Nuclear Physics_ Radioativity_Duetron at

Nuclear Physics

1. Physics 102: Lecture 27, Slide 1
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2. Physics 102: Lecture 27, Slide 2
Nuclear Binding, Radioactivity
Physics 102: Lecture 28

3. Physics 102: Lecture 27, Slide 3
Nucleus = Protons + Neutrons
nucleons
A = nucleon number (atomic mass number)
Gives you mass density of element
Z = proton number (atomic number)
Gives chemical properties (and name)
N = neutron number
A=N+Z
Recall: Nuclear Physics
Li
6
3
A
Z

4. Physics 102: Lecture 27, Slide 4
A material is known to be an isotope of lead
Based on this information which of the following
can you specify?
1) The atomic mass number
2) The neutron number
3) The number of protons
Lead Z=82
Preflight 27.1
Chemical properties (and name) determined by
number of protons (Z)

5. Physics 102: Lecture 27, Slide 5
Hydrogen atom: Binding energy =13.6eV
Binding energy of deuteron = or
2.2Mev! That’s around 200,000 times bigger!
2.210
6
eV
Simplest Nucleus:
Deuteron=neutron+proton
(Isotope of H)
neutron proton
Very strong force
Coulomb force
electron
proton
Strong Nuclear Force
(of electron to nucleus)

6. Physics 102: Lecture 27, Slide 6
Can get 4 nucleons into
n=1 state. Energy will
favor N=Z
Pauli Principle - neutrons and protons have
spin like electron, and thus m
s
= 1/2.

nnpp

nnpp
But protons repel one another
(Coulomb Force) and when Z is large
it becomes harder to put more
protons into a nucleus without adding
even more neutrons to provide more
of the Strong Force. For this reason,
in heavier nuclei N>Z.
# protons = # neutrons
7

7. Physics 102: Lecture 27, Slide 7
ground state
2.2 MeV
Deuteron Binding Energy

8. Physics 102: Lecture 27, Slide 8
Nuclei have energy level (just like atoms)
12
C energy levels
Note the energy scale is MeV rather than eV
energy needed to
remove a proton from
12
C is 16.0 MeV
energy needed to
remove a neutron from
12
C is 18.7 MeV

9. Physics 102: Lecture 27, Slide 9
Preflight 27.2
Where does the energy released in the
nuclear reactions of the sun come from?
(1)covalent bonds between atoms
(2)binding energy of electrons to the nucleus
(3)binding energy of nucleons

10. Physics 102: Lecture 27, Slide 10
Binding Energy
Einstein’s famous equation E = m c
2
Proton: mc
2
= 938.3MeV
Neutron: mc
2
= 939.5MeV
Deuteron: mc
2
=1875.6MeV
Adding these, get
1877.8MeV
Difference is
Binding energy,
2.2MeV
M
Deuteron = M
Proton + M
Neutron – |Binding Energy|
proton:
mc
2
=(1.67x10
-27
kg)(3x10
8
m/s)
2
=1.50x10
-10
J

11. Physics 102: Lecture 27, Slide 11
ACT: Binding Energy
Which system “weighs” more?
1)Two balls attached by a relaxed spring.
2)Two balls attached by a stretched spring.
3)They have the same weight.
M
1
= M
balls
+ M
spring
M
2
= M
balls
+ M
spring
+ E
spring
/c
2
M
2
– M
1
= E
spring
/c
2
~ 10
-16
Kg

12. Physics 102: Lecture 27, Slide 12
Iron (Fe) has most binding energy/nucleon. Lighter
have too few nucleons, heavier have too many.
B
I
N
D
I
N
G

E
N
E
R
G
Y

i
n

M
e
V
/
n
u
c
l
e
o
n
92
238
U
10
Binding Energy Plot
Fission
F
u
s
io
n
Fusion = Combining small atoms into large
Fission = Breaking large atoms into small

13. Physics 102: Lecture 27, Slide 13
Which element has the highest binding
energy/nucleon?
Preflight 27.3
• Neon (Z=10)
• Iron (Z=26)
• Iodine (Z=53)
37%
19%
44%

14. Physics 102: Lecture 27, Slide 14
Which of the following is most correct for the
total binding energy of an Iron atom (Z=26)?
9 MeV
234 MeV
270 MeV
504 Mev
For Fe, B.E./nucleon  9MeV
26
56
Fehas 56 nucleons
Total B.E  56x9=504 MeV
Preflight 27.4
13%
39%
31%
17%

15. Physics 102: Lecture 27, Slide 15
 particles: nuclei
2
4
He


particles: electrons
 : photons (more energetic than x-rays) penetrate!
3 Types of Radioactivity
Easily Stopped
Stopped by metal
Radioactive
sources
B field
into
screen
detector

16. Physics 102: Lecture 27, Slide 16
92
238
U
90
234
Th: example
2
4
Herecall
: example
Decay Rules
1)Nucleon Number (A) is conserved.
2)Atomic Number (Z) is conserved.
3)Energy and momentum are conserved.
: example 
0
0
*
PP
A
Z
A
Z
1)238 = 234 + 4 Nucleon number
conserved
2)92 = 90 + 2Charge conserved


 e
0
1
1
1
1
0
pn
Needed to conserve
momentum.

0
0


17. Physics 102: Lecture 27, Slide 17
A nucleus undergoes  decay. Which of the
following is FALSE?
1. Nucleon number decreases by 4
2. Neutron number decreases by 2
3. Charge on nucleus increases by 2
Preflight 27.6
 decay is the emission of
2
4
He
He
4
2
234
90
238
92
ThU Ex.
Z decreases by 2
(charge decreases!)
A decreases by 4
27%
39%
34%

18. Physics 102: Lecture 27, Slide 18


The nucleus undergoes decay.
90
234
Th
Which of the following is true?
1. The number of protons in the daughter
nucleus increases by one.
2. The number of neutrons in the daughter
nucleus increases by one.


decay is accompanied by the emission of an
electron: creation of a charge -e.
In fact, inside the nucleus,
and the electron and neutrino “escape.”

npe


e
Preflight 27.7

0
0
0
1
???
??
234
90 XTh 

e 
0
0
0
1
234
91
234
90 PaTh 

e

19. Physics 102: Lecture 27, Slide 19
ACT: Decay
Which of the following decays is NOT allowed?
HePbPo
4
2
210
82
214
84

92
238
U
90
234
Th
40 40 0 0
19 20 1 0
K P e


  
NC
14
7
14
6
1
2
3
4
238 = 234 + 4
92 = 90 + 2
214 = 210 + 4
84 = 82 + 2
14 = 14+0
6 ≠ 7+0
40 = 40+0+0
19 = 20-1+0

20. Physics 102: Lecture 27, Slide 20

N
t
N
If the number of radioactive nuclei present is cut in
half, how does the activity change?
1 It remains the same
2 It is cut in half
3 It doubles
No. of nuclei
present
decay constant
Decays per second,
or “activity”
Radioactive decay rates
Preflight 27.8
26%
58%
16%

21. Physics 102: Lecture 27, Slide 21
ACT: Radioactivity
Start with 16
14
C atoms.
After 6000 years, there are only 8 left.
How many will be left after another 6000 years?
1) 0 2) 4 3) 8
Every 6000 years ½ of atoms decay

N
t
N
No. of nuclei
present
decay constant
Decays per second,
or “activity”

22. Physics 102: Lecture 27, Slide 22 time

N(t)N
0
e
t
N
0
2

t
T
1/2
Decay Function

23. Physics 102: Lecture 27, Slide 23
Instead of base e we can use base 2:

N(t)N
0e
t
Survival:
No. of nuclei
present at time t
No. we started
with at t=0
e
t
2

t
T
1/2

T
1/2
0.693

where
Then we can write

N(t)N
0
e
t
N
0
2

t
T
1/2
Half life
Radioactivity Quantitatively

N
t
N
No. of nuclei
present
decay constant
Decays per second,
or “activity”

24. Physics 102: Lecture 27, Slide 26
ACT/Preflight 27.9
The half-life for beta-decay of
14
C is ~6,000 years.
You test a fossil and find that only 25% of its
14
C is
un-decayed. How old is the fossil?
1. 3,000 years
2. 6,000 years
3. 12,000 years
At 0 years: 100% remains
At 6,000 years: 50% remains
At 12,000 years: 25% remains

25. Physics 102: Lecture 27, Slide 27
Summary
•Nuclear Reactions
–Nucleon number conserved
–Charge conserved
–Energy/Momentum conserved
–  particles = nuclei
– 
-
particles = electrons
–  particles = high-energy photons
•Decays
–Half-Life is time for ½ of atoms to decay

N(t)N
0e
t
Survival:

T
1/2
0.693

2
4
He