Cs-137 Experiment: Effects of Heavy Metal Shielding on Radiation Levels

In summary, the conversation discusses an experiment with Cs-137 radiation sources and the use of lead and other heavy metals as shields. The individual is trying to determine the rate of radiation and the effects of removing the source on the reading. They also discuss the type of radiation produced by Cs-137 and the amount of lead needed to shield it. The conversation also mentions the possibility of backscatter and characteristic x-rays causing high readings, resulting in the use of aluminum as a potential solution. The conversation ends with the individual recalibrating the detector and repeating the experiment with thicker layers of aluminum.
  • #1
Z3r0
Hey guys, I am currently running an experiment with Cs-137 multiple sources ranging from 1 to 10 uCi, i have a lead pig with a Cs-137 source at the top and a 1/4" small tunnel drilled through the 2" thick slab inside the pig is the Gieger counter, Using various heavy metals as a shield i seem to only get the radiation shielded down to certain level, even with 2mm of lead the level doesn't drop any lower then .2mm of lead. Is this radiation causing other reactions on the other side of the shield to cause a consistent transmission level?
 
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  • #2
Do you have a sketch of the setup?
What is the rate you measure?
What happens if you remove the source?
 
  • #3
What kind(s) of radiation does Cs-137 produce, and how much lead do you need to shield them?
 
  • #4
Pending the requested diagram let me note that in comparing count rates between 0.2mm and 2mm of lead shielding the difference may be too small for you to reliably notice a difference if you are trying to read the rate meter because it may be too low with too much fluctuation. The fraction transmitted through 0.2mm slab Is expected to be 0.98 and through the 2mm 0.84. If you have a scalar you should collect enough data to get a statistically significant difference between the different reading.. BTW the half value layer for Cs-137 is 8 .mm of lead.
 
  • #5
After checking the exposure rate constant for Cs-137 which is 0.33mR/mCi.hr at 1m. a 10uCi source would produce an exposure of only 0.052 mR/hr at 25 cm which would only be measureable on the lowest scale of most GM counters and subject to large fluctuations. So you need a stronger source to get a reasonable steady reading.
 
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  • #6
The source is about 3-4 in from the detector, without a sample in the direct beam the reading is apprx 5 mR/hr with my 5uCi source. When i remove the source the reading drops to less than .004 mR/hr
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  • #7
With no source the reading is 0.004 hr/hr and with a 5uCi sources the reading is 5 mR/hr.

However at 3 inches (7.5 cm) the expected reading should be 0.34 mR/hr for a 5 uCi source. So why the high reading? From your diagram I would expect backscatter scatter from the shielding behind the detector from the Compton effect from the Cs gammas that pass through. Also the 662 kV gamma from Cs will interact with the lead via the photoelectric effect to emit 70 -80 KeV x-rays which in your case are entering the GM counter mostly from the rear. You have what we call in the business "bad geometry" . You must reduce the scattered gammas and characteristic xray. One way is to move the lead behind the detector farther away using the inverse square law to reduce these radiations. You could also add some low atomic number material like aluminum. With sufficient thickness it will reduce the backscatter and characteristic xrays from the lead while not contributing as much as the lead would.
 
  • #8
Okay so when i removed the rear lead wall my reading was unchanged, still about 5 mR/hr. To cut down on any interactions from the aperture I ran another test with a free floating source and no lead anywhere in the path my reading jumped to 23 mR/hr @ 7.5cm. Both tests were run without a shield in the path of the beam.
 
  • #9
The reason that you have a larger reading without any shielding is because you are exposing the whole GM tube. The GM counter is calibrated by exposing the whole tube to a radiation field that is constant over its volume. I do not know why you are reading 5mR/hr since the source is not capable of emitting that much radiation assuming the counter is calibrated correctly.

Question, what are the dimensions of the GM tube.

Also another aspect of bad geometry is that the absorber is next to the tube and might be producing its own scatter/xrays that might have otherwise not have passed through the tube. Move the absorber closer to the source until the reading of the GM counter reaches a minimum. This is the optimal position.
 
  • #10
Pancake Gieger 5x2.5cm calibrated not more then 6 months ago. Just tested the same experiment with another detector and received a much more believable reading, .35mR/hr it appears my main Gieger is out of calibration i'll be sending that out soon for re-calibration in the mean time my back up Gieger doesn't fit in my chamber nor does it communicate with a computer :/

The reason that you have a larger reading without any shielding is because you are exposing the whole GM tube.
I figured that and to reduce the chance of other reactions we reduced the amount of the counter that is exposed by having a smaller aperture. Hence the lower count.
 
  • #11
The pancake chamber is a thin window chamber an sensitive to electrons and almost 100% efficient as comparted to gammas The electrons which will be knocked out of the lead absorber by the Cs gamma (Compton recoil electrons) could account for the high readings. To check this hypothesis put a few sheets of Aluminum foil between the absorber and the pancake chamber and see if this helps.
 
  • #12
Even with the aluminum sheets (3) I'm still having the high counts in the 4-5 mR/hr range, which shouldn't be happening with a 5uCi source...
 
  • #13
I should have checked the range of the electrons .It's more the 0.5mm Al. not a few sheets of Al foil. sorry.
 
  • #14
Okay, I have some Cs-137 calibrated sources I'm going re-cal the GM tomorrow morning and try the Al tests again with thicker layer. i'll post the results. Thank you
 
  • #15
I've calibrated the detector and repeated the recoil electron hypothesis, with apprx .8mm of Al @ 7.5cm I am reading a measure of .9 - 1.6 mR/hr open source.
Much lower reading but still hot for a 5uCi source.
 
  • #16
You said previously that the GM counter was connected to a computer. If the GM counter a stand alone instrument with an output to a computer or what?
Tell me about you calibration procedure.
 
  • #17
The GM is a SEI Inspector EXP usb, it is capable of connecting to a computer to store and print a graph read out of exposure or you can use it by itself as a handheld with a probe. I receive the same reading either way.

I called SEI directly and they put me in touch with their calibration lab. Using a 1 uCi calibrated source they had me put the source directly on the detector screen while connected to the computer, and change the "Sensitivity" to a higher setting. Until the detector was reading an average of 35 mR/hr with the source directly on the screen.
 
  • #18
Not what I would consider a standard calibration procedure. First do you know if your source has a calibration certificate? If not how do you know if it is a 1 uCi source and not a 0.8 uCi source. Is the source a button source or a rod?
 
  • #19
It is a button source, we don't no the exact Ci, but the paperwork that came with the source say its +,- 10%, as far as the tech on the phone i don't know what kind of cert's his source has. TBH the whole experience seemed a little weird as far as "calibration" goes, just by changing a sensitivity to calibrate seems iffy.
Most everything I've read about calibrating this particular unit says u need to have the probe at a distance that corresponds to 50mR/hr and record the data for 20 consecutive readings.(which also doesn't make sense cause its a continuous readout).
 
  • #20
So you know it is between .9 and 1.1 uCs. If SEI is a certified calibration lab. it will have a source traceable to the NIST (National Institute for Science and Technology formerly the National Bureau of Standards). A typical calibration procedure would be to use a relative strong source say 100 mCi and expose the probe at a distance a meter or more from the source where the radiation field is fairly uniform over the volume of the detector. They know the exposure rate at this point form the accepted value of the Gamma Ray exposure constant which is 0.38 mR/hr/mCi. They may repeat this for different scales by using different distances.
Now having done that they can place a 1uCi source a specific way on the detector and note the reading which of course will be different. If you repeat this procedure at a future date and the reading is the same they you should be reasonably confident that your instrument is still in calibration. Of course you have only check the reading on one scale.

Z3r0 said:
TBH the whole experience seemed a little weird as far as "calibration" goes, just by changing a sensitivity to calibrate seems iffy.

Your instrument has built into it a set of calibration factors for different radiation sources since each source emits different amounts of radiation per mCi. The probe only measure the number of interactions per minute so it does not have any idea of the type of energy of the radiation that it detects.
 
  • #21
Yes, so based on the 1uCi scale our instrument wasn't that far off but who knows on a larger scale. @ 5 uCi we're still getting these extremely high readings my guess from the high energy beta reaction from such a close distance. The "bad geometry" was taken care of and still received a high measurement even when .8mm Al was in place to reduce the electrons contacting the detector. I'm thinking we're going to need a larger source as you stated earlier in order to measure the fine changes in attenuation for different shielding materials. I believe 10 uCi is the highest source obtainable without licensing, would that be correct?
 
  • #22
Yes 10 uCi may be the largest source you may possesses without a license and I think that is too small for your purposes. BTW why are you making these measurements since the Pb attenuation of Cs137 is well known?.
 
  • #23
The user manual for the SEI Inspector EXP(the detector I've been using) says it can be calibrated using a pulse generator I actually have access to one I'm going to mess around with that to see if I can calibrate it that way.
BTW why are you making these measurements since the Pb attenuation of Cs137 is well known?.
Seeing if I can use a composite material with similar attenuation curves and lighter weight.
This is just one part of the tests, i also have access to a medical x-ray generator and use a calibrated detector for it, but that's further off my work campus, whilst the Cs-137 i have in my lab easier to work with and run multiple tests quickly.
 
  • #24
The pulse generator is good only for measure count frequency and is unrelated to exposure rate. If exposure rate is not important then go ahead and ckeck all scales with a pulse generator, you are only interested in relative measurements. The caveat is make sure you are only measuring the radiation that you are interested in.

What do you mean by composite? What will it be made of.?
 
  • #25
Yeah counts don't mean much to my data, I'm more interested in exposure rate, counts have no correlation to mR/hr?(i thought there would be) This user manual doesn't give very much information on any of these topics kinda of annoying. Might have to end up sending the unit back to SEI and have them calibrate it.

What do you mean by composite? What will it be made of.?
http://www.nitenterprises.com/ I'm the lab tech for NIT, i can't say too much, but feel free to poke around on our website.
 
  • #26
Z3r0 said:
counts have no correlation to mR/hr?(i thought there would be

By that I mean that if you do not know the type of radiation the counter is registering you cannot know the exposure rate. The purpose of the calibration by a radioactive source is to establish this correlation. I you are trying to measure an attenuation factor for some type of radiation all you need is to determine the ratio of a reading with the absorber in place to the reading without the absorber. It is a fraction. If you want to know the exposure rate of the transmitted raidaion all you need is the exposure rate of the unshielded source (which you can calculate) and the traction of radiation that is transmitted. If you have a particular material in mind you can get a pretty good guess from published data even if your absorber has not been measured.
 
  • #27
I actually have been doing these tests based on the ratio of unshielded vs shielded detector, but i thought that if the detector wasn't calibrated who's to say it's not off by a % in which case it would become more inaccurate depending on source strength. but also the detector doesn't decipher between beta, gamma, x-ray or electrons. i can only guess x-ray and gamma are the only two transmitting.
 
  • #28
I see that your enterprise is interested in radioprotective substances. I expect that at some time to test them you must expose something to a certain well known amount of radiation (a dose) and evaluate the effect. How do you propose to do this. By that I mean what will be the source of your radiation and how will you calibrate that source? .I bring this up because it can be more difficult than you might think. Your experience in trying to measure the attenuation of materials which is (should be) very easy should give you a heads up when working with radiation.
 
  • #29
My background is more specifically in X-ray, and we have a partnership with a local college that has an x-ray generator. but in my lab we have Cs-137 sources that we are using to measure the attenuation differences between the composites, all are very small sources and as you said earlier it's difficult to measure on such a small scale. When using the X-ray machine i have a calibrated detector for x-ray only, and i can measure those differences in exposure while using different exposure techniques.
 
  • #30
You intend using the x-ray unit at the college for the evaluation of the company's product?
 
  • #31
Just for our tests yes, when we have a final product for high energy attenuation we'll be sending our product out to 3rd party laboratories for accurate ASTM standards.
 
  • #32
I don't understand the ;phrase "high energy attenuation" in this context.
 
  • #33
high energy photon* attenuation, sorry.

Thanks for the input I appreciate it.
 

What is Cs-137?

Cs-137, or cesium-137, is a radioactive isotope of cesium. It is commonly used in medical and industrial applications, as well as in scientific research.

Why is Cs-137 used in this experiment?

Cs-137 is used in this experiment because it is a gamma emitter, which means it releases high-energy radiation that can penetrate materials. This makes it a useful tool for studying the effects of heavy metal shielding on radiation levels.

What are the potential effects of Cs-137 exposure?

Cs-137 exposure can have various effects on living organisms, including damaging cells and DNA, causing radiation sickness, and increasing the risk of cancer. The severity of these effects depends on the level and duration of exposure.

How does heavy metal shielding affect radiation levels from Cs-137?

Heavy metal shielding, such as lead or concrete, can absorb or block the radiation emitted by Cs-137. This can reduce the amount of radiation that reaches the surrounding environment or living organisms.

What are the practical applications of studying the effects of heavy metal shielding on Cs-137 radiation levels?

Understanding how heavy metal shielding affects radiation levels can help in the development of safety measures and protocols for handling radioactive materials. It can also inform the design of radiation shielding for medical and industrial facilities, as well as aid in the cleanup and containment of radioactive waste.

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