lecture 11 - nassau community college 152/152 lecture 1… · · 2012-05-23homer trapped in the...
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Copyright © 2009 Charles Hicks
Lecture 11Professor Hicks
Inorganic Chemistry (CHE152)
Copyright © 2009 Charles Hicks
Radioactive decays are all
first order processes
Copyright © 2009 Charles Hicks
Half-Lives of Various Nuclides
Nuclide Half-LifeType of
Decay
Th-232 1.4 x 1010 yr alpha
U-238 4.5 x 109 yr alpha
C-14 5730 yr beta
Rn-220 55.6 sec alpha
Th-219 1.05 x 10–6 sec alpha
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Copyright © 2009 Charles Hicks
Copyright © 2009 Charles Hicks
Carbon-14 dating
Earth
Earth’s atmosphere
space
cosmic radiation promotes
Transmutation
of nitrogen-14 to carbon-14
N +147 n1
0 C +146 p1
1
CO2146
photosynthesisC6H12O6
(sugar)
donuts
study the slides on
C-14 for their content
Copyright © 2009 Charles Hicks
Carbon-14 dating
Earth
Earth’s atmosphere
space
eating the donuts makes
Homer slightly radioactive
Rest in
Peace
when Homer dies he stops replenishing the
carbon-14 in his body and the amount that
is there starts to decay
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Copyright © 2009 Charles Hicks
Carbon-14 dating
• almost all life is part of the same food chain
• plants make sugars
• animals eat plants
• animals eat animals
• %carbon-14 is constant for an organism constantly taking in food
• when they die they stop replenishing carbon-14 and the clock on its decay starts
• t ½ = 5730 years
• [14C] = [14C]initiale-kt
• useful for dating 1000-50,000 years
Copyright © 2009 Charles Hicks
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Carbon-14 dating% C-14 (compared to living
organism)Object’s Age (in years)
100% 0
90% 870
80% 1850
60% 4220
50% 5730
40% 7580
25% 11,500
10% 19,000
5% 24,800
1% 38,100
Copyright © 2009 Charles Hicks
Kinetics of radioactive decay
• first order process
• [Uranium-238] = [Uranium-238]initiale-kt
• [ ]’s can be replaced with any quantity that
proportional to the amount of element:
mass, moles, volume under constant T, P,
or rate of radiation emission
• Shorter half-lifemore decay per second
- we say the sample is hotter and in many
cases it is at higher temperature
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Example: An ancient skull gives 4.50 particles/min∙gC. If a
living organism gives 15.3 particles/min∙gC, how old is the
skull?
= e-kt
1
2
[C-14]
[C-14]initial
= e-kt1/2
(4.5/15) = e -0.0001209*t
1
2= e-k*5730
k = 1.209 x 10-4 yr-1
= 0.0001209 yr-1
ln(1/2) = -k*5730
t = 9958 yr
1) use half-life t½ to find k 2) use the k value to solve for t
use ratio of rates of particle
emission instead of ratio of [ ]’s
Copyright © 2009 Charles Hicks
Copyright © 2009 Charles Hicks
Mass Defect and
Binding Energy
• when a nucleus forms, some of the mass of the
separate nucleons is converted into energy
• the difference in mass between the separate
nucleons and the combined nucleus is called the
mass defect
• the energy that is released when the nucleus
forms is called the binding energy
E = mc2
Albert Einstein Lise MeitnerLise Meitner
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Copyright © 2009 Charles Hicks
homer on the
earth’s surface
separated protons, neutrons
homer trapped in the well b/c he
does not have energy to escape
heat
released
heat
released
binding energy = heat released when nucleus forms
it comes from mass energy
binding
energy=
carbon-12
nucleus
+
+
+ N
N
N
+
+
+ N
N
N
+ +
+
+
+
N
N
N
N
N
N
+N
mass
energy
total mass =
12.000000 amu
12.0984 amu
total mass
6 1.00866
+ 6 1.00783
E = mc2
c = speed light
m = mass defect
0.0984 amu here
E = binding energy
Copyright © 2009 Charles Hicks
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• compare elements binding energy per nucleon
• Iron-56 has the most stable nucleus
• energy will be released when:
Copyright © 2009 Charles Hicks
Calculate the amount of energy released
when a helium-4 nucleus is formed from
two protons and two neutrons. This is also
referred to as the binding energy of a
helium-4 nucleus.
Mass He-4 = 4.00150
Mass Neutron = 1.00866
Mass proton = 1.00728
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Copyright © 2009 Charles Hicks
Fission/Fusion• a few nuclei are so unstable that
if their nucleus is hit by a neutron, the large nucleus splits into two smaller nuclei - this is called fission
• small nuclei can be smashed together to make a larger nucleus - this is called fusion
• both fission and fusion release enormous amounts of energy– fusion releases more energy per
gram than fission
Lise Meitner
Copyright © 2009 Charles Hicks
Fission
Copyright © 2009 Charles Hicks
where does the energy from
fission/fusion come from?
• during nuclear fission, mass is converted into energy as a more stable nucleus forms
• the energy can be calculated from E=mc2
• U-235 that undergoes fission produces about 1.7 x 1013 J per mole
– a very exothermic chemical reaction produces around 106 J per mole
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Copyright © 2009 Charles Hicks
Fission Chain Reaction• a chain reaction occurs when a reactant in
the process is also a product of the process
– in fission it is neutrons
– small amount of neutrons start the chain
• many of the neutrons produced in fission are
either ejected from the uranium before they
hit another U-235 or are absorbed by the
surrounding U-238
• minimum amount of fissionable isotope
needed to sustain the chain reaction is called
the critical mass
Copyright © 2009 Charles Hicks
if sample is very dilute most neutrons will escape
- they will not initiate another reaction
if sample is absorbing more than 1 neutron on the
average then the process will very rapidly accelerate
- this is called a Criticality Excursion
Copyright © 2009 Charles Hicks
Criticality excursions
• Samples that are undergoing fission, releasing
neutrons, can experience sudden accelerations
due to nuclear chain reactions
• Caused by
• Precipitations
• Neutrons reflected back
• Change in shape of container
• Powerful bursts of radiation emitted
All increase the number of
emitted neutrons that are
absorbed initiating the next
step of the chain reaction
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Copyright © 2009 Charles Hicks
Nuclear Power Plants - Core• fissionable material is stored in long tubes,
called fuel rods, arranged in a matrix
• between the fuel rods are control rods
made of neutron absorbing material
– B or Cd
– neutrons needed to sustain the chain reaction
• when the rods are lowered slow down
ejected neutrons, called a moderator
– allows rate of chain reaction to be controlled
Copyright © 2009 Charles Hicks
Nuclear Fusion
Copyright © 2009 Charles Hicks
Fusion
• potentially safer fuels than fission
H2
1H
3
1He
4
2n
1
0+ +
products not radioactive isotopes!tritium relatively safe
t ½ = 12 years
beta decay
problems
1) activation energy is high T ~ 108 K
2) hard to create/control high enough
temperatures
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Copyright © 2009 Charles Hicks
Fusion
Copyright © 2009 Charles Hicks
heat
released
overall
reaction
(heat absorbed)
Cold Fusion????
Copyright © 2009 Charles Hicks
Describe the effect of raising or lowering
the control rods in a nuclear fission reactor
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Copyright © 2009 Charles Hicks
Copyright © 2009 Charles Hicks
Estimate the energy released when 1.0 mole of Am-241
undergoes alpha decay.
Mass Am-241 = 241.00471 amu
Mass Np-237 = 236.99715 amu
Mass He-4 = 4.00150 amu
Compare the value you obtain to the amount of energy obtained
from combustion of 1 mole of octane 5.0 x106 J/mol
Copyright © 2009 Charles Hicks
Example: If you have a 1.35 mg sample of Pu-236,
calculate the mass that will remain after 5.00 years
Pu-236 has a half life of 2.86 yr
1) use half-life t½ to find k 2) use the k value and the t of interest
to solve for mass at that time
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Copyright © 2009 Charles Hicks
Blocking radiation
• An elements ability to block X-rays
increases with nuclear size (Z)
• Pb is often used as shielding because it is
almost the heaviest element that is not
radioactive itself
• Soft body tissue is mostly H2O, which is
mostly O-16 by mass
• Bone and cartilige contain substantial
amounts of Ca and P which are larger
nuclei absorb more radiation
Copyright © 2009 Charles Hicks
X-ray imaging• Medical x-rays are of the “shadows” of
denser body tissue – bones, cartilage, etc
X-ray
source
Copyright © 2009 Charles Hicks
CT Scans
• Series of x-rays used to construct a 3-
dimensional image
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Copyright © 2009 Charles Hicks
PET Scan
• imaging technique based on positron emission
positron + electron gamma rays
• isotope incorporated into a molecule
• molecule ingested
• positrons emitted from places molecule is concentrated
• gives a three dimensional “x-ray” of the region the molecule binds
• example F-18 labeled drugs that bind in the brain’s addiction centers
- F-18 labeled cocaine, heroine
Copyright © 2009 Charles Hicks
Barium
Enema
• radiation absorption increases with size of nucleus
• bones Ca, P causes them to absorb more than
soft tissue mostly H, O, C, N
• colon can be imaged with x-rays if it is filled with
BaSO4 because Ba absorbs X-rays well
Copyright © 2009 Charles Hicks
Radiation therapy
• Cancerous tumors dosed with radiation
• Can be performed with focused beams, or
• “seeding” radioactive material near the
tumor, or
• Molecules labeled with radioactive
isotopes that target specific organs
• Radiotherapy works by damaging the
DNA of the cancer cells
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Radiation therapy
External beam radiation therapy
• Cobalt-60 often used as a source of
radiation
• It is a beta emitter
• beam is focused on
the site of the tumor
Copyright © 2009 Charles Hicks
Radiation therapy
Internal radiotherapy• I naturally accumulates in the thyroid gland
• I-131 is radioactive and can be used to treat
thyroid cancer
• I-131 after being ingested a NaI-131
accumulates in thyroid where it undergoes -
decay dosing the thyroid cancer
Non-radioactive iodine is eaten to prevent damage to the
thyroid caused by I-131 released from nuclear bombs or
accidents
It works by flooding the body with I- so that most of the I-
at the thyroid gland is not radioactive
Copyright © 2009 Charles Hicks
Radiation therapy
Internal radiotherapy• Prostate cancer treated with radioactive seeds
• Palladium-103 is an example of a seed material
• It has t½ = 17 days
• decays by electron capture emitting gamma rays
Pd-103 seeds
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Copyright © 2009 Charles Hicks
Dangers of Radioactivity• high energy radioactive decay products called
Ionizing Radiation
• Ionizing radiation can directly cleave DNA
- called primary damage, or
- can break molecules up forming species that
cause damage by chemical reactions
- called secondary damage
• most common secondary pathway is water
absorbing radiation forming hydroxyl radicals
• radical = odd number of electrons
• Very reactive and an oxidizing agent
OH
Copyright © 2009 Charles Hicks
Relative Biological Effectiveness
(at causing damage)
Type and Energy Range Relative Biological Effectiveness
X and Gamma rays 1
Electrons 1
Neutrons (energy dependent) 10
Protons 5
Alpha Particles 20
you will be provided with this table on the exam
Copyright © 2009 Charles Hicks
Dose
• amount of energy absorbed in an exposure has a unit
called the gray (Gr)
1 gray =1 Joule
kg tissue
gray is a large unit for typical exposures
A more common unit is the Radiation Absorbed Dose (RAD)
0.01 gray = 1 RAD
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Copyright © 2009 Charles Hicks
REM’s
dose in REM = dose in RAD x RBE
• unit used to measure total risk associated with a dose
• accounts for differences in extent of damage caused
by different particle types
dose (REM) effect
5 none felt, yearly limit radiation workers
50 none felt, red blood cell count lowered
1000 near 100% fatal
• typical x-ray deliver 1-100 mREM
• background level is 30-60 mREM per year
• barium enema recently? you got 400 mREM
Copyright © 2009 Charles Hicks
Factors besides size of dose• Getting a dose in regions that are mostly
muscle (legs, arms) is much less dangerous
than the same dose in your organs
• Distributing a dose over time is much less
damaging
• Cells have repair mechanisms
• If repair can keep up much less damage can
accumulate
- DNA single strand breaks are repairable
- Double strand breaks – not very repairable
Copyright © 2009 Charles Hicks
Dangers of radiation and
penetrating power
• gamma radiation strongly penetrating requires thick layers of most protecting materials
• without protection dangerous doses quickly delivered
• and emitters easy to block
• and emitters very dangerous if ingested since they can deliver large doses accumulated over time
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Copyright © 2009 Charles Hicks
Why do beta emitters not have to be kept
in a thick-walled lead containers, but
precautions must be taken to prevent
ingesting them?
Copyright © 2009 Charles Hicks
Calculate how many REMs were delivered
in 10 barium enemas if the dose for each
barium enema is 0.40 RAD
Copyright © 2009 Charles Hicks
How many RAD of alpha particles could a
radiation worker be dosed with before they
reached their yearly safety limit of 5.0
REM?