reactor.

(b) The energy released is

) ) )( ( (E = ⎣⎡2m C12 − m Ne20 − m He4 ⎦⎤ c2

E = (24.000 000 − 19.992 440 − 4.002 603)(931.5) MeV = 4.62 MeV

In the second reaction,

) )( (E = ⎣⎡2m C12 − m Mg24 ⎦⎤ (931.5) MeV u

E = (24.000 000 − 23.985 042)(931.5) MeV = 13.9 MeV

(c) The energy released is the energy of reaction of the number of carbon nuclei in a 2.00-kg
sample, which corresponds to

( )∆E = ⎛ 6.02 × 1023 atoms mol ⎞ ⎛ 4.62 MeV fusion event ⎞ ⎛ 1 kWh ⎞
2.00 ×103 g ⎜ ⎟ ⎜ 2 nuclei fusion event ⎟ ⎜⎝ × 1019 MeV ⎠⎟
⎝ 12.0 g mol ⎠ ⎝ ⎠ 2.25

( )∆E = (4.62)
1.00 ×1026 1.03×107 kWh
kWh =
( )2 2.25 ×1019

Applications of Nuclear Physics 579

P45.40 To conserve momentum, the two fragments must move in opposite directions with speeds v1and
v2 such that

m1v1 = m2v2 or v2 = ⎛ m1 ⎞ v1
⎜⎝ m2 ⎟⎠

The kinetic energies after the break-up are then

⎛ m1 ⎞ 2 ⎛ m1 ⎞
⎜⎝ m2 ⎠⎟ ⎜⎝ m2 ⎟⎠
K1 = 1 m1v12 and K2 = 1 m2 v22 = 1 m2 v12 = K1
2 2 2

The fraction of the total kinetic energy carried off by m1 is

( )K1 = K1 = m2

K1 + K2 K1 + m1 m2 K1 m1 + m2

and the fraction carried off by m2 is 1− m2 = m1 .
m1 + m2 m1 + m2

P45.41 (a) Q = 236.045 562u c2 − 86.920 711u c2 −148.934 370u c2 = 0.190 481u c2 = 177 MeV
Immediately after fission, this Q-value is the total kinetic energy of the fission products.

(b) K Br ⎛ mLa ⎞ from Problem 45.40
=⎜ ⎟Q,
⎝ mBr + mLa ⎠

= ⎛ 87 149 u u ⎞ (177.4 MeV) = 112 MeV
⎝⎜ u +149 ⎠⎟

KLa = Q − KBr = 177.4 MeV − 112.0 MeV = 65.4 MeV

( ( )( ) )(c)
vBr = 2KBr = 2 112 ×106 eV 1.6 ×10−19 J eV
mBr = 1.58 ×107 m s

(87 u) 1.66 ×10−27 kg u

( ( )( ) )vLa =
2KLa = 2 65.4 ×106 eV 1.6 ×10−19 J eV = 9.20 ×106 m s
mLa
(149 u) 1.66 ×10−27 kg u

P45.42 For a typical 235 U fission, Q = 208 MeV and the initial mass is 235 u. Thus, the fractional
energy loss is

Q = (235 208 MeV u) = 9.50 × 10−4 = 0.095 0%
mc2
u)(931.5 MeV

For the D-T fusion reaction, Q = 17.6 MeV

The initial mass is m = (2.014 u) + (3.016 u) = 5.03 u

The fractional loss in this reaction is Q = (5.03 17.6 MeV u) = 3.75 × 10−3 = 0.375%
mc2
u) (931.5 MeV

0.375% = 3.95 or the fractional loss in D-T fusion is about 4 times that in 235 U fission .
0.0950%

580 Chapter 45

P45.43 ( )The decay constant is λ = ln 2 = ln 2 = 1.78 ×10−9 s−1.

T1 2 (12.3 yr) 3.16 ×107 s yr

The tritium in the plasma decays at a rate of

⎡⎛ 2.00 ×1014 ⎞ ⎛106 cm3 ⎞ ⎤
( ) ( )R = λ N = m3 ⎥
1.78 ×10−9 s−1 ⎢⎣⎜⎝ cm 3 ⎟⎜ 1 m3 ⎟ 50.0 ⎦
⎠⎝ ⎠

( )R = 1.78 × 1013 ⎛ 1 Ci ⎞
Bq = 1.78 × 1013 Bq ⎝⎜ 3.70 × 1010 Bq ⎠⎟ = 482 Ci

The fission inventory is 4 × 1010 Ci ~ 108 times greater than this amount.
482 Ci

5 × 106 Ci ⎛ 1 km ⎞ 2
104 km2 ⎝ 103 m ⎠
*P45.44 The original activity per area is = 5 × 10−4 Ci/m2.

The decay constant is l = ln 2/27.7 yr.

The decay law N = N0 e–lt becomes the law of doef carcetaivseityofpaecrtaivreitayRR/A==R0Re0/–Alt.eI–fltt.hSeomlvaitnegrigailviess
not transported, it describes the time evolution

eλt = R0 /A λt = ln ⎛ R0 /A ⎞ = ln 2 t
R/A ⎜ ⎟
⎝ R/A ⎠ 27.7 yr

t = 27.7 yr ln ⎛ R0 /A ⎞ = 27.7 yr ln ⎛ 5 × 10−4 Ci/m2 ⎞ = 221 yr
ln 2 ⎜ ⎟ ln 2 ⎜ 2 × 10−6 Ci/m2 ⎟
⎝ R/A ⎠ ⎝ ⎠

P45.45 The complete fissioning of 1.00 gram of U235 releases

) )( (Q = (1.00 g) 6.02 × 1023 atoms mol (200 MeV fission) 1.60 × 10−13 J MeV
235 grams mol
= 8.20 × 1010 J

If all this energy could be utilized to convert m kilograms of 20.0°C water to 400°C steam (see
Chapter 20 of text for values),

then Q = mcw ∆T + mLv + mcs ∆T

Q = m⎣⎡(4186 J kg °C)(80.0 °C) + 2.26 ×106 J kg + (2010 J kg °C)(300 °C)⎤⎦

Therefore m = 8.20 × 1010 J = 2.56 × 104 kg
3.20 × 106 J kg

Applications of Nuclear Physics 581

P45.46 When mass m of 235 U undergoes complete fission, releasing 200 MeV per fission event, the total
energy released is:

⎛ m ⎞ N (200 MeV) where NA is Avogadro’s number.
Q=⎜ g ⎟
mol ⎠ A
⎝ 235

If all this energy could be utilized to convert a mass mw of liquid water at Tc into steam at Th,

then Q = m w ⎣⎡cw (100°C − Tc ) + L v + c s (Th −100°C)⎦⎤

where cw is the specific heat of liquid water, Lv is the latent heat of vaporization, and c s is the
specific heat of steam. Solving for the mass of water converted gives

mw = ⎡⎣c w Q + c s (Th − 100°C)⎤⎦

(100°C − Tc ) + L v

= mNA (200 MeV) .
(235 g mol)⎡⎣cw (100°C − Tc ) + Lv + cs (Th −100°C)⎦⎤

*P45.47 (a) We have 0.9928 kg of 238U, comprising

N = 0.9928 kg (6.02 × 1023 atoms/mol)/(0.238 kg/mol) = 2.51 × 1024 nuclei, with activity

R = λ N = (ln 2/T1/2)N = 2.51 × 1024 (ln 2/4.47 × 109 yr)(1 yr/3.16 × 107 s)(1 Ci/3.7 × 1010/s)
= 333 µCi

We have 0.0072 kg of 235U, comprising

N = 0.0072 kg (6.02 × 1023 atoms/mol)/(0.235 kg/mol) = 1.84 × 1022 nuclei, with activity
R = λN = (ln 2/T1/2)N = 1.84 × 1022 (ln 2/7.04 × 108 yr)(1 yr/3.16 × 107 s)(1 Ci/3.7 × 1010/s)

= 15.5 µCi

We have 0.00005 kg of 234U, comprising

N = 5 × 10–5 kg (6.02 × 1023 atoms/mol)/(0.23404 kg/mol) = 1.29 × 1020 nuclei, with activity

R= λN = (ln 2/T1/2)N = 1.29 × 1020 (ln 2/2.44 × 105 yr)(1 yr/3.16 × 107 s)(1 Ci/3.7 × 1010/s)
= 312 µ Ci

(b) The total activity is (333 + 15.5 + 312) µCi = 661 µCi, so the fractional contributions are
respectively 333/661 = 50.4% 15.5/661 = 2.35% and 312/661 = 47.3%

(c) It is potentially dangerous, notably if the material is inhaled as a powder. With precautions
to minimize human contact, microcurie sources are routinely used in laboratories.

( )P45.48 (a) ∆V = 4πr2∆ r = 4π 14.0 ×103 m 2 (0.05 m) = 1.23×108 m3 ~108 m3

(b) The force on the next layer is determined by atmospheric pressure.

( )( )W = P∆V = 1.013×105 N/m2 1.23×108 m3 = 1.25 ×1013 J ~1013 J

(c) 1.25 ×1013 J = 1 (yield), so yield = 1.25 ×1014 J ~1014 J

10

(d) 1.25 × 1014 J = 2.97 × 10 4 ton TNT ~ 104 ton TNT
× 10 9 J ton TNT
4.2

or ~ 10 kilotons

582 Chapter 45

P45.49 (a) The number of molecules in 1.00 liter of water (mass = 1 000 g) is

⎛1.00 ×103 g ⎞
⎜ ⎟
( )N =
⎝ 18.0 g mol ⎠ 6.02 ×1023 molecules mol = 3.34 ×1025 molecules.

The number of deuterium nuclei contained in these molecules is

( )N′ = ⎛ 1 deuteron ⎞
3.34 ×1025 molecules ⎜⎝ 3300 molecules ⎠⎟ = 1.01 × 10 22 deuterons.

Since 2 deuterons are consumed per fusion event, the number of events possible is

N ′ = 5.07 ×1021 reactions, and the energy released is
2

( )Efusion = 5.07 ×1021 reactions (3.27 MeV reaction) = 1.66 ×1022 MeV

( )( )Efusion = 1.66 ×1022 MeV 1.60 ×10−13 J MeV = 2.65 ×109 J .

(b) In comparison to burning 1.00 liter of gasoline, the energy from the fusion of deuterium is

Efusion = 2.65 ×109 J = 78.0 times larger .
Egasoline 3.40 ×107 J

P45.50 Momentum conservation: 0 = mLivLi + mαvα or mLivLi = mαvα

mLivLi 2 = 2
mLi
( ) ( )KLi ⎛ mα2 ⎞
Thus, = 1 mLi vL2 i = 1 mα vα = ⎜ 2 mLi ⎟ vα2
2 2 2 mLi ⎝ ⎠

⎛ (4.002 6 u) 2 ⎞
⎜⎜⎝ 2 (7.016 0 u) ⎠⎟⎟
K Li = ⎛ 9.25 × 10 6 m s⎞2 = (1.14 u) ⎛ 9.25 × 10 6 m s⎞2
⎜⎝ ⎟⎠ ⎜⎝ ⎠⎟

( )KLi = 1.14 1.66 ×10−27 kg ⎛ 9.25 × 106 m s⎞ 2 = 1.62 × 10−13 J= 1.01 MeV .
⎝⎜ ⎟⎠

P45.51 (a) The thermal power transferred to the water is Pw = 0.970 (waste heat)

Pw = 0.970 (3 065 −1 000) MW = 2.00 ×109 J s

rw is the mass of water heated per hour:

)rw
= Pw ) = (2.00 × 109 J s (3600 s h) = 4.91 × 108 kg h
c ( ∆T
(4186 J kg ⋅°C)(3.50 °C)

The volume used per hour is 4.91 × 108 kg h = 4.91 × 105 m3 h
1.00 × 103 kg m3

(b) The 235 U fuel is consumed at a rate

rf = ⎛ 3 065 × 106 J s⎞ ⎛ 1 kg ⎞ ⎛ 3 600 s⎞ = 0.141 kg h
⎜⎝ 7.80 × 1010 J g⎟⎠ ⎜⎝ 1 000 g⎟⎠ ⎝ 1h ⎠

Applications of Nuclear Physics 583

P45.52 The number of nuclei in 0.155 kg of 210 Po is

⎛ 155 g ⎞
⎝⎜ 209.98 g mol ⎠⎟
( )N0 = 4.44 × 1023 nuclei
= 6.02 × 1023 nuclei mol

The half-life of 210 Po is 138.38 days, so the decay constant is given by

( )λ= ln 2 = d) ln 2 = 5.80 × 10−8 s−1
T1 2 (138.38 8.64 × 104 sd

The initial activity is

( )( )R0 = λ N0 = 5.80 × 10−8 s−1 4.44 × 1023 nuclei = 2.58 × 1016 Bq

The energy released in each 210 Po → 206 Pb + 4 He reaction is
84 82 2

Q = ⎣⎡M − M − M ⎦⎤ c 2 :

210 Po 206 Pb 4 He
84 82 2

Q = [209.982 857 − 205.974 449 − 4.002 603]u(931.5 MeV u) = 5.41 MeV

Thus, assuming a conversion efficiency of 1.00%, the initial power output of the battery is

) )P = (0.010 0) R0Q = (0.010 0)(2.58 × 1016 decays s (5.41 MeV (decay) 1.60 × 10−13 J MeV

= 223 W

V = 3 = m , so ⎛m⎞1 3 ⎛ 70.0 kg ⎞1 3
ρ ⎝⎜18.7 × 103 kg
P45.53 (a) = ⎜ ρ ⎟ = m 3 ⎟ = 0.155 m
⎝ ⎠ ⎠

(b) Add 92 electrons to both sides of the given nuclear reaction. Then it becomes

U238 atom → 8 4 He atom + 206 Pb atom + Qnet /c2
2 82
92

Qnet = ⎡ M 238 − 8 M − M ⎤ c206 2
⎣ 92 ⎦82
U 4 He Pb
2

= ⎡⎣238.050 783− 8(4.002 603)− 205.974 449⎦⎤ u (931.5 MeV u)

Qnet = 51.7 MeV

(c) If there is a single step of decay, the number of decays per time is the decay rate R and the

energy released in each decay is Q. Then the energy released per time is P = QR . If

there is a series of decays in steady state, the equation is still true, with Q representing the
net decay energy.

(d) The decay rate for all steps in the radioactive series in steady state is set by the parent
uranium:

⎛ 7.00 × 104 g ⎞
( )N = 1.77 × 1026
= ⎜ 238 g mol ⎟ 6.02 × 1023 nuclei mol nuclei
⎝ ⎠

λ = ln 2 = ln 2 yr = 1.55 × 10−10 1
T1 2 4.47 × 109 yr

⎛ 1⎞
⎜⎝1.55 yr ⎠⎟
( )R
= λ N = × 10−10 1.77 × 1026 nuclei = 2.75 × 1016 decays yr

( )so ⎛ 1 ⎞
P = QR = (51.7 MeV) ⎜ 2 .75 × 1016 ⎟ 1.60 × 10−13 J MeV = 2.27 ×105 J yr
⎝ yr ⎠

continued on next page

584 Chapter 45

(e) dose in rem = dose in rad × RBE

5.00 rem yr = (dose in rad yr)1.10, giving (dose in rad yr) = 4.55 rad yr

The allowed whole-body dose is then (70.0 kg)(4.55 rad yr ) ⎛10−2 J kg ⎞ = 3.18 J yr .
⎜ ⎟
⎝ 1 rad ⎠

P45.54 ET ≡ E (thermal) = 3 kBT = 0.039 eV
2

= ⎛⎜ 1 ⎞⎟ n E ⎛ 1 ⎞ n
⎝2⎠ ⎝ 2 ⎠
( )ET
where n ≡ number of collisions, and 0.039 = 2.0 × 106

Therefore n = 25.6 = 26 collisions

P45.55 Conservation of linear momentum and energy can be applied to find the kinetic energy of the
neutron. We first suppose the particles are moving nonrelativistically.
The momentum of the alpha particle and that of the neutron must add to zero, so their velocities
must be in opposite directions with magnitudes related by

mnvn + mα vα = 0 or (1.008 7 u) vn = (4.002 6 u) vα

At the same time, their kinetic energies must add to 17.6 MeV

E = 1 mn vn2 + 1 mα vα2 = 1 (1.008 7 u) vn2 + 1 ( 4.002 6) vα2 = 17.6 MeV
2 2 2
2

Substitute vα = 0.252 0vn: E = (0.504 35 u) vn2 + (0.127 10 u) vn2 = 17.6 ⎛ 1 u ⎞
MeV⎜ MeV ⎟
⎝ 931.494 c2 ⎠

vn = 0.018 9c2 = 0.173c = 5.19 × 107 m s
0.631 45

Since this speed is not too much greater than 0.1c, we can get a reasonable estimate of the kinetic
energy of the neutron from the classical equation,

K = 1 mv2 = 1 (1.008 7 u)(0.173c)2 ⎛ 931.494 MeV c2 ⎞ = 14.1 MeV
2 2 ⎝⎜ u ⎠⎟

For a more accurate calculation of the kinetic energy, we should use relativistic expressions.
Conservation of momentum gives

γ n mnvn + γ α mα vα = 0 1.008 7 vn = 4.002 6 vα
yielding 1 − vn2 c2 1 − vα2 c2
Then
vα2 = 15.746c2 vn2
c2 − 14.746vn2

(γ n − 1) mnc2 + (γ α )− 1 mα c2 = 17.6 MeV

and vn = 0.171c implying that (γ n − 1) mnc2 = 14.0 MeV

Applications of Nuclear Physics 585

P45.56 From the table of isotopic masses in Chapter 44, the half-life of 32 P is 14.26 d. Thus, the decay
constant is

λ = ln 2 = ln 2 = 0.048 6 d−1 = 5.63 × 10−7 s−1
T1 2 14.26 d

N0 = R0 = 5.22 × 106 decay s = 9.28 × 1012 nuclei
λ 5.63 × 10−7 s−1

At t = 10.0 days, the number remaining is

( )N = N0 e−λ t = 9.28 × 1012 nuclei e ( )− 0.048 6 d−1 (10.0 d) = 5.71 × 1012 nuclei

so the number of decays has been N0 − N = 3.57 × 1012 and the energy released is

) )( (E = 3.57 × 1012 (700 keV) 1.60 × 10−16 J keV = 0.400 J

If this energy is absorbed by 100 g of tissue, the absorbed dose is

Dose = ⎛ 0.400 J ⎞ ⎛ 1 rad ⎞ = 400 rad
⎜⎝ 0.100 kg⎟⎠ ⎜⎝ 10−2 J kg⎠⎟

P45.57 (a) The number of Pu nuclei in 1.00 kg = 6.02 × 1023 nuclei mol (1 000 g).

239.05 g mol

( )The total energy = 25.2 × 1023 nuclei (200 MeV) = 5.04 × 1026 MeV
( )( )E = 5.04 × 1026 MeV 4.44 × 10−20 kWh MeV = 2.24 × 107 kWh

or 22 million kWh

(b) E = ∆m c2 = (3.016 049 u + 2.014 102 u − 4.002 603 u − 1.008 665 u)(931.5 MeV u)

E = 17.6 MeV for each D-T fusion

( )(c) En = (Total number of D nuclei)(17.6) 4.44 × 10−20

⎛⎜ 1 000 ⎟⎞ (17.6) 4.44 × 10−20

⎝ 2.014 ⎠
( ) ( )En = 2.34 × 108 kWh
6.02 × 1023 =

(d) En = the number of C atoms in 1.00 kg × 4.20 eV

⎛6.02 × 1026 ⎞
⎜ ⎟
⎝ 12 ⎠
( )( )En
= 4.20 × 10−6 MeV 4.44 × 10−20 = 9.36 kWh

(e) Coal is cheap at this moment in human history. We hope that safety and waste disposal
problems can be solved so that nuclear energy can be affordable before scarcity drives
up the price of fossil fuels. Burning coal in the open puts carbon dioxide into the
atmosphere, worsening global warming. Plutonium is a very dangerous material to have
sitting around.

586 Chapter 45

P45.58 Add two electrons to both sides of the given reaction.

Then 4 1 H atom → 4 He atom + Q/ c2
1 2

where Q = (∆m)c2 = ⎡⎣4(1.007 825) − 4.002 603⎤⎦ u(931.5 MeV u) = 26.7 MeV
or
( )Q = (26.7 MeV) 1.60 × 10−13 J MeV = 4.28 × 10−12 J

The proton fusion rate is then

3.85 × 1026 J s
× 10−12
( )rate = power output = J (4 protons) = 3.60 × 1038 protons s
energy per proton
4.28

P45.59 (a) [ ] [ ]QI = M A + M B − M C − M E c2 , and QII = M C + M D − M F − MG c2
[ ]Qnet = QI + QII = M A + M B − M C − M E + M C + M D − M F − M G c2
[ ]Qnet = QI + QII = M A + M B + M D − M E − M F − M G c2

Thus, reactions may be added. Any product like C used in a subsequent reaction does not
contribute to the energy balance.

(b) Adding all five reactions gives

1 H + 1 H+ 0 e + 1 H+ 1 H+ 0 e → 4 He + 2ν + Qnet /c2
1 1 −1 1 1 −1 2

or 4 1 H + 2 0 e → 4 He + 2ν + Qnet /c2
1 −1 2

Adding two electrons to each side gives 4 1 H atom → 4 He atom + Qnet /c2
1 2

Thus Qnet = ⎡ 4 M 1 H − M 4 He ⎤ c2 = ⎣⎡4 (1.007 825) − 4.002 603⎤⎦u (931.5 MeV u)
⎣ 1 2 ⎦

= 26.7 MeV

( )P45.60 ⎡ 4π ⎛1.50 × 10− 2 cm ⎞ 3 ⎤ 10− 7
(a) The mass of the pellet is m = ρV = 0.200 g cm3 ⎢ ⎜ 2 ⎟⎥ = 3.53 × g
⎢⎣ 3 ⎝ ⎠ ⎦⎥

The pellet consists of equal numbers of 2 H and 3 H atoms, so the average molar mass is
2.50 and the total number of atoms is

⎛3.53 × 10−7 g ⎞
( )N
= ⎜ 2 .50 g mol ⎟ 6.02 × 1023 atoms mol = 8.51 × 1016 atoms
⎝ ⎠

When the pellet is vaporized, the plasma will consist of 2N particles (N nuclei and

N electrons). The total energy delivered to the plasma is 1.00% of 200 kJ or 2.00 kJ. The
( )temperature of the plasma is found from
E = (2N) 3 kBT as
2

= E = 2.00 × 103 J = 5.68 × 108 K
3NkB 8.51 × 1016 1.38 × 10−23
( )( )T
3 JK

(b) Each fusion event uses 2 nuclei, so N events will occur. The energy released will be
2

⎛ N ⎞ ⎛ 8.51 × 1016 ⎞
⎝ 2 ⎠ ⎝⎜ 2 ⎟⎠
( )E
= Q = (17.59 MeV) 1.60 × 10−13 J MeV = 1.20 × 105 J = 120 kJ

Applications of Nuclear Physics 587

P45.61 (a) The solar-core temperature of 15 MK gives particles enough kinetic energy to overcome

the Coulomb-repulsion barrier to 1 H + 3 He → 4 He + e+ + ν, estimated as ke (e)(2e) . The
1 2 2
r

Coulomb barrier to Bethe’s fifth and eight reactions is like ke (e)(7e) , larger by 7 times,

r2

( )so the required temperature can be estimated as 7 15 ×106 K ≈ 5 ×107 K .
2

(b) For 12 C + 1H → 13 N + Q,

Q1 = (12.000 000 + 1.007 825 − 13.005 739)(931.5 MeV) = 1.94 MeV

For the second step, add seven electrons to both sides to have:
13 N atom → 13C atom + e+ + e− + Q

Q2 = ⎡⎣13.005 739 − 13.003 355 − 2 (0.000 549)⎤⎦ (931.5 MeV) = 1.20 MeV
Q3 = Q7 = 2 (0.000 549)(931.5 MeV) = 1.02 MeV
Q4 = [13.003 355 + 1.007 825 − 14.003 074](931.5 MeV) = 7.55 MeV
Q5 = [14.003 074 + 1.007 825 − 15.003 065](931.5 MeV) = 7.30 MeV
Q6 = ⎣⎡15.003 065 − 15.000 109 − 2 (0.000 549)⎦⎤ (931.5 MeV) = 1.73 MeV
Q8 = [15.000 109 + 1.007 825 − 12 − 4.002 603](931.5 MeV) = 4.97 MeV

The sum is 26.7 MeV , the same as for the proton-proton cycle.

(c) Not quite all of the energy released appears as internal energy in the star. When a neutrino
is created, it will likely fly directly out of the star without interacting with any other
particle.

P45.62 (a) I2 = I 0 e− µ2 x = e−(µ2 −µ1)x
(b) I1 I0e− µ1x
(c)
I50 = e−(5.40−41.0)(0.100) = e3.56 = 35.2
I100

I50 = e−(5.40−41.0)(1.00) = e35.6 = 2.89 × 1015
I100

Thus, a 1.00-cm-thick aluminum plate has essentially removed the long-wavelength x-rays
from the beam.

588 Chapter 45

P45.63 (a) The number of fissions occurring in the zeroth, first, second, . . . nth generation is

N0 , N0K , N0K 2 , . . ., N0K n

The total number of fissions that have occurred up to and including the nth generation is

( )N = N0 + N0K + N0K 2 + + N0K n = N0 1 + K + K 2 + + K n

Note that the factoring of the difference of two squares, a2 −1 = (a +1)(a −1), can be

generalized to a difference of two quantities to any power,

a3 − 1 = (a2 + a + 1)(a − 1)
( )an+1 − 1 = an + an−1 + + a2 + a + 1 (a − 1)

Thus K n + K n−1 + + K 2 + K + 1 = K n+1 − 1
K −1

and N = N0 K n+1 − 1
K −1

(b) The number of U-235 nuclei is

N = 5.50 kg ⎛ 1 atom ⎞ ⎛ 1.66 1u −27 ⎞ = 1.41 × 1025 nuclei
⎝ 235 u ⎠ ⎝⎜ × 10 kg ⎟⎠

We solve the equation from part (a) for n, the number of generations:

N (K − 1) = K n+1 − 1

N0

N (K − 1) + 1 = K n (K )

N0

n ln K = ln ⎛⎜ N (K − 1) N0 + 1⎞⎟ = ⎛ N (K − 1) ⎞ − ln K
⎠ ln ⎜ + 1⎟
⎝ K ⎝ N0
⎠

( )n = ln (N (K − 1) N0 + 1) − 1 = ln 1.41 × 1025 (0.1) 1020 + 1 − 1 = 99.2
ln K ln1.1

Therefore time must be allotted for 100 generations:

( )∆tb = 100 10 × 10−9 s = 1.00 × 10−6 s

(c) v= B= 150 ×109 N m2 = 2.83 × 10 3 ms
ρ 18.7 ×103 kg m3

(d) V = 4 πr3 = m
3ρ

⎛ 3m ⎞1 3 ⎛ 3(5.5 kg) ⎞1 3
⎜ 4πρ ⎟ ⎜⎜⎝ ⎠⎟⎟ = 4.13 ×10−2
= ⎝ ⎠ = 18.7 ×103 kg
( )r 4π m3 m

∆td = r = 4.13 ×10−2 m = 1.46 ×10−5 s
v 2.83×103 m s

continued on next page

Applications of Nuclear Physics 589

(e) 14.6 µs is greater than 1 µs, so the entire bomb can fission. The destructive energy
released is

⎛ 200 ×106 eV ⎞ ⎛1.6 × 10−19 J ⎞ = 4.51 × 1014 J
1.41×1025 nuclei⎜ ⎟⎜ ⎟
⎝ fissioning nucleus ⎠ ⎝ 1 eV ⎠

= 4.51×1014 J ⎛ 1 ton TNT ⎞
⎜⎝ 4.2 × 109 J ⎠⎟

= 1.07 ×105 ton TNT

= 107 kilotons of TNT

What if? If the bomb did not have an “initiator” to inject 1020 neutrons at the moment
when the critical mass is assembled, the number of generations would be

( )ln 1.41 × 1025 (0.1) 1 + 1
( )n =
ln 1.1 − 1 = 582 requiring 583 10 × 10−9 s = 5.83 µs

This time is not very short compared with 14.6 µs, so this bomb would likely release
much less energy.

ANSWERS TO EVEN PROBLEMS
P45.2 184 MeV

P45.4 (a) 173 MeV (b) 0.078 8%

P45.6 (a) 8.68 MeV (b) The proton and the boron nucleus have positive charges. The
colliding particles must have enough kinetic energy to approach very closely in spite
of their electric repulsion.

P45.8 2.63 kg d

P45.10 (a) 4.84V −1 3 (b) 6V −1 3 (c) 6.30V −1 3 (d) The sphere has minimum loss and the
parallelepiped maximum.

P45.12 6.25 × 1019 Bq

P45.14 25.6 MeV

P45.16 (a) (144 keV) Z1 Z2 (b) The energy is proportional to each atomic number. (c) Take Z1 =1
and Z2 = 59 or vice versa. This choice minimizes the product Z1 Z2. (d) 144 keV for both,
according to this model

P45.18 (a) 2.53 × 1031 J (b) 1.14 × 109 yr

P45.20 (a) 1.7 × 107 J (b) 7.3 kg

P45.22 12.4 h

P45.24 (a) 10.0 h (b) 3.16 m

P45.26 (a) 0.436 cm (b) 5.79 cm

590 Chapter 45

P45.28 2.39 × 10−3° C

P45.30 (a) 422 MBq (b) 153 ng

P45.32 (a) 10 (b) 106 (c) 108 eV

P45.34 (a) about 8 min (b) 27.6 min (c) 30 min ± 30%
P45.36 (a) ~106 (b) ~10−15 g

P45.38 (a) 0.963 mm (b) It increases by 7.47%.

P45.40 See the solution.

P45.42 The fractional loss in D - T is about 4 times that in 235U fission.

P45.44 221 yr
P45.46
mNA (200 MeV)
(235 g mol)⎡⎣cw (100°C − Tc ) + Lv + cs (Th −100°C)⎦⎤

P45.48 (a) ~108 m3 (b) ~1013 J (c) ~1014 J (d) ~10 kilotons

P45.50 1.01 MeV

P45.52 223 W

P45.54 26 collisions

P45.56 400 rad

P45.58 3.60 × 1038 protons s

P45.60 (a) 5.68 × 108 K (b) 120 kJ
P45.62 (a) See the solution. (b) 35.2 (c) 2.89 × 1015

46

Particle Physics and Cosmology

CHAPTER OUTLINE ANSWERS TO QUESTIONS

46.1 The Fundamental Forces in Q46.1 Strong Force—Mediated by gluons.
Nature
46.2 Positrons and Other Antiparticles Electromagnetic Force—Mediated by photons.
46.3 Mesons and the Beginning of Weak Force—Mediated by W+, W−, and Z0 bosons.
Particle Physics
46.4 Classification of Particles Gravitational Force—Mediated by gravitons.
46.5 Conservation Laws
46.6 Strange Particles and *Q46.2 Answer (b). The electron and positron together have
Strangeness very little momentum. A 1.02-MeV photon has a definite
46.7 Finding Patterns in the Particles chunk of momentum. Production of a single gamma ray
46.8 Quarks could not satisfy the law of conservation of momentum,
46.9 Multicolored Quarks which must hold true in this—and every—interaction.
46.10 The Standard Model
46.11 The Cosmic Connection
46.12 Problems and Perspectives

Q46.3 Hadrons are massive particles with structure and size.
There are two classes of hadrons: mesons and baryons.
Hadrons are composed of quarks. Hadrons interact via
the strong force. Leptons are light particles with no
structure or size. It is believed that leptons are funda-
mental particles. Leptons interact via the weak force.

Q46.4 Baryons are heavy hadrons with spin 1 or 3 composed of three quarks. Mesons are light
22

hadrons with spin 0 or 1 composed of a quark and an antiquark.

*Q46.5 Answer (c). The muon has much more rest energy than the electron and the neutrinos together.
The missing rest energy goes into kinetic energy.

*Q46.6 Answer (b). The z component of its angular momentum must be 3/2, 1/2, –1/2, or –3/2, in
units of .

Q46.7 The baryon number of a proton or neutron is one. Since baryon number is conserved, the baryon
number of the kaon must be zero.

Q46.8 Decays by the weak interaction typically take 10−10 s or longer to occur. This is slow in particle
physics.

*Q46.9 Answer a, b, c, and d. Protons feel all these forces; but within a nucleus the strong interaction
predominates, followed by the electromagnetic interaction.

591

592 Chapter 46

Q46.10 You can think of a conservation law as a superficial regularity which we happen to notice,
as a person who does not know the rules of chess might observe that one player’s two bishops
are always on squares of opposite colors. Alternatively, you can think of a conservation law as
identifying some stuff of which the universe is made. In classical physics one can think of both
matter and energy as fundamental constituents of the world. We buy and sell both of them. In
classical physics you can also think of linear momentum, angular momentum, and electric charge
as basic stuffs of which the universe is made. In relativity we learn that matter and energy are
not conserved separately, but are both aspects of the conserved quantity relativistic total energy.
Discovered more recently, four conservation laws appear equally general and thus equally
fundamental: Conservation of baryon number, conservation of electron-lepton number,
conservation of tau-lepton number, and conservation of muon-lepton number. Processes involving
the strong force and the electromagnetic force follow conservation of strangeness, charm,
bottomness, and topness, while the weak interaction can alter the total S, C, B, and T quantum
numbers of an isolated system.

Q46.11 No. Antibaryons have baryon number –1, mesons have baryon number 0, and baryons have
baryon number +1. The reaction cannot occur because it would not conserve baryon number,
unless so much energy is available that a baryon-antibaryon pair is produced.

Q46.12 The Standard Model consists of quantum chromodynamics (to describe the strong
interaction) and the electroweak theory (to describe the electromagnetic and weak interactions).
The Standard Model is our most comprehensive description of nature. It fails to unify the two
theories it includes, and fails to include the gravitational force. It pictures matter as made of six
quarks and six leptons, interacting by exchanging gluons, photons, and W and Z bosons.

Q46.13 (a) and (b) All baryons and antibaryons consist of three quarks. (c) and (d) All mesons and
antimesons consist of two quarks. Since quarks have spin quantum number 1 and can be spin-up

2
or spin-down, it follows that the three-quark baryons must have a half-integer spin, while the
two-quark mesons must have spin 0 or 1.

Q46.14 Each flavor of quark can have colors, designated as red, green, and blue. Antiquarks are colored
antired, antigreen, and antiblue. A baryon consists of three quarks, each having a different color.
By analogy to additive color mixing we call it colorless. A meson consists of a quark of one color
and antiquark with the corresponding anticolor, making it colorless as a whole.

Q46.15 The electroweak theory of Glashow, Salam, and Weinberg predicted the W+ , W−, and
Z particles. Their discovery in 1983 confirmed the electroweak theory.

*Q46.16 Answer (e). Both trials conserve momentum. In the first trial all of the kinetic energy K1 + K2 = 2K1
is converted into internal energy. In the second trial we end up with a glob of twice the mass
moving at half the speed, so it has half the kinetic energy of one original clay ball, K1/2. Energy
K1/2 is converted into internal energy, one-quarter of that converted in trial one.

Q46.17 Hubble determined experimentally that all galaxies outside the Local Group are moving away
from us, with speed directly proportional to the distance of the galaxy from us.

*Q46.18 Answer c, b, d, e, a, f, g. The temperature corresponding to b is on the order of 1013 K. That for
hydrogen fusion d is on the order of 107 K. A fully ionized plasma can be at 104 K. Neutral atoms
can exist at on the order of 3 000 K, molecules at 1 000 K, and solids at on the order of 500 K.

Q46.19 Before that time, the Universe was too hot for the electrons to remain in any sort of stable orbit
around protons. The thermal motion of both protons and electrons was too rapid for them to be in
close enough proximity for the Coulomb force to dominate.

Particle Physics and Cosmology 593

*Q46.20 Answer (a). The vast gulfs not just between stars but between galaxies and especially between

clusters, empty of ordinary matter, are important to bring down the average density of the

Universe. We can estimate the average density defined for the Solar System as the mass of the

sun divided by the volume of a lightyear-size sphere around it:

2 × 1030 kg = 6 × 10−20 kg/m3 = 6 × 10−23 g/cm3 , ten million times larger than the critical

4 π (2 × 1016 m)3
3

density 3H2/8p G = 6 × 10–30 g/cm3.

Q46.21 The Universe is vast and could on its own terms get along very well without us. But as the cos-
mos is immense, life appears to be immensely scarce, and therefore precious. We must do our
work, growing corn to feed the hungry while preserving our planet for future generations and
preserving future possibilities for the universe. One person has singular abilities and opportunities
for effort, faithfulness, generosity, honor, curiosity, understanding, and wonder. His or her place
is to use those abilities and opportunities, unique in all the Universe.

SOLUTIONS TO PROBLEMS

Section 46.1 The Fundamental Forces in Nature

Section 46.2 Positrons and Other Antiparticles

P46.1 Assuming that the proton and antiproton are left nearly at rest after they are produced, the energy
P46.2 E of the photon must be

E = 2E0 = 2 (938.3 MeV) = 1 876.6 MeV = 3.00 ×10−10 J

Thus, E = hf = 3.00 × 10−10 J

f = 3.00 × 10−10 J = 4.53 × 1023 Hz
6.626 × 10−34 J ⋅ s

λ = c = 3.00 × 108 m s = 6.62 × 10−16 m
f 4.53 × 1023 Hz

The half-life of 14O is 70.6 s, so the decay constant is λ = ln 2 = ln 2 = 0.009 82 s−1.
T1 2 70.6 s

The number of 14O nuclei remaining after five minutes is

( )N = N0e−λ t = 1010 (e− 0.009 82 )s−1 (300 s) = 5.26 × 108

The number of these in one cubic centimeter of blood is

( )⎛ ⎞ ⎛ cm 3 ⎞
⎟= ⎜ cm 3 ⎟
N′ = N⎜ ⎝ ⎠
1.00 cm3 5.26 × 108 1.00 = 2 .63 × 105
2000
⎝ total volume of blood ⎠

( ) ( )and their activity is R = λ N′ = 0.009 82 s−1 2 .63 ×105 = 2 .58 ×103 Bq ~103 Bq

*P46.3 (a) The rest energy of a total of 6.20 g of material is converted into energy of electromagnetic
radiation:

( )E = mc2 = 6.20 × 10−3 kg 3 × 108 m s 2 = 5.58 × 1014 J

(b) 5.58 ×1014 J = 5.58 ×1014 J ⎛ $0.14 ⎞ ⎛ k ⎞ ⎛ W ⎞ ⎛ 3 1h s ⎞ = $2.17 ×107
⎝⎜ kWh ⎠⎟ ⎜⎝1 000 ⎟⎠ ⎜ Js ⎟ ⎜⎝ 600 ⎠⎟
⎝ ⎠

All from two cents’ worth of stuff.

594 Chapter 46

P46.4 The minimum energy is released, and hence the minimum frequency photons are produced, when
P46.5 the proton and antiproton are at rest when they annihilate.

That is, E = E0 and K = 0. To conserve momentum, each photon must carry away one-half the
energy.

Thus Emin = 2E0 = E0 = 938.3 MeV = hfmin
2

( )(938.3 MeV) 1.60 ×10−13 J MeV 2.27 × 1023 Hz
Thus, ( )fmin = =
6.626 × 10−34 J ⋅ s

λ= c = 3.00 ×108 m s = 1.32 ×10−15 m
fmin 2.27 ×1023 Hz

In γ → p+ + p− ,

we start with energy 2.09 GeV

we end with energy 938.3 MeV + 938.3 MeV + 95.0 MeV + K2

where K2 is the kinetic energy of the second proton.

Conservation of energy for the creation process gives K2 = 118 MeV

Section 46.3 Mesons and the Beginning of Particle Physics

P46.6 The reaction is µ+ + e− → ν + ν
P46.7 muon-lepton number before reaction:
electron-lepton number before reaction: (−1) + (0) = −1
(0) + (1) = 1

Therefore, after the reaction, the muon-lepton number must be –1. Thus, one of the neutrinos
must be the anti-neutrino associated with muons, and one of the neutrinos must be the neutrino
associated with electrons:

Then νµ and νe
µ+ + e− → νµ + νe

The creation of a virtual Z 0 boson is an energy fluctuation ∆E = 91 × 109 eV. It can last no

longer than ∆t = 2∆E and move no farther than

( ( )( ) )c(∆t)
= hc = 6.626 ×10−34 J ⋅ s 3.00 ×108 ms ⎛ 1 eV ⎞
4π ∆E 4π 91×109 eV ⎝⎜1.60 ×10−19 J ⎟⎠

= 1.06 ×10−18 m = ~10−18 m .

Particle Physics and Cosmology 595

*P46.8 (a) The particle’s rest energy is mc2. The time interval during which a virtual particle of this

mass could exist is at most ∆t in ∆E∆t = = mc2∆t. The distance it could move is at most
2

( ( )( ) )c∆t
= c = 6.626 × 10−34 J ⋅ s 2.998 × 108 m/s = 1.240 × 10−6 eV ⋅ m = 1240 eV ⋅ nm
2mc2 4π mc2 1.602 × 10−19 J/eV 4π mc2 4π mc2

= 98.7 eV ⋅ nm
mc2

According to Yukawa’s line of reasoning, this distance is the range of a force that could be
associated with the exchange of virtual particles of this mass.

(b) The range is inversely proportional to the mass of the field particle.

(c) Our rule describes the electromagnetic, weak, and gravitational interactions.
For the electromagnetic and gravitational interactions, we take the limiting form of the
rule with infinite range and zero mass for the field particle. For the weak interaction,
98.7 eV ⋅ nm/90 GeV ≈ 10–18 m = 10–3 fm, in agreement with the tabulated information.
For the strong interaction, we do not have a separately measured mass for a gluon, so we
cannot say that this rule defines the range.

(d) 98.7 eV⋅nm/938.3 MeV ≈ 10–1–9–6 m ~10–16 m

P46.9 From Table 46.2 in the chapter text M π0 = 135 MeV c2.

Therefore, Eγ = 67.5 MeV for each photon

p = Eγ = 67.5 MeV c
c

and f = Eγ = 1.63 × 1022 Hz
h

P46.10 The time interval for a particle traveling with the speed of light to travel a distance of 3 ×10−15 m is
∆ t = d = 3×10−15 m = ~10−23 s

v 3×108 m s

596 Chapter 46

( )P46.11 (a) ∆E = mn − mp − me c2

From the table of isotopic masses in Chapter 44,

∆E = (1.008 665 −1.007 825) (931.5) = 0.782 MeV

(b) Assuming the neutron at rest, momentum conservation for the decay process implies
pp = pe. Relativistic energy for the system is conserved

( ) ( )mpc2 2 + p2pc2 + mec2 2 + pe2c2 = mnc2

Since pp = pe, (938.3)2 + ( pc)2 + (0.511)2 + ( pc)2 = 939.6 MeV

Solving the algebra gives pc = 1.19 MeV

If pec = γ mevec = 1.19 MeV, then γ ve = 1.19 MeV = x = 2.33 where x = ve
Solving, c 0.511 MeV 1− x2 c

Then mpvp = γemeve : ( )x2 = 1 − x2 5.43 and x = ve = 0.919
c

ve = 0.919c

( ( )( ) )vp
= γ e me ve c = (1.19 MeV) 1.60 ×10−13 J MeV
mpc ms
1.67 ×10−27 3.00 ×108

vp = 3.80 ×105 m s = 380 km s

(c) The electron is relativistic; the proton is not. Our criterion for answers accurate to three

significant digits is that the electron is moving at more than one-tenth the speed of light and
the proton at less than one-tenth the speed of light.

Section 46.4 Classification of Particles

P46.12 In ? + p+ → n + µ+, charge conservation requires the unknown particle to be neutral. Baryon
number conservation requires baryon number = 0. The muon-lepton number of ? must be –1.
So the unknown particle must be νµ .

Particle Physics and Cosmology 597

Section 46.5 Conservation Laws Le 0+0 →0+1
P46.13 (a) p + p → µ+ + e− Lµ 0 + 0 → −1+ 0
charge −1+1 → +1+1
and baryon number : 1+1→1+ 0
(b) π − + p → p + π +
(c) p + p → p + π +

(d) p + p → p + p + n baryon number : 1+1 → 1+1+1

(e) γ + p → n + π 0 charge 0+1→ 0+0

P46.14 (a) Baryon number and charge are conserved, with respective values of 0 +1 = 0 +1
and 1+1 = 1+1 in both reactions.

(b) Strangeness is not conserved in the second reaction.

P46.15 (a) π − → µ− + νµ Lµ : 0 → 1 − 1 Le : 0 → 1 −1+ 0
(b) K+ → µ+ + νµ Lµ : 0 → −1+ 1
(c) νe + p+ → n + e+ Le : −1+ 0 → 0 − 1
(d) νe + n → p+ + e− Le : 1+ 0 → 0 +1
(e) νµ + n → p+ + µ− Lµ : 1+ 0 → 0 + 1
(f ) µ− → e− + νe + νµ Lµ : 1 → 0 + 0 + 1 and

P46.16 Baryon number conservation allows the first and forbids the second .

P46.17 (a) p+ → π + + π 0 Baryon number conservation is violated: 1 → 0 + 0

(b) p+ + p+ → p+ + p+ + π 0 This reaction can occur .

(c) p+ + p+ → p+ + π + Baryon number is violated: 1+1→1+ 0

(d) π + → µ+ + νµ This reaction can occur . 0 → 0+1
(e) n0 → p+ + e− + νe This reaction can occur .
(f ) π + → µ+ + n Violates baryon number :

Violates muon-lepton number : 0 → −1+ 0

598 Chapter 46

P46.18 Momentum conservation for the decay requires the pions to have equal speeds.

The total energy of each is 497.7 MeV
so
Solving, 2

and ( )E2 = p2c2 + mc2 2 gives

(248.8 MeV)2 = ( pc)2 + (139.6 MeV)2

pc = 206 MeV = γ mvc = mc2 c)2 ⎛ v ⎞
⎝⎜ c ⎟⎠
1− (v

pc = 206 MeV = 1 c)2 ⎛ v ⎞ = 1.48
mc2 139.6 MeV ⎜⎝ c ⎠⎟
1− (v

v = 1.48 ⎛ v ⎞ 2
c ⎝⎜ c ⎠⎟
1 −

⎛ v ⎞2 = ⎡ − ⎛ v ⎞2 ⎤ = 2.18 − ⎛ v ⎞2
⎝⎜ c ⎠⎟ 2.18⎢1 ⎜⎝ c ⎠⎟ ⎥ 2.18 ⎝⎜ c ⎟⎠
⎦⎥
⎣⎢

⎛ v ⎞2 = 2.18
3.18 ⎝⎜ c ⎠⎟

so v = 2.18 = 0.828
c 3.18

and v = 0.828c

P46.19 (a) In the suggested reaction p → e+ + γ

We would have for baryon numbers +1 → 0 + 0

∆B ≠ 0, so baryon number conservation would be violated.

(b) From conservation of momentum for the decay: pe = pγ
Then, for the positron,
becomes ( )Ee2 = 2 + E2
pec 0,e

( )Ee2 = 2 + E2 = Eγ2 + E02,e
pγ c 0,e

From conservation of energy for the system: E0, p = Ee + Eγ
or
so Ee = E0,p − Eγ

Ee2 = E2 − 2E0,p Eγ + Eγ2
0, p

Equating this to the result from above gives Eγ2 + E2 = E2 − 2E0,p Eγ + Eγ2
0,e 0, p

or Eγ = E2 − E2 = (938.3 MeV)2 − (0.511 MeV)2 = 469 MeV
0, p 0,e 2 (938.3 MeV)

2 E0, p

Thus Ee = E0,p − Eγ = 938.3 MeV − 469 MeV = 469 MeV

Also, pγ = Eγ = 469 MeV
c c

and pe = pγ = 469 MeV
c

continued on next page

Particle Physics and Cosmology 599

(c) The total energy of the positron is Ee = 469 MeV
But,
E0,e
1− v c 2
( )Ee = γ E0,e =

so 1 − ⎛ v ⎞2 = E0,e = 0.511 MeV = 1.09 × 10−3
⎝⎜ c ⎟⎠ Ee 469 MeV

which yields v = 0.999 999 4c

P46.20 The relevant conservation laws are ∆Le = 0
and ∆Lµ = 0
∆Lτ = 0

(a) π + → π 0 + e+ + ? Le : 0 → 0 − 1+ Le implies Le = 1 and we have a νe

(b) ? + p → µ− + p + π + Lµ: Lµ + 0 → + 1 + 0 + 0 implies Lµ = 1 and we have a νµ

(c) Λ0 → p + µ− + ? Lµ : 0 → 0 + 1+ Lµ implies Lµ = −1 and we have a νµ

(d) τ + → µ+ + ? + ? Lµ : 0 → − 1 + Lµ implies Lµ = 1 and we have a νµ

Lτ : −1 → 0 + Lτ implies Lτ = −1 and we have a ντ

Conclusion for (d): Lµ = 1 for one particle, and Lτ = −1 for the other particle.
We have νµ
and
ντ

Section 46.6 Strange Particles and Strangeness

P46.21 (a) Λ0 → p + π − Strangeness: −1 → 0 + 0 (strangeness is not conserved )

(b) π − + p → Λ0 + K0 Strangeness: 0 + 0 → −1+1 ( 0 = 0 and strangeness is conserved )

(c) p + p → Λ0 + Λ0 Strangeness: 0 + 0 → +1 −1 ( 0 = 0 and strangeness is conserved )

(d) π − + p → π − + Σ+ Strangeness: 0 + 0 → 0 −1 ( 0 ≠ −1 : strangeness is not conserved )

(e) Ξ− → Λ0 + π − Strangeness: −2 → −1+ 0 ( −2 ≠ −1 so strangeness is not conserved )

(f) Ξ0 → p + π − Strangeness: −2 → 0 + 0 ( −2 ≠ 0 so strangeness is not conserved )

P46.22 The ρ0 → π + + π − decay must occur via the strong interaction.

The K 0 → π+ + π− decay must occur via the weak interaction.
S

600 Chapter 46

P46.23 (a) µ− → e− + γ Le : 0 → 1+ 0,
and Lµ : 1→0
Le : 0 → 0+1+1
(b) n → p + e− + νe
(c) Λ0 → p + π 0 Strangeness: −1 → 0 + 0,

and charge: 0 → +1+ 0

(d) p → e+ + π 0 Baryon number: +1 → 0 + 0
(e) Ξ0 → n + π 0 Strangeness: −2 → 0 + 0

P46.24 (a) π − + p → 2η violates conservation of baryon number as 0 +1 → 0, not allowed .

(b) K− + n → Λ0 + π −

Baryon number, 0+1→1+ 0
Charge, −1+ 0 → 0 −1
Strangeness, −1+ 0 → −1+ 0

Lepton number, 0→0

The interaction may occur via the strong interaction since all are conserved.

(c) K− → π − + π 0

Strangeness, −1 → 0 + 0

Baryon number, 0→0

Lepton number, 0→0

Charge, −1 → −1+ 0

Strangeness conservation is violated by one unit, but everything else is conserved. Thus,

the reaction can occur via the weak interaction , but not the strong or electromagnetic
interaction.

(d) Ω− → Ξ− + π 0

Baryon number, 1→1+ 0
Lepton number, 0→0
Charge, −1 → −1+ 0
Strangeness, −3 → −2 + 0

May occur by weak interaction , but not by strong or electromagnetic.

(e) η → 2γ

Baryon number, 0→0

Lepton number, 0→0

Charge, 0→0

Strangeness, 0→0

No conservation laws are violated, but photons are the mediators of the electromagnetic

interaction. Also, the lifetime of the h is consistent with the electromagnetic interaction .