First publicized/Available Online (Article-1, Article-2): Mar 28, 2011, April 1, 2011
Citation: “Radioactivity of cigarettes and banana”, Manmohan Dash, Communicating Science, April 11, 2011, publisher: Invariance Publishing House, MDash Foundation
Link to permaweblink in citation or copy/archive material as it isΒ with Creative Commons and other copyrights in this web-site in mind:Β permaweblinkΒ Β
Radioactivity of cigarettes and banana
Manmohan Dash
1βActivity of Cigarettes
mol ofΒ Pband
mol of Po. 1 molβ =β 6.022β Γβ 1023βelementsβ. This implies
nuclei of Pb is 1.45β Γβ 1015β ββ cigarette. This in turn implies 6.022β Γβ 1017β Γβ (0.5)/(210) nuclei of Po is 1.43β Γβ 1015β ββ cigarette. Activity: Pb: (1015β Γβ 1.45β Γβ 0.693)/(β 22.3β Γβ 365β Γβ 24β Γβ 3600)β =β 1.43β Γβ 106 decaysβ ββ secondβ =β 1.43 MBqβ =β (0.00143)/(37). Units: Curiesβ =β 38.65 microCurie, Po: 1015β Γβ 1.43β Γβ 0.693β Γβ 137.376β Γβ 24β Γβ 3600β =β 8.35β Γβ 107 decaysβ ββ secondβ =β 83.5 MBqβ =β (0.0835)/(37) Curiesβ =β 2.26 milliCuries. So the Ξ² energy of the Pb (210) makes it 1.43 MBqβ Γβ 0.064 MeVβ =β 91.52 GeVβ =β 91.52 GeVβ ββ cigaretteβ =β 91.52β Γβ 109β Γβ 1.6Γ10β ββ 19Jβ =β 14.64 nanoJβ ββ cigarette.
Or 14.64 nanoGrayβ ββ cigarette, considering 1 kg of absorbing material = 1.76 nSvβ ββ cigarette. Considering 20 cigarettes a day, that is, a pack of cigarettes, and regular smoking through a year this would be 20β Γβ 365β Γβ 1.76 nSvβ =β 12.83 microSvβ ββ year. Lung has a weighing factor of 0.12 and Beta (Ξ²) emission has a weighing factor of 1. So Po(210) with Ξ± emission would be 83.5 MBqβ Γβ 5.407 MeV which is actually 4.51β Γβ 105 GeVβ =β 4.51β Γβ 1014β Γβ 1.6β Γβ 10β ββ 19 Jβ =β 72.2 microJβ ββ cigarette. Or 72.2 microGrayβ ββ cigaretteβ =β 8.664 microSvβ ββ cigarette. So with a pack of 20 cigarettes and 365 days of smoking one would collect a dose of 20β Γβ 365β Γβ 8.664 microSvβ =β 63.247 milliSvβ ββ year.
This is considering 1 kg of absorbing material, lungβs radiation damage factor and a simple Ξ± emission effect not considering Ξ± emission nuclear recoil. Also I have not multiplied the factor 20 for Ξ±β ββ particles which is prescribed, since I already calculated the energy I am not sure its necessary or not. In any case its dangerous enough. Po is more dangerous than Pb for lung cancer. If the cigarette would indeed contain 0.5 microβ ββ gram of Pb and Po, which is not known a priori, the values from experiment performed, 2 examples shown below shows different value, which just means the cigarettes contain correspondingly different radioactive contents, which is nonetheless harmful enough to kill smokers by lung cancer.
2Β ActivityΒ of Bananas
Bananas Are Radioactive
Anne Marie Helmenstineβ[Ph.D., About.com Guide]
Source: Chemistry, About.Com
Excerpt/Abstract: from above article:
- JOE: so the half life is 1.25 billion years and decays 14 times a second? are you sure you know what your talking about?
- AMASA @joe: There are many, many, many, many, many molecules of potassium in 450 mg of potassium.
- CHRIS @joe, the math looks a bit off, but not in the way youβre thinking, so let me break it down. half life of Kβ ββ 40β =β 1.248β Γβ 109 years years, natural abundance of Kβ ββ 40β =β 0.012, molar mass of Kβ ββ 40β =β 39.96399848 gβ ββ mol, 450 mgβ Γβ 0.012, 5.4 mgβ =β 0.0054 g, (0.0054 g)/(39.96399848 gβ ββ mol)β =β 1.3512β Γβ 10β ββ 4 mol,β 1.3512β Γβ 10β ββ 4molβ Γβ 6.022β Γβ 1023particlesβ ββ molβ =β 8.137β Γβ 1019atoms, Kβ ββ 40,β 4.0685β Γβ 1019 decay in the first 1.248β Γβ 109 years, average of 3.26β Γβ 1010 per year, average of 1033β ββ second
- MARK ANDERSON @Chris Close, but its .012 which is really 0.00012 which works out to about 0.054 mg.
- ELIOT Good work Chris and Mark. However your estimate for number of decays per second will be off because you didnβt figure them using logs. Radioactivity is an exponential decay function. So the number of decays per time unit starts higher and then slowly gets lower over time. So one second now will have almost twice as many decays as one second 1.248β Γβ 109 years from now. Of course we are interested in the rate of decays for seconds now not 1 billion years in the future. This is what pushed the number to 14 per second.
- MANMOHAN DASHβ [βindependent work of Manmohan Dash] Hi Chris, Mark: you laid the ground work. Thanks. I will complete the calculation and show you this is exactly rounded to 14 decays per second. If you change your fraction of radioactive Kβ ββ 40 to 0.01 as in the article rather than 0.012 etc I think it will give the exact answer. Here is the answer: I take the calculation you two have done correctly, i.e. the 450 milligram banana contains 8.137β Γβ 1017 nuclei of Kβ ββ 40 (not 1019 as corrected by Mark) Now the decay constant or transition probability as one may call it which gives the probability at any time of a single nucleus to decay at any time is Οβ =β (0.693)/(Thalfβ ββ life). This is obtained by using Heisenberg Uncertainty principle for the nuclear decay. Here decay width which is given as a width of energy and mean life time which is given as a width or uncertainty in time, must multiply to h-cross (time – energy uncertainty). Now Mean life is related to half-life by the factor 0.693 (69.3% of nucleus would decay in the mean life where as 50% would decay in a half-life) So the decay probability = Ο gives the probability or likelihood that any single nucleus will decay or not. So we know this probability because we know the half life to be 1.25 billion years that is 1.25β Γβ 365β Γβ 24β Γβ 3600β Γβ 109secondsβ =β 1.25β Γβ 3.15β Γβ 1016seconds. Since the banana has450 milliβ ββ grams of Potassium it has as many radioactive Kβ ββ 40 as we just counted, 8.137β Γβ 1017 nuclei, at the time of eating. So the probability of decay is Ο and you know how many nuclei you got. Multiply them to get the exact number of radioactivity of your banana. Needless to say this product is 14.3.(8.137β Γβ 0.693)/(1.25β Γβ 3.15β Γβ 1017β ββ 16)β =β 1.43β Γβ 10β =β 14.3.
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