Direct detection of Alpha Decay from Radon Gas> Tutorial by Geo
Radon
collection is one of the few "separations" that can be done in the
home lab,
and is relatively easy.
There are a number of Radon isotopes, all coming
from decay of different
Radium isotopes. The two of major interest to us in
the home lab are
1) Rn-220, also called Thoron, from Radium 224, which is in the Thorium-232 decay chain, milked from Thorium Lantern Mantles,
2)
Rn-222 the one commonly called RADON when
we are
referring to Radon in homes. Rn-222 comes from the Radium 226 in the
Uranium-238 decay chain. Radon is a gas, heavier than air and sometimes is
called "radium emanation". Milked from Radium Watch Hands or natural Uranium
ore.

Collection
can be accomplished by adsorption onto activated charcoal, or air pumping.
see:
Once the sample is captured, you have pure Radon gas for a time,
depending on half-life of the isotope.
Our goal is to count Alpha
particles coming from the Radon, and time the half-life. Using a Lucas Cell makes
it easy. A Lucas Cell consists of a container, whose inside walls are coated
with Zinc Sulfide, at one end is a clear window so the scintillations can be
observed and counted by a photomultiplier tube, and the other end contains one
or two valves for the introduction of air. Cells with one valve must be first
pumped to a vacuum with a pump, the an air sample is "grabbed" by releasing the
valve until the air is sucked inside, then closed again.
Grabbing air samples to test for Radon in air can be accomplished by pumping out the air from a Lucas Cell, transporting the cell to the test site ( cave, mine etc.), then quickly crack open the valve. Air rushing in will fill the cell with a representative sample and the Lucas Cell can be immediately tested on a portable PMT tube as shown in this apparatus that I made up from commercial parts, a hand vacuum pump, and cardboard tubes:
Naturally this is called a GRAB SAMPLER
Cells with two valves use a simple air pump to circulate the air, until a
sample is collected, when both valves are closed.
Once the air and Radon are inside the Cell, you must count the CPM
being created by the Alphas right away. For Radon-222, the counts will remain
steady over a period of time, hours at least. The reason for this is the long
half-life ( 3.8 days) of the Radon itself, and also the high energy of the
Alphas from the decay daughters, Po-218 and Po-214. Over time, the energy of the
Alphas will shift from 5.49 MeV of Rn-222 to 6.02 MeV of Po-218 to 7.69 of Po-214. See
the decay scheme at:
http://www.ead.anl.gov/pub/doc/natural-decay-series.pdf
For Thoron, it is more dramatic, and far better for lab
demonstration
purposes. I use a "cow" for collection, which is simply a large
kitchen funnel
with a coffee filter in the bottom. In the bowl of the funnel
is placed the
uranium ore or thorium mantles. On the spigot is a tube going to
an air
pump, which sucks the air over the samples, and delivers it via
another
inline filter to the Lucas Cell ( or whatever detector you
choose).
Picture shows 15 gm Th-232 in Pepsi Bottle cow. Airpump is
surplus "breathing
machine" or nebulizer purchased at a garage sale for 5
bucks. Container of
activated carbon in background is for canister
collection
experiments.
Air is drawn through 40 Th-232 lantern mantles,
pulling gaseous Radon 220 (Thoron)
off through filter which removes solid decay daughters. Air
flows
through light trap and valve into a 1 liter ZnS(Ag) chamber. Air exits
the other
valve and light trap.
After a minute or two , the count rate
stabilizes due to direct reading of Alpha particles from the
Rn-220. At a
point after seeing the steady state, the valves are closed,
trapping a given
sample which is then observed for decay due to the short
56 second half-life
of Rn-220.
Running the
air with the cow empty yields around 15 CPM with no radiation
present other
than random junk in the air.
Adding the mantles quickly increases the count
to almost 2000 CPM, and this
is with the mantles STILL INSIDE the plastic
baggies. Each baggies has a
tiny vent hole, through which some of the Thoron
escapes. Later naked
mantles will be tested.
The above are large
readings, with HV set to around 900. In practice, HV
will be set lower on the
plateau with a background reading way down at only
50 CPH ( counts per hour),
and then the radon will register 200 to 230 CPH
per
pCi/L.
Thoron collected in this way
gives a great reading on the meter, and begins
to die away in mere seconds as
the half-life of Rn-220 is only 56 seconds.
The Polonium-216 daughter decays
in less than a second, so within a few
minutes the experiment is over. If not
flushed, the daughters will again
start producing Alphas in about 12 hours,
from the further decay into
Po-212.
For those of you who have purchased one of my
Radon
cows, here are some tips on milking it with simple
apparatus:.
First of
all, it takes about 100-200 radium watch hands to provide enough "parent" to get
1 uCi of
activity, depending upon the size of the watch hand. One uCi of parent will
produce 1 uCi of the
daughter
Ra-222 when equilibrium is reached. Half-life of Ra-222 is 3.8 days.
Once milked, the radon will re establish equilibrium in 20 days.
See:
http://physics.nist.gov/GenInt/Curie/1927.html
or use the
Universal Decay calculator at:
http://www.wise-uranium.org/rcc.html
One whole
microCurie of Radium will produce one whole microCurie of Radon every 20 days,
but
the actual
gas volume is quite small, only .000002 mL. Not all of the gas will be free
to leave the matrix either,
so don't try
to calculate the exact dose from simple math.
The THORON
Cow of course uses Thorium in the form of mantles to produce the THORON gas,
which is an even better
type of
Radon ( Radon 220) from a home lab experiment standpoint. Having a much shorter
half-life of only 56 seconds,
some pretty
dramatic demonstrations can be accomplished, well within the attention span of
even grade school aged
students.
It takes
about 50 mantles to provide an approximate 1 uCi of parent. IF the material is
40 years old, there will be an approximate
equilibrium
between the parent Th-232 and the daughter Ra-224 which is responsible for the
Rn-220. Our mantles are probably
no where
near that old, but even 9 year old material will have about 50% equilibrium
already. One day, we will have to do the age
test on this
stock on mantles to determine the material's equilibrium fraction. I recommend
100 mantles for a serious Thoron Cow.
Nonetheless,
whatever the equilibrium fraction, it is assured that there is at least 50% of
the maximum Radon-220 available, and
the Thoron
Cow can be milked once per hour.
A gas extractor is simplicity itself. Use a squeeze bottle as designed for Ketchup or Mustard that has a pointy top.
Clear plastic versions are more dramatic, and can be obtained from any
kitchen supply aisle.
Fill the
bottom 1/3 of the container with cotton wadding, then layer on your parent
material, either radium or thorium. Finally add another 1/3 filling of loose
cotton, leaving 1/3 at the top empty for expansion/contraction. Place a piece of
cloth over the container mouth before adding the top to it, to act as a
pre-filter against solids. Cap when not in use to accumulate the gas, and when
ready for use, uncap and slip your lab tubing over the pointy dispensing end. A
few puffs and you will have enough gas to fill your Lucas Cell, or to use in any
other desired detector. Always use an inline filter to eliminate any solid
particles that may get into the air stream, any of which would contaminate your
detector. Contact me if you need any glass-fiber-on-paper filter media, as I
have several boxes of the roll material. It can be cut or punched into standard
discs and is very cheap.
Don't forget that any Radon gas is heavier than air.
Radon in water ideas:
Have
fun
George Dowell
New London Nucleonics Lab
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Materials available from the author:
George Dowell
NLNL/ New London Nucleonics Laboratory
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