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1
Nuclear Physics and Society
Physics Department
University of Richmond
Nuclear Basics
Motivation:
Educate the Public and University
communities about basic nuclear physics
ideas and issues
2
U.S. Department of Energy Workshop
July 2002, Washington D.C.
Role of the Nuclear Physics Research Community (universities
and national laboratories) in Combating Terrorism
Education and Outreach
•Community
•Local PD and FD
DOE Workshop …
3
Border Control/ US Customs
•1,000,000 visas/year
•422 ports of entry
•1700 flights / day
•290 ships / day
•60 trains / day
•1200 busses / day
•540,000,000 border entries /
year
Time per primary inspection
8 seconds => 1 hour delay
Cargo Containers
10,000,000 per year … 10,000 per
ship!
5 / minute @ L.A.
< 3% inspected
What the Course is/is not
4
This is not a radiation workers course
This is not a course that will certify you for anything
We hope that we can introduce you to some basic facts about
nuclear physics, about radiation, about detectors etc., which
may be useful for you to know.
Who are We
5
Con Beausang
Chairman & Associate Professor Physics Department
Jerry Gilfoyle
Professor, Physics Department
Paddy Regan
Professor Physics Department, University of Surrey, U.K.
6
Monday April 13th
Lecture 1:
The types of radiation, their properties and how these can be used to detect them.
Some basic definitions.
Introduction to radiation detectors.
Tuesday April 14th
Laboratory Session: 12:15  3:30 pm
Environmental Radiation Laboratory experience
Measurement of half-life
Demonstration of shielding
Find the source
Lecture 2:
The creation of the elements. Nuclear physics in the cosmos.
Wednesday April 15th
Laboratory Session 2: 12:15  3:30
Repeat of Tuesdays experience
Lecture 3:
Applications of Nuclear Physics: Nuclear weapons, nuclear power and nuclear medicine.
Thursday April 16th
Lecture 4
Some of the frontiers of modern nuclear physics research
Nuclear Physics and Society
7
The Cookie Quiz
Alpha
cookie
Beta
cookie
Gamma
cookie
Neutron
cookie
8
The Cookie Quiz
Alpha
cookie
Beta
cookie
Gamma
cookie
Neutron
cookie
Throw away
Put in pocket
Hold in clenched fist
Eat one … GOAL: Minimize your
radiation exposure
9
The Cookie Quiz: Answer 1
Alpha
cookie
Beta
cookie
Gamma
cookie
Neutron
cookieThrow away
Put in pocket
Hold in clenched fist
Eat one …
10
The Cookie Quiz: Correct Answer
Alpha
cookie
Beta
cookie
Gamma
cookie
Neutron
cookie
Throw away
Put in pocket
Hold in clenched fist
Eat one …
GOAL: Minimize your
radiation exposure
Mutiny at once
Retire from the navy and
Toss ALL cookies away
… when I was
young(er), I was curious
…
What are we made of ?
… sugar and spice and all things nice
… that’s what little girls are made of
… snips and snails and puppy dogs tails
… that’s what little boys are made of.
… ok mum, … so what
are sugar, spice and
snails etc. made of? … cells
… molecules
… atoms
… nuclei
The Uncertainty Principle
Heisenberg (Quantum Mechanics)
∆(position) ∆(momentum) > Constant
Beausang (Teaching)
∆(truth) ∆(clarity) > Constant
Atoms … are made of …
Electrons
… very light, but occupy most of the volume
inside an atom
Nuclei
… lie at the Core of Atoms
… very heavy, very small, very compact
…occupies almost none of the volume inside
the atom
How do we know?
How to see the invisible?
… size of your probe
… scattering
Alpha-particle beam
Detector
Zinc-sulfide
screen
Discovery of the
nucleus
~1910
The eyes of
Geiger and
Marsden
16-inch
Battleship
shells and
tissue paper
Think of atoms as being like a mini solar system
… The sun at the center is the nucleus, the electrons
orbit the nucleus, like the planets orbit around the
sun
Bohr Model
Electrons
•Very small
•Point-like particles (i.e.nothing inside an electron)
•Very light ~ 1/2000th
of proton mass
•Negatively charged (-1 elementary charge)
•Electrons occupy almost all the space in the atom (orbiting the
nucleus like the earth and other planets orbit the sun)
•Have almost none of the mass of the atom
•All of chemistry has to do with electrons from different atoms
interacting with each other
The Nucleus
•Made up of protons and neutrons
•Almost all of the mass of the atom is
concentrated in the nucleus.
• >99.9% of the known mass in the universe.
•Occupies almost none of the volume of the
atom.
•Radius < 1/10,000
•Volume < 1/1,000,000,000,000
•The nucleus is the source of almost all the
things we commonly think of as being
radioactive.
The Nucleus Protons
•Positively charged
(+1 elementary charge)
•Size ~ 1 fm (10-15
m)
•Mass 938 MeV/c2
= 1
Neutrons
•Neutral
(0 charge)
•Size ~ 1 fm (10-15
m)
•Mass 939 MeV/c2
~ 1
Neutrons are slightly more massive than
the protons!!!
This has huge consequences for us!
Delicate Balances
Laws of Physics
1) If it can happen … it will happen …
2) If some law forbids it to happen … it will happen more
slowly …
3) If a process is really REALLY forbidden to happen …
it just takes a long time …
Standard Model:
Neutron and proton are
very close relatives
quark structure
… proton (uud)
… neutron (udd)
Many laws allow neutrons to `change into’
into protons … change a d-quark into a u-
quark (or vice versa)
… beta-decay
The half life of a free neutron (i.e., one not inside a
nucleus) is only about 12 minutes!!!
Mass Neutron = 939.565330 MeV/c2
Mass Proton = 938.271998 MeV/c2
But …
Inside a nucleus … neutrons are stable
The half life of a free proton is > 1031
years
Inside some nuclei protons can ‘decay’ into neutrons
Imagine … if they were not!
Then in ~ 1-2 hours the entire universe
would be made of Hydrogen
E = mc2
The Nucleus
•Atoms are electrically neutral
•The number of protons in a nucleus is equal to and determines the number
of orbiting electrons
the chemistry
the element name
•Hydrogen (1
1H)
1 proton, 0 neutrons
Mass = 1
•Helium (4
2He) (Alpha-particle)
2 protons, 2 neutrons
Mass = 4
•Uranium (238
92U)
92 protons, 146 neutrons
Mass = 238
The Nucleus
Many elements have several stable nuclei with the
same number of protons but different numbers of
neutrons …
same name
same chemistry
different mass
Isotopes
The Periodic Table of the Elements
Chart of the Nuclei
1
H 2
D
3
He 4
He
6
Li 7
Li
n
9
Be
3
T
5
He 6
He
5
Li
6
Be 7
Be 8
Be
8
Li
7
He
9
Li
10
Be
10
Li 11
Li
8
He 9
He
11
Be 12
Be
10
B 11
B9
B
14
Be
12
B 13
B 14
B 15
B8
B7
B
12
C 13
C 14
C 15
C 16
C 17
C11
C10
C9
C8
C
Z=No.ofProtons
0
1
2
3
4
5
6
N = No. of Neutrons
0 1 2 3 4 5 6 7 8 9
Chart
of the
Nuclei
The Landscape
~300 stable
~ 7000 unstable … radioactive.
Half Life
28
Time taken for half of the substance to decay away
Example:
If you have 1000 radioactive nuclei
and
If their half life is 30 minutes
After 30 minutes 500 nuclei remain
After 60 minutes 250 remain
After 90 minutes 125 remain
After 120 minutes 62 remain
There is a huge variation in
half lives of different isotopes
…. From a tiny fraction of a
second to roughly the age of the
universe.
Some Isotopes & Their Half LivesSome Isotopes & Their Half Lives
ISOTOPEISOTOPE HALF-HALF-
LIFELIFE
APPLICATIONSAPPLICATIONS
Uranium billions
of years
Natural uranium is comprised of several different isotopes.
When enriched in the isotope of U-235, it’s used to power
nuclear reactor or nuclear weapons.
Carbon-14 5730 y Found in nature from cosmic interactions, used to “carbon
date” items and as radiolabel for detection of tumors.
Cesium-137 30.2 y Blood irradiators, tumor treatment through external
exposure. Also used for industrial radiography.
Hydrogen-3 12.3 y Labeling biological tracers.
Irridium-192 74 d Implants or "seeds" for treatment of cancer. Also used for
industrial radiography.
Molybdenum-99 66 h Parent for Tc-99m generator.
Technicium-99m 6 h Brain, heart, liver (gastoenterology), lungs, bones, thyroid,
and kidney imaging, regional cerebral blood flow, etc.
29
The Amount of Radioactivity isThe Amount of Radioactivity is
NOT Necessarily Related to SizeNOT Necessarily Related to Size
• Specific activity is the amount of
radioactivity found in a gram of
material.
• Radioactive material with long half-
lives have low specific activity.
1 gram of Cobalt-60
has the same activity as
1800 tons of natural Uranium
30
31
For Example: Suppose we have
1,000,000,000 atoms of material A with a half life of 1 second
and
1,000,000,000 atoms of material B with a half life of 1 year
(real sources have many more atoms in them)
Suppose they both decay by alpha emission.
In the First Second
Substance A: Half the nuclei will decay
… 500,000,000 alpha particles will come zipping out at you.
1 year = 365 days * 24 hours * 60 minutes * 60 seconds = 31,536,000 seconds
In the First Second for substance B
Only ~ 500,000,000 / 31,536,000 = 16 nuclei will decay
… only 16 alpha particles will come zipping at you
32
On the other hand …
In 10 seconds … almost all of the radioactivity in substance A is gone away
But it takes years for the activity of substance B to go away!
Nuclear Bombs …
The fissile material (U or Pu) has a long half-life. Low specific activity. Not
much activity on the outside.
Dirty Bombs …
The radioactive material wrapped around the explosive would probably
have a much shorter half-life. Perhaps significant activity on the outside.
Types of Radioactivity
33
Each type of radiation has
different properties which affect
the hazards they pose, the
detection mechanism and the
shielding required to stop them.
Five Common Types
Alpha Decay
Beta Decay
Gamma Decay
Fission
Neutron Emission
Each of the particles emitted in the decay carries a lot of
kinetic energy. Damage can be caused when this energy
is absorbed in a human cell.
Alpha Decay
34
An alpha particle (α) is an energetic, He nucleus
(4
2He2)
Alpha decay mostly occurs for heavy nuclei
Example
238
94Pu  234
92U + 4
2He
Half-life: 88 years
Energy α =5.56 MeV
Alpha Decay
35
Very easy to shield
A sheet of paper, skin, or a few cm (~inch)
of air will stop an alpha particle
External Hazard: Low
Internal Hazard: High
Alpha Decay
238
94Pu144 234
92U142 + α
• Parent nucleus 238
94Pu144
• Daughter Nucleus 234
92U142
–Often the daughter nucleus is also
radioactive and will itself subsequently
decay.
–Decay chains or families (e.g. uranium,
thorium decay chains). 36
Decay Chains
37
238
94Pu  234
92U + α t1/2 = 88 yrs
234
92U  230
90Th + α t1/2 = 2.5 105
yrs
230
90Th  226
88Ra + α t1/2 = 8.0 104
yrs
226
88Ra  222
86Rn + α t1/2 = 1.6 103
yrs
222
86Rn  218
84Po + α t1/2 = 3.8 days
218
84Po  214
82Pb + α t1/2 = 3.1 min
214
82Pb  214
83Bi + β t1/2 = 27 min
214
83Bi  214
84Po + β t1/2 = 20 min
214
84Po  210
82Pb + α t1/2 = 160 µs
Decay Chains
38
210
82Pb  210
83Bi + β t1/2 = 22 yrs
210
83Bi  210
84Po + β t1/2 = 5 days
210
84Po  206
82Pb + α t1/2 = 138 days
206
82Pb is STABLE
Decay Chains
39
Pu
U
Th
Ra
Rn
Po
Pb
Hg
Au
Beta Decay
• The neutron and the proton are very similar to
each other (very closely related).
• A neutron can ‘change into’ a proton, or vice
versa.
• When this happens, an energetic electron (or
positron) is emitted.
• This is called beta-decay
40
A beta-particle is an electron (e) or
its anti-particle the positron (e+
)
n  p + e-
+ ν
p  n + e+
+ ν
Beta Decay
41
In terms of nuclei beta-decay looks like
As in the case of alpha decay the daughter nuclei are
usually radioactive and will themselves decay.
•Beta-particles are HARDER to stop
Since the electron is lighter than an alpha-particle
and carries less charge.
•Therefore, the range of a beta-particle is greater and it
137
55Cs82  137
56Ba81 + e-
+ ν
Beta-Decay
42
•Beta-particles are HARDER to stop
Since the electron is lighter than an alpha-
particle and carries less charge.
•Therefore, the range of a beta-particle is greater
and it takes more shielding to stop beta-particles
(electrons or positrons) than alpha particles
~ few mm or 1 cm of lead
~ few feet of air
Gamma-Decay
43
•A beta-decay or alpha-decay typically leaves the
daughter nucleus in a highly excited state.
•To get to the ground state the nucleus (rapidly …
almost instantly) emits one or more gamma-rays
•Gamma-rays are a very energetic form of light.
More energy and more penetrating than x-rays.
•No charge
•Much more penetrating than either alpha or beta.
•Few inches of Pb, many feet of air
Gamma-Decay
44
•Gamma-ray energies are characteristic of the nucleus.
•Measure the energies … identify the nucleus.
(just like atoms or molecules give off characteristic
colors of light).
Measuring the gamma-ray is by far the best and easiest
way to measure what type of radioactive substance you
are dealing with.
Fission
45
What holds nuclei together?
•Protons repel each other (opposites attract, like
repel)
•Coulomb Force
Some other force must hold nuclei together
The STRONG FORCE
•Attractive and Stronger than the Coulomb Force
•But short range
Fission
46
What happens if you have a lot of protons (i.e in a
heavy nucleus)?
…Eventually the Coulomb repulsion will win
… and the nucleus will fall apart into two smaller
(radioactive!!) nuclei.
FISSION
An enormous amount of energy is released.
This energy is utilized in power plants and in fission
bombs.
Fission
47
The heavy parent
nucleus fissions …
into two lighter fission
fragment nuclei …
Plus some left over bits
… energetic neutrons
Example:
252
Cf is a spontaneous fission source …
Sometimes this
process happens
spontaneously …
sometimes you can
‘poke’ at the
nucleus and induce
it to fission
Fission …Fission Fragments
48
Are emitted with a huge energy but stop very quickly
(very short range).
Are all radioactive nuclei and will decay usually by
beta-and gamma-decay
Mass 
Probability Heavy
fragment
Light
fragment
They have a broad
range of masses
Induced Fission
49
Some nuclei can be made to fission when struck by
something …
Usually the something is a neutron
Example: 235
U + n  fission
Remember … in the fission process extra neutrons
are released
If some of these strike other 235
U nuclei … they can
induce another fission
Induced Fission
50
Chain Reaction
Controlled … nuclear power plant … exactly
one neutron per fission induces another fission.
Uncontrolled … nuclear bomb … more than one
neutron per reaction induces another fission
What is a “Dose” of Radiation?What is a “Dose” of Radiation?
• When radiation’s energy is deposited into our body’s
tissues, that is a dose of radiation.
• The more energy deposited into the body, the higher the
dose.
• Rem is a unit of measure for radiation dose.
• Small doses expressed in mrem = 1/1000 rem.
• Rad & R (Roentgens) are similar units that are often
equated to the Rem.
51
From Understanding Radiation, Brooke Buddemeier, LLNL
Typical DosesTypical Doses
Average Dose to US Public from All sources 360 mrem/year
Average Dose to US Public From Natural Sources 300 mrem/year
Average Dose to US Public From Medical Uses 53 mrem/year
Coal Burning Power Plant 0.2 mrem/year
Average dose to US Public from Weapons Fallout < 1 mrem/year
Average Dose to US Public From Nuclear Power < 0.1 mrem/year
Occupational Dose Limit for Radiation Workers 5,000 mrem/yr
Coast to coast Airplane roundtrip 5 mrem
Chest X ray 8 mrem
Dental X ray 10 mrem
Head/neck X ray 20 mrem
Shoe Fitting Fluoroscope (not in use now) 170 mrem
CT (head and body) 1,100 mrem
Therapeutic thyroid treatment (dose to the whole
52
From Understanding Radiation, Brooke Buddemeier, LLNL
Types of Exposure & Health EffectsTypes of Exposure & Health Effects
• Acute Dose
– Large radiation dose in a short period of time
– Large doses may result in observable health effects
• Early: Nausea & vomiting
• Hair loss, fatigue, & medical complications
• Burns and wounds heal slowly
– Examples: medical exposures and
accidental exposure to sealed sources
• Chronic Dose
– Radiation dose received over a long period of time
– Body more easily repairs damage from chronic doses
– Does not usually result in observable effects
– Examples: Background Radiation and
Internal Deposition
53
Inhalation
From Understanding Radiation, Brooke Buddemeier, LLNL
Dividing Cells are the MostDividing Cells are the Most
RadiosensitiveRadiosensitive
• Rapidly dividing cells are more susceptible to
radiation damage.
• Examples of radiosensitive cells are
– Blood forming cells
– The intestinal lining
– Hair follicles
– A fetus
54
This is why the fetus has a exposure limit (over gestation period)
of 500 mrem (or 1/10th
of the annual adult limit)
From Understanding Radiation,Brooke Buddemeier, LLNL
At HIGH Doses, We KNOWAt HIGH Doses, We KNOW
Radiation Causes HarmRadiation Causes Harm
• High Dose effects seen in:
– Radium dial painters
– Early radiologists
– Atomic bomb survivors
– Populations near Chernobyl
– Medical treatments
– Criticality Accidents
• In addition to radiation sickness, increased cancer rates
were also evident from high level exposures.
55
From Understanding Radiation,Brooke Buddemeier, LLNL
Effects of ACUTE ExposuresEffects of ACUTE Exposures
Dose (Rads*) Effects
25-50
First sign of physical effects
(drop in white blood cell count)
100
Threshold for vomiting
(within a few hours of exposure)
320 - 360
~ 50% die within 60 days
(with minimal supportive care)
480 - 540
~50 % die within 60 days
(with supportive medical care)
1,000 ~ 100% die within 30 days
56
* For common external exposures 1 Rad ~ 1Rem = 1,000 mrem
From Understanding Radiation,Brooke Buddemeier, LLNL
At LOW Doses, We PRESUMEAt LOW Doses, We PRESUME
Radiation Causes HarmRadiation Causes Harm
• No physical effects have been observed
• Although somewhat controversial, this
increased risk of cancer is presumed to be
proportional to the dose (no matter how small).
The Bad News: Radiation is a carcinogen
and a mutagen
The Good News: Radiation is a very weak
carcinogen and mutagen!
Very Small DOSE = Very Small RISK
57
From Understanding Radiation
Brooke Buddemeier, LLNL
Radiation Detectors
58
Range of Radiation
Alpha: Small. Shield with a piece of paper
Beta: Smallish Shield with a ½ inch or so of Pb
Gamma: Long Shield with a few inches of Pb
Neutron: Very long Shield with many inches of parafin
To detect the radiation it has to
a) Get to and b) Get into your detector
Radiation Detectors
59
Almost all work on the same general idea
When an energetic charged particle passes through matter it will
rapidly slow down and lose its energy by interacting with the
atoms of the material (detector or body)
•Mostly with the atomic electrons
It will ‘kick’ these electrons off of the atoms leaving a trail of
ionized atoms behind it (like a vapor trail of a jet plane)
Radiation detectors use a high voltage and some electronics to
measure these vapor trails. They measure a (small) electric
current).
Radiation Detectors
60
Like a bullet going through something
A friction force will slow it down and stop it
Friction
More Charge  More friction
More Massive  More friction
More friction  Shorter Range
Radiation Detectors
61
It has to get into your detector
e.g. Alpha …. A few inches of air or a piece of paper
stops it … if your detector is a few feet away, it will not
detect the alpha …
e.g. Alpha … if the sides of the detector are too thick the
alpha will not get in and will not be detected
Radiation Detectors
62
Neutrons and gamma-rays are neutral
No charge … much less friction … much longer range
When they penetrate matter eventually they also will interact
somehow (gamma-rays interact via Compton scattering,
photoelectic effect or pair production, neutrons will collide with
protons in the nuclei) and these interactions produce energetic
charged particles.
The detectors are sensitive to these secondary particles.
Types of detector
63
Alpha, Beta and Gamma radiation
Film Badges
Gas Counters (Geiger counters)
Scintillators
Solid State Detectors
Film Badges
64
Will detect: beta, gamma and neutron
Need to send away and develop the film and then later will tell
you what does you received
Used by radiation workers
TLC devices … similar idea but with real-time readout
Gas Counters
65
e.g. Geiger Counters
Will Detect: Alpha, Beta, some gamma
No identification … just tells you something is there
With a thin entrance window GM-tube is sensitive to alphas
Scintillators
66
Make a flash of light when something interacts
Sodium Iodide
Cesium Iodide
Will Detect: Alpha (with thin window), beta (with thin window)
and gamma.
Gives moderate to bad energy information … some information
on the type of radiation
Semiconductor Detectors
67
Germanium
Silicon
Will Detect: Gamma rays (also beta and alphas in a
laboratory, not in the field)
Excellent energy resolution: Can measure exactly was source
you are looking at.
Spare Transparencies
68
Radioactive Decay
69
When can a nucleus decay? …
•When there is a lighter nucleus for it to decay into
•When this decay is allowed by certain conservation laws ….
•Conservation of energy
•Conservation of charge
•Certain other ‘quantum numbers’
When a physical process can
happen … it will happen.
When it is forbidden to happen
… it just takes a little longer!
If a nucleus can decay
… it will
Beta Decay
70
Various laws must be obeyed, including
1. Conservation of Energy
• E = mc2
… a heavy particle can decay into
lighter one(s).
• The excess energy is turned into kinetic
energy of the light particles
2. Conservation of Charge
• An electron is produced
3. Conservation of Lepton Number
• a very nebulous particle called a neutrino is
also produced
n  p + e-
+ ν

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Lecture1 cwb

  • 1. 1 Nuclear Physics and Society Physics Department University of Richmond Nuclear Basics
  • 2. Motivation: Educate the Public and University communities about basic nuclear physics ideas and issues 2 U.S. Department of Energy Workshop July 2002, Washington D.C. Role of the Nuclear Physics Research Community (universities and national laboratories) in Combating Terrorism Education and Outreach •Community •Local PD and FD
  • 3. DOE Workshop … 3 Border Control/ US Customs •1,000,000 visas/year •422 ports of entry •1700 flights / day •290 ships / day •60 trains / day •1200 busses / day •540,000,000 border entries / year Time per primary inspection 8 seconds => 1 hour delay Cargo Containers 10,000,000 per year … 10,000 per ship! 5 / minute @ L.A. < 3% inspected
  • 4. What the Course is/is not 4 This is not a radiation workers course This is not a course that will certify you for anything We hope that we can introduce you to some basic facts about nuclear physics, about radiation, about detectors etc., which may be useful for you to know.
  • 5. Who are We 5 Con Beausang Chairman & Associate Professor Physics Department Jerry Gilfoyle Professor, Physics Department Paddy Regan Professor Physics Department, University of Surrey, U.K.
  • 6. 6 Monday April 13th Lecture 1: The types of radiation, their properties and how these can be used to detect them. Some basic definitions. Introduction to radiation detectors. Tuesday April 14th Laboratory Session: 12:15  3:30 pm Environmental Radiation Laboratory experience Measurement of half-life Demonstration of shielding Find the source Lecture 2: The creation of the elements. Nuclear physics in the cosmos. Wednesday April 15th Laboratory Session 2: 12:15  3:30 Repeat of Tuesdays experience Lecture 3: Applications of Nuclear Physics: Nuclear weapons, nuclear power and nuclear medicine. Thursday April 16th Lecture 4 Some of the frontiers of modern nuclear physics research Nuclear Physics and Society
  • 8. 8 The Cookie Quiz Alpha cookie Beta cookie Gamma cookie Neutron cookie Throw away Put in pocket Hold in clenched fist Eat one … GOAL: Minimize your radiation exposure
  • 9. 9 The Cookie Quiz: Answer 1 Alpha cookie Beta cookie Gamma cookie Neutron cookieThrow away Put in pocket Hold in clenched fist Eat one …
  • 10. 10 The Cookie Quiz: Correct Answer Alpha cookie Beta cookie Gamma cookie Neutron cookie Throw away Put in pocket Hold in clenched fist Eat one … GOAL: Minimize your radiation exposure Mutiny at once Retire from the navy and Toss ALL cookies away
  • 11. … when I was young(er), I was curious … What are we made of ? … sugar and spice and all things nice … that’s what little girls are made of … snips and snails and puppy dogs tails … that’s what little boys are made of. … ok mum, … so what are sugar, spice and snails etc. made of? … cells … molecules … atoms … nuclei
  • 12. The Uncertainty Principle Heisenberg (Quantum Mechanics) ∆(position) ∆(momentum) > Constant Beausang (Teaching) ∆(truth) ∆(clarity) > Constant
  • 13. Atoms … are made of … Electrons … very light, but occupy most of the volume inside an atom Nuclei … lie at the Core of Atoms … very heavy, very small, very compact …occupies almost none of the volume inside the atom
  • 14. How do we know? How to see the invisible? … size of your probe … scattering Alpha-particle beam Detector Zinc-sulfide screen Discovery of the nucleus ~1910 The eyes of Geiger and Marsden 16-inch Battleship shells and tissue paper
  • 15. Think of atoms as being like a mini solar system … The sun at the center is the nucleus, the electrons orbit the nucleus, like the planets orbit around the sun Bohr Model
  • 16. Electrons •Very small •Point-like particles (i.e.nothing inside an electron) •Very light ~ 1/2000th of proton mass •Negatively charged (-1 elementary charge) •Electrons occupy almost all the space in the atom (orbiting the nucleus like the earth and other planets orbit the sun) •Have almost none of the mass of the atom •All of chemistry has to do with electrons from different atoms interacting with each other
  • 17. The Nucleus •Made up of protons and neutrons •Almost all of the mass of the atom is concentrated in the nucleus. • >99.9% of the known mass in the universe. •Occupies almost none of the volume of the atom. •Radius < 1/10,000 •Volume < 1/1,000,000,000,000
  • 18. •The nucleus is the source of almost all the things we commonly think of as being radioactive.
  • 19. The Nucleus Protons •Positively charged (+1 elementary charge) •Size ~ 1 fm (10-15 m) •Mass 938 MeV/c2 = 1 Neutrons •Neutral (0 charge) •Size ~ 1 fm (10-15 m) •Mass 939 MeV/c2 ~ 1 Neutrons are slightly more massive than the protons!!! This has huge consequences for us!
  • 20. Delicate Balances Laws of Physics 1) If it can happen … it will happen … 2) If some law forbids it to happen … it will happen more slowly … 3) If a process is really REALLY forbidden to happen … it just takes a long time …
  • 21. Standard Model: Neutron and proton are very close relatives quark structure … proton (uud) … neutron (udd) Many laws allow neutrons to `change into’ into protons … change a d-quark into a u- quark (or vice versa) … beta-decay
  • 22. The half life of a free neutron (i.e., one not inside a nucleus) is only about 12 minutes!!! Mass Neutron = 939.565330 MeV/c2 Mass Proton = 938.271998 MeV/c2 But … Inside a nucleus … neutrons are stable The half life of a free proton is > 1031 years Inside some nuclei protons can ‘decay’ into neutrons Imagine … if they were not! Then in ~ 1-2 hours the entire universe would be made of Hydrogen E = mc2
  • 23. The Nucleus •Atoms are electrically neutral •The number of protons in a nucleus is equal to and determines the number of orbiting electrons the chemistry the element name •Hydrogen (1 1H) 1 proton, 0 neutrons Mass = 1 •Helium (4 2He) (Alpha-particle) 2 protons, 2 neutrons Mass = 4 •Uranium (238 92U) 92 protons, 146 neutrons Mass = 238
  • 24. The Nucleus Many elements have several stable nuclei with the same number of protons but different numbers of neutrons … same name same chemistry different mass Isotopes
  • 25. The Periodic Table of the Elements
  • 26. Chart of the Nuclei 1 H 2 D 3 He 4 He 6 Li 7 Li n 9 Be 3 T 5 He 6 He 5 Li 6 Be 7 Be 8 Be 8 Li 7 He 9 Li 10 Be 10 Li 11 Li 8 He 9 He 11 Be 12 Be 10 B 11 B9 B 14 Be 12 B 13 B 14 B 15 B8 B7 B 12 C 13 C 14 C 15 C 16 C 17 C11 C10 C9 C8 C Z=No.ofProtons 0 1 2 3 4 5 6 N = No. of Neutrons 0 1 2 3 4 5 6 7 8 9
  • 27. Chart of the Nuclei The Landscape ~300 stable ~ 7000 unstable … radioactive.
  • 28. Half Life 28 Time taken for half of the substance to decay away Example: If you have 1000 radioactive nuclei and If their half life is 30 minutes After 30 minutes 500 nuclei remain After 60 minutes 250 remain After 90 minutes 125 remain After 120 minutes 62 remain There is a huge variation in half lives of different isotopes …. From a tiny fraction of a second to roughly the age of the universe.
  • 29. Some Isotopes & Their Half LivesSome Isotopes & Their Half Lives ISOTOPEISOTOPE HALF-HALF- LIFELIFE APPLICATIONSAPPLICATIONS Uranium billions of years Natural uranium is comprised of several different isotopes. When enriched in the isotope of U-235, it’s used to power nuclear reactor or nuclear weapons. Carbon-14 5730 y Found in nature from cosmic interactions, used to “carbon date” items and as radiolabel for detection of tumors. Cesium-137 30.2 y Blood irradiators, tumor treatment through external exposure. Also used for industrial radiography. Hydrogen-3 12.3 y Labeling biological tracers. Irridium-192 74 d Implants or "seeds" for treatment of cancer. Also used for industrial radiography. Molybdenum-99 66 h Parent for Tc-99m generator. Technicium-99m 6 h Brain, heart, liver (gastoenterology), lungs, bones, thyroid, and kidney imaging, regional cerebral blood flow, etc. 29
  • 30. The Amount of Radioactivity isThe Amount of Radioactivity is NOT Necessarily Related to SizeNOT Necessarily Related to Size • Specific activity is the amount of radioactivity found in a gram of material. • Radioactive material with long half- lives have low specific activity. 1 gram of Cobalt-60 has the same activity as 1800 tons of natural Uranium 30
  • 31. 31 For Example: Suppose we have 1,000,000,000 atoms of material A with a half life of 1 second and 1,000,000,000 atoms of material B with a half life of 1 year (real sources have many more atoms in them) Suppose they both decay by alpha emission. In the First Second Substance A: Half the nuclei will decay … 500,000,000 alpha particles will come zipping out at you. 1 year = 365 days * 24 hours * 60 minutes * 60 seconds = 31,536,000 seconds In the First Second for substance B Only ~ 500,000,000 / 31,536,000 = 16 nuclei will decay … only 16 alpha particles will come zipping at you
  • 32. 32 On the other hand … In 10 seconds … almost all of the radioactivity in substance A is gone away But it takes years for the activity of substance B to go away! Nuclear Bombs … The fissile material (U or Pu) has a long half-life. Low specific activity. Not much activity on the outside. Dirty Bombs … The radioactive material wrapped around the explosive would probably have a much shorter half-life. Perhaps significant activity on the outside.
  • 33. Types of Radioactivity 33 Each type of radiation has different properties which affect the hazards they pose, the detection mechanism and the shielding required to stop them. Five Common Types Alpha Decay Beta Decay Gamma Decay Fission Neutron Emission Each of the particles emitted in the decay carries a lot of kinetic energy. Damage can be caused when this energy is absorbed in a human cell.
  • 34. Alpha Decay 34 An alpha particle (α) is an energetic, He nucleus (4 2He2) Alpha decay mostly occurs for heavy nuclei Example 238 94Pu  234 92U + 4 2He Half-life: 88 years Energy α =5.56 MeV
  • 35. Alpha Decay 35 Very easy to shield A sheet of paper, skin, or a few cm (~inch) of air will stop an alpha particle External Hazard: Low Internal Hazard: High
  • 36. Alpha Decay 238 94Pu144 234 92U142 + α • Parent nucleus 238 94Pu144 • Daughter Nucleus 234 92U142 –Often the daughter nucleus is also radioactive and will itself subsequently decay. –Decay chains or families (e.g. uranium, thorium decay chains). 36
  • 37. Decay Chains 37 238 94Pu  234 92U + α t1/2 = 88 yrs 234 92U  230 90Th + α t1/2 = 2.5 105 yrs 230 90Th  226 88Ra + α t1/2 = 8.0 104 yrs 226 88Ra  222 86Rn + α t1/2 = 1.6 103 yrs 222 86Rn  218 84Po + α t1/2 = 3.8 days 218 84Po  214 82Pb + α t1/2 = 3.1 min 214 82Pb  214 83Bi + β t1/2 = 27 min 214 83Bi  214 84Po + β t1/2 = 20 min 214 84Po  210 82Pb + α t1/2 = 160 µs
  • 38. Decay Chains 38 210 82Pb  210 83Bi + β t1/2 = 22 yrs 210 83Bi  210 84Po + β t1/2 = 5 days 210 84Po  206 82Pb + α t1/2 = 138 days 206 82Pb is STABLE
  • 40. Beta Decay • The neutron and the proton are very similar to each other (very closely related). • A neutron can ‘change into’ a proton, or vice versa. • When this happens, an energetic electron (or positron) is emitted. • This is called beta-decay 40 A beta-particle is an electron (e) or its anti-particle the positron (e+ ) n  p + e- + ν p  n + e+ + ν
  • 41. Beta Decay 41 In terms of nuclei beta-decay looks like As in the case of alpha decay the daughter nuclei are usually radioactive and will themselves decay. •Beta-particles are HARDER to stop Since the electron is lighter than an alpha-particle and carries less charge. •Therefore, the range of a beta-particle is greater and it 137 55Cs82  137 56Ba81 + e- + ν
  • 42. Beta-Decay 42 •Beta-particles are HARDER to stop Since the electron is lighter than an alpha- particle and carries less charge. •Therefore, the range of a beta-particle is greater and it takes more shielding to stop beta-particles (electrons or positrons) than alpha particles ~ few mm or 1 cm of lead ~ few feet of air
  • 43. Gamma-Decay 43 •A beta-decay or alpha-decay typically leaves the daughter nucleus in a highly excited state. •To get to the ground state the nucleus (rapidly … almost instantly) emits one or more gamma-rays •Gamma-rays are a very energetic form of light. More energy and more penetrating than x-rays. •No charge •Much more penetrating than either alpha or beta. •Few inches of Pb, many feet of air
  • 44. Gamma-Decay 44 •Gamma-ray energies are characteristic of the nucleus. •Measure the energies … identify the nucleus. (just like atoms or molecules give off characteristic colors of light). Measuring the gamma-ray is by far the best and easiest way to measure what type of radioactive substance you are dealing with.
  • 45. Fission 45 What holds nuclei together? •Protons repel each other (opposites attract, like repel) •Coulomb Force Some other force must hold nuclei together The STRONG FORCE •Attractive and Stronger than the Coulomb Force •But short range
  • 46. Fission 46 What happens if you have a lot of protons (i.e in a heavy nucleus)? …Eventually the Coulomb repulsion will win … and the nucleus will fall apart into two smaller (radioactive!!) nuclei. FISSION An enormous amount of energy is released. This energy is utilized in power plants and in fission bombs.
  • 47. Fission 47 The heavy parent nucleus fissions … into two lighter fission fragment nuclei … Plus some left over bits … energetic neutrons Example: 252 Cf is a spontaneous fission source … Sometimes this process happens spontaneously … sometimes you can ‘poke’ at the nucleus and induce it to fission
  • 48. Fission …Fission Fragments 48 Are emitted with a huge energy but stop very quickly (very short range). Are all radioactive nuclei and will decay usually by beta-and gamma-decay Mass  Probability Heavy fragment Light fragment They have a broad range of masses
  • 49. Induced Fission 49 Some nuclei can be made to fission when struck by something … Usually the something is a neutron Example: 235 U + n  fission Remember … in the fission process extra neutrons are released If some of these strike other 235 U nuclei … they can induce another fission
  • 50. Induced Fission 50 Chain Reaction Controlled … nuclear power plant … exactly one neutron per fission induces another fission. Uncontrolled … nuclear bomb … more than one neutron per reaction induces another fission
  • 51. What is a “Dose” of Radiation?What is a “Dose” of Radiation? • When radiation’s energy is deposited into our body’s tissues, that is a dose of radiation. • The more energy deposited into the body, the higher the dose. • Rem is a unit of measure for radiation dose. • Small doses expressed in mrem = 1/1000 rem. • Rad & R (Roentgens) are similar units that are often equated to the Rem. 51 From Understanding Radiation, Brooke Buddemeier, LLNL
  • 52. Typical DosesTypical Doses Average Dose to US Public from All sources 360 mrem/year Average Dose to US Public From Natural Sources 300 mrem/year Average Dose to US Public From Medical Uses 53 mrem/year Coal Burning Power Plant 0.2 mrem/year Average dose to US Public from Weapons Fallout < 1 mrem/year Average Dose to US Public From Nuclear Power < 0.1 mrem/year Occupational Dose Limit for Radiation Workers 5,000 mrem/yr Coast to coast Airplane roundtrip 5 mrem Chest X ray 8 mrem Dental X ray 10 mrem Head/neck X ray 20 mrem Shoe Fitting Fluoroscope (not in use now) 170 mrem CT (head and body) 1,100 mrem Therapeutic thyroid treatment (dose to the whole 52 From Understanding Radiation, Brooke Buddemeier, LLNL
  • 53. Types of Exposure & Health EffectsTypes of Exposure & Health Effects • Acute Dose – Large radiation dose in a short period of time – Large doses may result in observable health effects • Early: Nausea & vomiting • Hair loss, fatigue, & medical complications • Burns and wounds heal slowly – Examples: medical exposures and accidental exposure to sealed sources • Chronic Dose – Radiation dose received over a long period of time – Body more easily repairs damage from chronic doses – Does not usually result in observable effects – Examples: Background Radiation and Internal Deposition 53 Inhalation From Understanding Radiation, Brooke Buddemeier, LLNL
  • 54. Dividing Cells are the MostDividing Cells are the Most RadiosensitiveRadiosensitive • Rapidly dividing cells are more susceptible to radiation damage. • Examples of radiosensitive cells are – Blood forming cells – The intestinal lining – Hair follicles – A fetus 54 This is why the fetus has a exposure limit (over gestation period) of 500 mrem (or 1/10th of the annual adult limit) From Understanding Radiation,Brooke Buddemeier, LLNL
  • 55. At HIGH Doses, We KNOWAt HIGH Doses, We KNOW Radiation Causes HarmRadiation Causes Harm • High Dose effects seen in: – Radium dial painters – Early radiologists – Atomic bomb survivors – Populations near Chernobyl – Medical treatments – Criticality Accidents • In addition to radiation sickness, increased cancer rates were also evident from high level exposures. 55 From Understanding Radiation,Brooke Buddemeier, LLNL
  • 56. Effects of ACUTE ExposuresEffects of ACUTE Exposures Dose (Rads*) Effects 25-50 First sign of physical effects (drop in white blood cell count) 100 Threshold for vomiting (within a few hours of exposure) 320 - 360 ~ 50% die within 60 days (with minimal supportive care) 480 - 540 ~50 % die within 60 days (with supportive medical care) 1,000 ~ 100% die within 30 days 56 * For common external exposures 1 Rad ~ 1Rem = 1,000 mrem From Understanding Radiation,Brooke Buddemeier, LLNL
  • 57. At LOW Doses, We PRESUMEAt LOW Doses, We PRESUME Radiation Causes HarmRadiation Causes Harm • No physical effects have been observed • Although somewhat controversial, this increased risk of cancer is presumed to be proportional to the dose (no matter how small). The Bad News: Radiation is a carcinogen and a mutagen The Good News: Radiation is a very weak carcinogen and mutagen! Very Small DOSE = Very Small RISK 57 From Understanding Radiation Brooke Buddemeier, LLNL
  • 58. Radiation Detectors 58 Range of Radiation Alpha: Small. Shield with a piece of paper Beta: Smallish Shield with a ½ inch or so of Pb Gamma: Long Shield with a few inches of Pb Neutron: Very long Shield with many inches of parafin To detect the radiation it has to a) Get to and b) Get into your detector
  • 59. Radiation Detectors 59 Almost all work on the same general idea When an energetic charged particle passes through matter it will rapidly slow down and lose its energy by interacting with the atoms of the material (detector or body) •Mostly with the atomic electrons It will ‘kick’ these electrons off of the atoms leaving a trail of ionized atoms behind it (like a vapor trail of a jet plane) Radiation detectors use a high voltage and some electronics to measure these vapor trails. They measure a (small) electric current).
  • 60. Radiation Detectors 60 Like a bullet going through something A friction force will slow it down and stop it Friction More Charge  More friction More Massive  More friction More friction  Shorter Range
  • 61. Radiation Detectors 61 It has to get into your detector e.g. Alpha …. A few inches of air or a piece of paper stops it … if your detector is a few feet away, it will not detect the alpha … e.g. Alpha … if the sides of the detector are too thick the alpha will not get in and will not be detected
  • 62. Radiation Detectors 62 Neutrons and gamma-rays are neutral No charge … much less friction … much longer range When they penetrate matter eventually they also will interact somehow (gamma-rays interact via Compton scattering, photoelectic effect or pair production, neutrons will collide with protons in the nuclei) and these interactions produce energetic charged particles. The detectors are sensitive to these secondary particles.
  • 63. Types of detector 63 Alpha, Beta and Gamma radiation Film Badges Gas Counters (Geiger counters) Scintillators Solid State Detectors
  • 64. Film Badges 64 Will detect: beta, gamma and neutron Need to send away and develop the film and then later will tell you what does you received Used by radiation workers TLC devices … similar idea but with real-time readout
  • 65. Gas Counters 65 e.g. Geiger Counters Will Detect: Alpha, Beta, some gamma No identification … just tells you something is there With a thin entrance window GM-tube is sensitive to alphas
  • 66. Scintillators 66 Make a flash of light when something interacts Sodium Iodide Cesium Iodide Will Detect: Alpha (with thin window), beta (with thin window) and gamma. Gives moderate to bad energy information … some information on the type of radiation
  • 67. Semiconductor Detectors 67 Germanium Silicon Will Detect: Gamma rays (also beta and alphas in a laboratory, not in the field) Excellent energy resolution: Can measure exactly was source you are looking at.
  • 69. Radioactive Decay 69 When can a nucleus decay? … •When there is a lighter nucleus for it to decay into •When this decay is allowed by certain conservation laws …. •Conservation of energy •Conservation of charge •Certain other ‘quantum numbers’ When a physical process can happen … it will happen. When it is forbidden to happen … it just takes a little longer! If a nucleus can decay … it will
  • 70. Beta Decay 70 Various laws must be obeyed, including 1. Conservation of Energy • E = mc2 … a heavy particle can decay into lighter one(s). • The excess energy is turned into kinetic energy of the light particles 2. Conservation of Charge • An electron is produced 3. Conservation of Lepton Number • a very nebulous particle called a neutrino is also produced n  p + e- + ν

Editor's Notes

  1. Here are some notes
  2. Narrative Here are some examples of radioactive isotopes commonly used in industry. {Read slide it time permits} ----------------------note: this slide can be removed for an overview
  3. Narrative You can’t judge how much radiation is being produced based on the physical size of the source. Radioactive material with long half-lives, meaning it decays away slowly, will not give off a lot of radiation per unit mass. This is referred to as the isotope’s Specific Activity. For isotopes like Cobalt-60, which only has a half life of a few years, a gram of Co-60 has the same activity (number of decays per minute) are almost two thousand tons of uranium.
  4. Lecture: Read slide ============================== Remove This Slide for an Overview presentation
  5. Narrative: Here are some examples of typical doses received by people. On Average, people in the US get about 360 mrem per year. Most of this, 300 mrem, is from “natural” sources such as the uranium in the ground and cosmic radiation from outer space. The second biggest contributor to our annual dose is medical use of radiation. If you can read this slide, you may notice that a Coal Burning power plant gives more dose to the public than nuclear power. This isn’t a type-O; Coal, oil, and natural gas all come from the ground and have trace quantities of uranium in them. When we burn this material in our powerplants and homes, the radioactive material exposes us when it is released in the exhaust, in addition to the greenhouse gasses and ash. Although Nuclear Power generates a lot more radioactive material, when everything goes as planned, it is contained in the spent fuel. No greenhouse gasses either. Highlighted in yellow is the annual occupational exposure limit of 5,000 mrem. I’ve also listed the doses you might get from a few events, such as flying across the country, which leads to a 5 mrem cosmic radiation dose, and some common medical procedures. ============================ Remove This Slide for an Overview presentation
  6. Suggested narrative: The types of radiation exposures that hurt us the most are Large Doses delivered over a short period of time. These types of exposures overwhelm our body’s repair mechanisms. These are referred to a ACUTE exposures or doses Pictured in that person’s hand is a dummy industrial radiography source. At least I hope it’s a dummy source, otherwise holding a source like that for a minute or two can cause painful burns and wounds that refuse to heal. In contrast, a CHRONIC exposure is one that is received over a long period, allowing the body to more effectively manage the effects. ===========Notes======================== Consider a (small) 30 Ci 192Ir radiography source. Surface dose = 36,000 rad/min at 1 cm - dose rate=2400 rad/min at 2 cm - dose rate = 600 rad/min at 3 cm - dose rate=267 rad/min at 4 cm - dose rate=150 rad/min at 5 cm - dose rate=96 rad/min Early: Nausea &amp; vomiting =&amp;gt; Usually happens within a few hours of large (&amp;gt; 100 rad) exposures. The higher the dose, the sooner and more severe the symptom. Burns and wounds heal slowly =&amp;gt; For localized exposures, burns and tissue necrosis. Hair loss, Fatigue, &amp; medical complications =&amp;gt; Dose (rads)Effects 25-50First sign of physical effects (drop in white blood cell count) 100Threshold for vomiting (within a few hours of exposure) 320 - 360~ 50% die within 60 days (with minimal supportive care) 480 - 540~50 % die within 60 days (with supportive medical care) 1,000~ 100% die within 30 days
  7. Suggested narrative: When cells are dividing (or undergoing mitosis) they are more susceptible to radiation damage because the cells don’t have their full suite of repair mechanisms. Because of this, cells that are often dividing like The cells that create our blood or line our intestine, also Hair follicles, and, of course, fetal cells are more susceptible to radiation damage. This is why the fetus has a exposure limit (over gestation period) of 500 mrem (or 1/10th of the annual adult limit) Specialized or slowly dividing cells, like brain cells are radio-insensitive. Credit: The vedio (and voiceover) was Excerpted from DOE’s Transportation Emergency Preparedness Program (TEPP) http://www.em.doe.gov/otem/program.html
  8. Narrative The Picture of woman using fluoroscope. Just off the picture to the right is the business end on an X-ray machine beaming toward her face. The beam hits the phosphors on the back of the “telescope” and she can she her hand as an X-ray and watch it move…. She also gets a whopping dose to the face! Throughout this century, people have been exposed to radiation. Some through accident or ignorance; others, like the atomic bomb survivors or medical patients, where exposed intentionally. Extensive data has been collected on these exposures in an attempt to understand more about it’s effects. At high doses of radiation, we know there are physical effects such as burns, radiation sickness and even death. Another observed effect of high doses of radiation is a detectable increase in certain cancer rates. Not a sure thing, but rather a slight increase over the natural incidence of cancer for large exposures.
  9. Narrative As we start talking about large doses, please note that I’ve changed the units on you. I’m now using RADs instead of mrem. It takes 1000 mrem to equal 1 rem which is about the same as a rad. For example, using the mrem units we talked about before, it would take 25,000 to 50,000 mrem to see any kind of physical effects in humans. Effects that we would not even feel, but a blood test could reveal due to the lower white blood cell count. =============== notes ============ Remove This Slide for an Overview presentation A Good source of information on Acute Effects of Radiation can be found on: http://radefx.bcm.tmc.edu/ionizing/subject/risk/acute.htm
  10. Narrative: Read the slide Verbally mention that the LNT theory is done for conservatism ============ Additional Info ------------ Rule of thumb: Every 1 rem of dose increase risk by 0.08%