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Typical Decay scheme II tp://www.nucleide.org/DDEP_WG/Nuclides/Na-22_tables.pdf •Nuclei can decrease their proton number by one in three ways, positron emission (the most common) Electron capture (much more rarely; see next slide), or proton emission (very rare). •Decay rates expressed in terms of Becquerrel (1/sec) or Curies (37 GBq)

Typical Decay scheme II Nuclei can decrease their proton number by one in three ways, positron

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Page 1: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

Typical Decay scheme II

http://www.nucleide.org/DDEP_WG/Nuclides/Na-22_tables.pdf

•Nuclei can decrease their proton number by one in three ways, positron emission (the most common)Electron capture (much more rarely; see next slide), or proton emission (very rare).•Decay rates expressed in terms of Becquerrel (1/sec) or Curies (37 GBq)

Page 2: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

Radiation Dose•Dose:

•1 Gray = 1 J/kg of whatever radiation (energy deposited per unit mass), supplants the RAD (Radiation absorbed dose)•Roentgen (older unit, radiation needed to produce a certain charge per unit mass (1 esu /cm3 of dry air). This corresponds to 0.258 mC/kg.

•Equivalent Dose•1 Sievert: absorbed dose multiplied by factors to account for relative biological effectiveness for particular radiation type (, n etc.; energy etc. ) and body part involved. NOTE units are the same as the Gray, but the meaning is quite different. •REM (Roentgen Equivalent Man): 1 REM = 10 mSv

Page 3: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

Radiation Dose

http://www.ccohs.ca/oshanswers/phys_agents/ionizing.html

NOTES:•Prior to 1990 the weighting factor was referred to as the “Quality Factor and you will still see this term used.•There is some controversy over the appropriateness of the weighting factors (especially for alphas)

Page 4: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

Effects of Radiation•“LD50/60” Dose that would result in death for 50% of the population so exposed within 60 days (Lethal Dose to 50% of the population)

•LD50/60 limit for gamma radiation is roughly 450 RAD (or 4.5Gray) for whole-body exposure•Threshold lethal Dose (2 Gy)

•Beyond these acute dose issues, future development of cancer is also a concern

•Doses at ~10 cSv appear to produce no increased risk of cancer•Occupational limits for radiation workers are set at levels below this to be conservative (typically 50 mSv/yr for radiation workers). •Typical background exposure in the US is of the order of 3.5 mSv/yr (as high as 8 mSv/yr in Colorado mountains).

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Sources of Background Radiation

•Cosmic Rays•Naturally occurring radioactive nuclei

•40K this is the most abundant radio-nuclide in your body•14C (e.g. about 50 times/sec one C atom in the DNA of one of your cells is converted to N by beta decay).•222R, a decay product from 238U, and a common concern in buildings

•Medical tests•Man-made nuclides (fallout, waste, release etc.).

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Sources of Background Radiation

http://web.princeton.edu/sites/ehs/osradtraining/backgroundradiation/background.htm

Page 7: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

Effects of Radiation

•Recall: 1 rem is roughly 10mGy for gammas•Typical background radiation is 350 mrem/yr, airline travel gives roughly 0.4-1 mrem/hr (4-10 Sv/hr) http://www.physics.isu.edu/radinf/risk.htmSee also: http://trshare.triumf.ca/~safety/EHS/rpt/rpt_4/node20.html

Page 8: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

Radiation Dose•Different types of radiation at a given energy have different “Relative Biological Effectiveness”, and different parts of the body have different susceptibilities to radiation, so you have to be a bit careful about how you quote numbers. •Today medical physicists discuss dose in Gray to specific organs, rather than Sieverts etc..

Page 9: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

Radiation Shielding•Different types of radiation penetrate through matter with different ranges. Alpha particles are very easily stopped (doubly charged and relatively slow), beta particles are relatively easy to stop, gamma rays need very heavy shielding, and neutrons are the hardest to shield against.•https://reich-chemistry.wikispaces.com/b.sulser+and+k.nagle+powerpoint+presentation

neutron

Page 10: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

Relative Biological Effectiveness

http://en.wikipedia.org/wiki/Relative_biological_effectiveness

Note that a 1.5 Gy dose of Carbon ions has the same biological effect as a 4.5Gy dose of photons (for this particular cell type).

Page 11: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

Applications of Radiation•Radiation and radioactive materials are used in numerous applications today, we’ll touch on only a few of these:

•Nuclear Medicine•Diagnostics (x-rays, CAT scans, PET scans, etc.)•Cancer treatment (x-rays/gamma-rays, radio-nuclides, protons, heavy ions)

•The key here is that rapidly reproducing cells (such as CANCER, in children/fetuses) are more susceptible to radiation damage AND CANCER cells are less able to repair the damage radiation causes.

•Dating of artifacts (archeologic, organic, geologic etc.)•trace element analysis•Nuclear power

Page 12: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

Proton Radiotherapy

http://en.wikipedia.org/wiki/Proton_therapy http://mpri.org/science/vstreatments.php

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Relative Biological Effectiveness

http://www.ccohs.ca/oshanswers/phys_agents/ionizing.html

NOTES:•Different parts of the body have different susceptibilities to radiation (in terms of their likelihood of developing cancer after a given exposure) •This is taken into account in planning radiation treatments for cancer.

Page 14: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

Nuclear Fission

http://hyperphysics.phy-astr.gsu.edu/hbase/nucene/fission.html

KEY element (from CALM):•Large, unstable, nuclei (6)•Neutron activated dissociation (4)•These are both necessary but not sufficient:•“Chain reaction (4)” but what does that mean?•More one neutron in MULTIPLE neutrons out (to sustain the reaction) (8) THIS IS THE KEY ingredient.

Page 15: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

Fission products

http://www.euronuclear.org/info/encyclopedia/f/fissionproducts.htm

http://en.wikipedia.org/wiki/Fission_products

Page 16: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

Nuclear Reactors (LWR’s)

http://reactor.engr.wisc.edu/power.html

Boiling water reactor (BWR) Pressurized water reactor (PWR)66% of US reactors are this type

Page 17: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

Yucca Mountain

http://www.ocrwm.doe.gov/ymp/about/why.shtml

Page 18: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

American Nuclear Plants

http://www.nrc.gov/info-finder/reactor/

Page 19: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

Nuclear Waste depots

http://en.wikipedia.org/wiki/Radioactive_waste

Page 20: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

Nuclear Decay Chains

Does not include the 4n+3 chain or Actinium series which terminates in 207Pb (Wikipedia does not have so nice a graphic for that chain; from: http://en.wikipedia.org/wiki/Decay_chain

4n chain: Thorium series 4n+1 chain

Neptunium series

4n+2 chain Radium series

Page 21: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

•Dates have to be calibrated to account for historic variations in the production and distribution of 14C in the atmosphere (thank goodness for the Bristlecone pine tree). Figs from:•http://www.ndt-ed.org/EducationResources/CommunityCollege/Radiography/Physics/carbondating.htm

and http://en.wikipedia.org/wiki/Radiocarbon_dating

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Various Dating schemes

See article at: http://physics.info/half-life/

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Early Particle discovery: -

From E. Segre “Nuclei and Particles”, 2nd editionParticles appear as tracks (in bubble chambers in the early days, in electronic trackers of various sorts today) that are bent by a magnetic field. By measuring curvature, track length etc.things like half-life, momentum, charge etc. can be determined.

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Early categorization of Particles

Early collider experiments started to reveal more and more particles, and people started to question whether they were truly “Fundamental”, but did allow for the prediction of “missing particles that were later found.Attempts to rationalize this “zoo” of particles led Gell-Mann (and independently Zweig) to suggest more fundamental building blocks (based largely on the observation of patterns [symmetries] in the properties of the particles; they appeared in families of 1, 8, 10, 27 etc. members]:

Page 25: Typical Decay scheme II  Nuclei can decrease their proton number by one in three ways, positron

The Standard Model

http://newsimg.bbc.co.uk/media/images/41136000/gif/_41136526_standard_model2_416.gif