Transcript Powerpoint - Missouri S&T

Radiochemistry
The purpose of this
experiment is
to use first-order nuclear
decay kinetics to determine
the half-life of a nuclear
reaction.
Where might we see radioactive materials in everyday life?
Nuclear Energy
Smoke Detectors
Americium-241
Smoke from a fire can be
detected at a very early stage
At a nuclear power station, water
vapor rises from the hyperboloid
shaped cooling towers. The
nuclear reactors are inside the
cylindrical containment buildings.
There is a reactor in Fulton, MO.
Where might we see radioactive materials in everyday life?
Agricultural applicationsradioactive traces
Helps scientists to understand the detailed
mechanism of how plants utilize
phosphorous to grow an reproduce
Food irradiation
Gamma rays of a radioisotopes
(Cobalt-61) destroy many diseasecausing bacteria as well as those that
cause food to spoil
But what is radioactivity?
Discovery of Radioactivity
In 1897, Becquerel
accidentally discovered
radioactivity in pitchblende
(a uranium mineral) while
studying sunlight induced
fluorescence of various
minerals. This mineral was
found to produce a
photographic image, even
through black paper.
Henri Antoine Becquerel
French Professor of Applied Physics
Nobel Prize in Physics 1903
(1852 – 1908)
Further experiments demonstrated that a mixture of charged
particles and electromagnetic radiation were being emitted
and were responsible for the effect on photographic film.
Radioactivity &
The Curies
 Studied radioactive materials,
particularly pitchblende, which
was more radioactive than the
uranium extracted from it.
Deduced (1898) the obvious
explanation:
Pitchblende must contain
traces of some unknown
radioactive component that was
far more radioactive than
uranium.
Pierre Curie – French Physicist
Nobel Prize in Physics – 1903
(May 15, 1859, – April 19, 1906)
Marie Sklodowska Curie
Polish/French Physicist & Chemist
Nobel Prize in Physics – 1903
Nobel Prize in Chemistry - 1911
(November 7, 1867 – July 4, 1934)
The Curies refined several tons of pitchblende (shown above)
progressively concentrating the radioactive components. Eventually
they isolated the chloride salts of the two new chemical elements, and
then the elements themselves.
The first they named polonium (Po) after Marie's native
country Poland; and, the other they named radium (Ra) from its
intense radioactivity.
Rutherford – The Father of Nuclear Physics
Pioneered the orbital theory of the
atom, in his discovery of
“Rutherford scattering” off the
nucleus with the gold foil experiment.
Demonstrated that radioactivity
was the spontaneous disintegration
of atoms.
First to note that in a sample of
radioactive material it invariably took
Ernst Rutherford
the same amount of time for half
Nuclear Physicist – New Zealand
the sample to decay, thus defining
Nobel Prize in Chemistry - 1908
(August 30, 1871 – October 19, 1937)
its “half-life”.
Rutherford’s Gold Foil Experiment
Implications of Radioactivity
 Radioactive materials undergoing nuclear decay
reactions violated the idea that atoms are the
unchanging, indivisible, ultimate building blocks
of matter.
 Additional experiments with cathode ray tubes,
accelerators and mass spectrometers eventually
showed atoms do consist of smaller components:
protons, neutrons, and electrons.
Some Important Terminology
Nuclear reactions involve the atomic
nucleus (i.e., protons and neutrons).
Regular chemical reactions involve only
the outer electrons of atoms.
An atom is the smallest entity that retains
the properties of an element.
Atoms are composed of one or more
electrons and a nucleus.
The nucleus is the central portion of an atom
and contains one or more protons and zero
or more neutrons.
Element = The simplest stable building blocks
of materials, consisting of protons, neutrons
and electrons.
Isotope = An atom of an element with the same
number of protons, but a different number
of neutrons.*
Radioisotope = An unstable isotope that
undergoes nuclear decay.
Radiochemistry = The study of radioisotopes.
*Note:
Atomic weights given on the periodic table are the
weighted average of all the natural isotopes of each element,
as determined using mass spectrometry.
Nuclear Notation
A
Z
X
For example:
A = mass number (sum of protons + neutrons)
X = element symbol
Z = atomic number (number of protons or charge)
Isotopes are atoms that have identical atomic
numbers but different mass numbers as the
result of differing numbers of neutrons.
carbon-12
12
6
C
carbon-13
13
6
C
For each carbon isotope, there are how many…
electrons?
protons?
neutrons?
The Chart of the Nuclides
As the number of protons, Z,
increases the neutron to proton ratio
required for nuclear stability also
increases.
Nuclides with Z > 83 (Bismuth)
are unstable.
Light nuclides are stable when the
neutron to proton ratio is close to
one.
Even numbers of protons and
neutrons seem to favor nuclear
stability.
Certain specific numbers of
protons or neutrons produce highly
stable nuclides. The magic numbers
are 2, 8, 20, 28, 50, 82, and 126.
Thermodynamics
1.010
Neutron
1.008
Energy, M/A (amu)
When the energies of all 2850
isotopes are plotted vs. their
charge density, the nuclides
form a parabola.
H-1
1.006
The free neutron has the highest
M/A & is unstable. It decays to
form a proton, 1H, in 10.6
minutes.
1.004
1.002
As the radioactive elements
decay, they go from higher M/A
values to lower M/A values thus
becoming more
thermodynamically stable.
1.000
Fe-56
0.998
0.0
0.2
0.4
0.6
0.8
Charge Density, Z/A
The open symbols are radioactive nuclides;
the filled symbols are stable and long lived.
1.0
The 56Fe atom has the lowest
value of M/A. So all elements on
the periodic table beyond 56Fe,
must have been formed by a
Super Nova.
The “Cradle of the Nuclides” results when the chart of the nuclides and the
parabolas are combined into one 3-D graph. It shows the ground states of all
stable and radioactive nuclides. The stable and long-lived nuclides are located
in the valley. The radioactive nuclides or those easily destroyed by fusion or
fission occupy higher positions in the cradle.
Most Common Particles Emitted by
Radioactive Materials
4
2
Alpha = a helium nucleus, He
Beta = an electron,
0
1
e
Gamma = electromagnetic radiation
1
0
Neutron = a neutral particle, n
with mass of about 1 amu or ~1 proton
Alpha Decay
Beta Decay
Occurs in nuclei with Z > 83.
Occurs in nuclei with a high
neutron:proton ratio.
The loss of two protons and two
neutrons moves the atom down
and to the left toward the belt of
stable nuclei.
A neutron is converted into a
proton inducing
a shift down and to the right on
the stability plot.
Positron Decay Electron Capture Decay
Occurs in nuclei with a low
neutron to proton ratio.
Electron capture is common in
heavier elements that have a low
neutron to proton ratio.
Gamma-ray Decay
A proton decays into a neutron and
an electron inducing a shift up and
to the left in the nuclear stability plot.
Gamma-ray decay generally
accompanies another radioactive
decay process because it carries
off any excess energy within the
nucleus resulting from the
radioactive decay.
All particles produced by the decay of an atomic
nucleus have the energy needed to penetrate
substances - but to very differing distances.
Balancing Nuclear Decay Reactions
Radioactive decay results in a redistribution of the basic
nuclear particles. The nuclear notation system keeps track of
where they are both before and after a nuclear transformation
has taken place.
To balance a nuclear decay reaction two rules must be followed.
1. Mass number is conserved in a nuclear decay reaction.
The sum of the mass numbers before the decay must equal
the sum of the mass numbers after the decay.
2. Electric charge is conserved in a nuclear decay reaction.
The total electric charge on subatomic particles and nuclei
before and after the decay must be equal.
Kinetics of Nuclear Decay
• Rate = (slope)
• dN/dt = -kN
Amount
 Radioactive decay processes
and many chemical reactions
show a direct correlation
between the rate of reaction
and the amount of reactant
present.
dN
 That is, if the amount of
dt
reactant is changed, the rate
of reaction changes by the
Time
same amount.
 The decay rate expresses the speed at which a substance
disintegrates. The rate (slope) decreases with time and
amount remaining.
N : The number of nuclei remaining
NO : The number of nuclei initially present
k : The rate of decay
t : the amount of time, t.
Linear Form of the Decay Equation
ln N / No = -kt  ln N - ln No = - kt  ln N = - kt + ln No
lnN
This is the equation of a straight line,
y = mx + b
where
y = ln N (N = any given amount)
m = -k
x=t
b = ln No (No = the initial amount)
time
The linear form is useful for finding the initial amount present
when t = 0 data was not measured.
Half Life Calculations
Another characteristic of a radioactive process is the half life.
The half life of a radioactive substance is the time required for
half of the initial number of nuclei to disintegrate.
Half life
Activity (cts/min)
30000
25000
t 12  0.693
k
Rate of decay
20000
15000
10000
5000
0
0
2
4 6 8
time (min)
10 12
Phosphorous-32 has a half life of 14.7 days
What about calculating lifetimes other than the
half-life? How would you calculate the t3/4 or t7/8?
 n0 
*
ln    kt
n
t  t 1  half life, where n  1 n0
2
2
*Notice that this is the reciprocal of ln (n/no) which was equal to –kt.
Therefore,
 n 
ln  0   kt 1
1 n 
2
0
 2 
ln 2  kt 1
2
k
ln 2 0.693

t1
t1
2
2
t1
t1
2
2
ln 2

k
0.693

k
If you know the specific
decay constant, k, you
know the half-life, t1/2.
OR
If you know the half-life,
t1/2, you know the specific
decay constant, k.
Today’s Experiment
Reactor:
• Irradiate Al with neutrons in reactor core.
• Measure gamma emission rate once a minute for 10 min.
• Plot by hand the exponential decay curve and linear plot for data.
(Plot these 2 scatterplot graphs on the postlab page 133.)
• Calculate the k, t1/2 and for the initial activity, lnAo & Ao of the Al.
Simulation:
• Run simulation for unknown sample number assigned by TA.
Copy data into Excel. (Record data in book or plan to print a copy.)
• Obtain second set of simulation data from your lab partner.
• Plot in Excel exponential decay curve and linear plot for both sets of data.
(So you should have 4 scatterplot graphs for the simulation data)
• Fit trendline equations to all 4 plots and use these to determine the k, t1/2
lnAo and Ao for both of the unknowns.
Part 1: Computer Simulation
• Run simulation for unknown sample number assigned by TA.
Copy data into Excel. (Record data in book or plan to print a copy.)
• Obtain second set of simulation data from your lab partner.
• Plot in Excel exponential decay curve and linear plot for both sets of data.
(So you should have 4 scatterplot graphs for the simulation data)
• Fit trendline equations to all 4 plots and use these to determine the k, t1/2
lnAo and Ao for both of the unknowns.
Sign in using your assigned
unknown number.
Press start.
Minutes are simulated – stop at
32 simulated minutes.
Reactor Tour & Nuclear Decay Lab
The S&T Nuclear Reactor has been in operation since 1961 and
was the first nuclear reactor in the State of Missouri.
The reactor is called a "swimming pool" reactor because it sits
near the bottom of a large concrete pool of water.
Part 2: Reactor Tour
The reactor pool contains 32,000 gal. of high-purity water and
is 9 ft wide, 19 ft long & 27-30 ft deep. In order to maintain that
high-purity, it is important not to touch the water or drop
anything into the pool.
Fuel Elements each contain between 9 and 18 fuel plates and
have dimensions of 3 in x 3 in x 3 ft. Each fuel plate contains 12.5
g of low-enriched Uranium-235. Fuel plates run the length of the
fuel elements and are .06 inch thick.
Measure gamma emission rate once a minute for 10 min.
Later
1. Plot exp. decay curve and linear ln N vs. time curve for data.
2. Calculate the k, t1/2 , lnAo and Ao for the Aluminum.
Today at the nuclear reactor you will follow the nuclear reactions
shown below and determine the half-life of aluminum-28.
27
13
Al  n 
28
13
Al 
1
0
Si 
28
14
Al   - ray
28
13
0
1
e
Write this
equation on
page 131.
Aluminum-27 is a stable natural abundance nuclide, which when
irradiated with neutrons from the reactor forms radioactive aluminum-28.
To determine the half-life of the aluminum-28 nuclide you will use a
Na-I scintillation counter to determine the number of gamma-rays
emitted as a function of time after the irradiation.
Then you will use first-order decay kinetics to determine the half-life.
Energy per Nucleon (M/A)
In today’s experiment, it will be shown that 28Al decays to
28Si because the latter is more thermodynamically favorable.
0.99940
0.99935
28
Al
27
0.99930
Al
0.99925
0.99920
0.99915
0.46
28
0.47
0.48
0.49
0.50
Si
0.51
Charge Density, Z/A
You will use first-order decay kinetics to determine the half-life.
FOR THE REACTOR TOUR
NO backpacks, NO cell phones & NO electronic devices allowed!
Leave them in the lab.
Bring photo ID, ink pen, and green book. (Record data on p131.)
TA’s will escort the students to the reactor.
Reactor staff will give a brief lecture before the experiment;
take notes (#4 on p 131), ask questions & volunteer to help.
After the reactor portion of the experiment:
You need to be working on the simulation (pp 127-9),
make at least 1 linear and 1 exponential scatterplot ***
and work on the radioactivity exercises (pp 135-6).
***This is also a good time to get help if you do not understand how to use Excel.
For April 28-30:
1. Turn in Nuclear Decay Lab pp 127-29 + 4 graphs
Reactor Lab (pp131-4) & Exercises (pp135-6).
2. Read over Gas Laws & Buoyancy Effects (pp193-210).