Lecture 6 Radioactive Isotopes

Slides:



Advertisements
Similar presentations
Nuclear Chemistry Chapter 25.
Advertisements

Nuclear Chemistry Chapter 25.
The ABC's (or Alpha, Beta, Gamma) of Radioactivity
Radiation in the Environment
Introduction to Radiation: Radiation Types ©Health Physics Society.
Kinetics of Radioactive Decays Decay Expressions Half-Life Average Life First-Order Decays Multi- Component Decays Mixtures – Independent Decays Consecutive.
Chapter 6: Isotopes. What is an isotope? What is the difference between.
Unit 1.3 Nuclear Chemistry
Radiation Protection Course
Chemistry 106 University of Nebraska SPRING April 2009.
A Nuclear Power Plant. Fallout from Chernobyl The question that all countries asked in 1986, and continue to ask to this day: Could it happen here?
Do Now (3/17/14): What are some words and images that come to mind when you hear the word “radioactivity”? What is an isotope? What makes an isotope.
Radiation Physics PHY471 A.M. El-Khayatt A. M. El-Khayatt, PHY464 Autumn 2014 Radiological physics is the science of ionizing radiation and its interaction.
Chapter 29 Nuclear Physics.
NUCLEAR CHEMISTRY The Basics. The Nucleus The nucleus is composed of nucleons –protons –neutrons A nucleus is characterized by two numbers –atomic mass.
NUCLEAR CHEMISTRY By: Stephanie Chen and Stephanie Ng.
Mini Quiz- Half Sheet H = 1.01 g/mol, O = g/mol S = g/mol, N = g/mol, I = g/mol 1.How many grams in 3.4 x molecules of H.
Nuclear Chemistry A subfield of chemistry dealing with radioactivity, nuclear processes and nuclear properties.
Lecture 12 Radioactive Isotopes Decay Equations Half Lives Useful Radiotracers in Oceanography Secular Equilibrium E & H Chpt 5.
Radiation Samar El-Sayed. Radiation Radiation is an energy in the form of electro-magnetic waves or particulate matter, traveling in the air.
Learning Outcomes Historical outline of radioactivity: work of Becquerel (discovery of radiation from uranium salts); Marie and Pierre Curie (discovery.
AMOLE Radioactivity. Science Park HS -- Honors Chemistry Early Pioneers in Radioactivity Roentgen: Discoverer of X- rays 1895 Becquerel: Discoverer of.
Chapter 9 pages And Chapter 18 pages
Nuclear Chemistry Chapter 25.
NUCLEAR CHEMISTRY 2F-1 (of 15) NUCLEONS – The particles found in the nucleus Protons (+) Neutrons (0) ATOMIC NUMBER (Z) – The number of protons in the.
Nuclear Chemistry Nine Mile Oswego, NY.  Radioisotope – an isotope that is radioactive  Example: Carbon-14  Radioactive isotopes can be naturally occurring,
Chemistry.
Nuclear chemistry.
The Nucleus and Radioactivity
Nuclear _____________of atom is changed Particles or energy is absorbed or emitted from nucleus Can involve one atom or multiple atoms New elements can.
Nuclear Chemistry Chapter 9.
Topic : Nuclear Physics
Principles and Applications
Fundamentals of Radiation
1 Nuclear Reactions and Radioactivity Part I. 2 Antoine-Henri Becquerel (1896) While experimenting with uranium compounds, he discovered that: The compounds.
Nuclear Chemistry Introduction Isotopes
CHAPTER 10 Nuclear Chemistry General, Organic, & Biological Chemistry Janice Gorzynski Smith.
Radioactivity. Henri Becquerel In 1896, Becquerel observed that uranium compounds emitted a penetrating radiation that passed through paper and affected.
General, Organic, and Biological Chemistry Fourth Edition Karen Timberlake 4.3 Radiation Measurement Chapter 4 Nuclear Chemistry © 2013 Pearson Education,
Dr. Bill Pezzaglia Nuclear Physics Updated: 2010May17 Modern Physics Series 1 INCOMPLETE DRAFT.
Unit IV: Nuclear Physics. What is Radioactivity?  Is the spontaneous breakdown of an unstable nucleus.  Results in the emission of particles or electromagnetic.
Chapter 9 Nuclear Radiation
Radioactivity Part 2 Nuclear Chemistry
Nuclear forces and Radioactivity Two forces are at work inside the nucleus of an atom.
1 Health Safety & Radiation Protection (RAD 453) Course : بسم الله الرّحمن الرّحيم Chapter 1: Fundamental Radiation Concepts Omrane KADRI, Ph.D.
Lecture 26 Atomic Structure and Radioactivity Chapter 29.1  29.4 Outline Properties of the Atomic Nucleus Binding Energy Radioactivity and Radioactive.
NUCLEAR CHEMISTRY An Energetic Concept. WHO DID WHAT Wilhelm Roentgen Laboratory generated phosphorescence X-rays.
Nuclear Chemistry. Nuclear Reactions  Chemical reactions  What can NOT change in a chemical reaction?  Nuclear Reactions: changes that occur in the.
Section 1Nuclear Changes Section 1: What is Radioactivity?
Radioisotopes.
Ch. 25 Nuclear Changes Begins on p. 35 of your PACKET.
Chapter 29:Nuclear Physics
1 Atomic Structure Protons 1 1 p ( amu) Neutrons 1 0 n ( amu) Electrons ( amu) Neon Ne ( amu)
Early Pioneers in Radioactivity Roentgen: Discoverer of X-rays 1895 Becquerel: Discoverer of Radioactivity 1896 The Curies: Discoverers of Radium and Polonium.
Nuclear Chemistry Unit 10. Radioactivity The spontaneous emission of radiation by an unstable atomic nucleus. Discovery Henri Becquerel-1896 Worked with.
Alpha and Beta Decay. Nuclear Reactions 1.Occur when nuclei emit particles and/or rays. 2.Atoms are often converted into atoms of another element. 3.May.
PHYSICS – Radioactive Decay
Early Pioneers in Radioactivity _________: Discoverer of X-rays 1895 _________: Discoverer of Radioactivity 1896 __________: Discoverers of Radium and.
Defining the Atom > A neutron walks into a bar and asks how much for a beer. Bartender replies “For you, no charge”.
Defining the Atom > A neutron walks into a bar and asks how much for a beer. Bartender replies “For you, no charge”.
Ch 21: Nuclear Chemistry. Radioactivity Wilhelm Roentgen made a big discovery in He found that invisible rays were emitted when electrons bombarded.
Lecture 6 Radioactive Isotopes
Lecture 8 Radioactive Isotopes
The Nuclear Atom In 1932, James Chadwick discovered a nuclear particle that was not affected by a charge. The nucleus contains PROTONS and.
SIJU PRAKASH ASST. PROFESSOR VIP-KUTCH Radiopharmaceuticals.
What is an isotope? Agenda for Tuesday Feb 8th Percent composition
General Physics (PHY 2140) Lecture 37 Modern Physics Nuclear Physics
General Physics (PHY 2140) Lecture 37 Modern Physics Nuclear Physics
Physics Chapter 33 and 34.
Presentation transcript:

Lecture 6 Radioactive Isotopes Definitions and types of decay Derivation of decay equations Half lives and mean lives Secular Equilibrium Useful radiotracers in oceanography E & H Chpt 5

The chart of the nuclides - decay Q. 230Th90 How many protons / neutrons?

Full Chart of the Nuclides Valley of Stability 1:1 line For 230Th N/P = 1.55

Radioisotopes and decay Definitions and Units Parent – Original radioactive atom Daughter – The product of decay Decay Chain – A series of sequential decays from one initial parent Decay is independent of chemistry and Temp and Pressure. Decay is only a property of the nucleus (see Chart of Nuclides) Types of Decay DP DN DAtomic Wt. Alpha a He2+ -2 -2 -4 Beta b e- + 1 -1 0 (n → P+ + e-) Gamma g “packets of excess energy” Measurements

The chart of the nuclides – decay pathways b decay X X a decay

Mathematical Formulation of Decay Decay Activity (A) = decays per time (e.g. minutes (dpm) or second (dps)) A = l N l = decay constant (t-1) N = # of atoms or concentration (atoms l-1) Remember 1 mol = 6.02 x 1023 atoms Units: Becquerel (Bq) = 1 dps (the official SI unit) Curie (Ci) = 3.7 x 1010 Bq = Activity of 1 gram of 226Ra Named after Pierre Curie See this link for the history: http://www.orau.org/ptp/articlesstories/thecurie.htm

Decay Equations (essential math lessons) Decay is proportional to the # of atoms present (first order) dN/dt = - N = AN where N = the number of atoms of the radioactive substance present at time t  = the first order decay constant (time-1) The number of parent atoms at any time t can be calculated as follows. The decay equation can be rearranged and integrated over a time interval. where No is the number of parent atoms present at time zero. Integration leads to or or

Decay Curve Both N and A decrease exponentially

Half Life The half life is defined as the time required for half of the atoms initially present to decay. After one half life: From the decay equation =  t1/2 ln (2) =  t1/2 0.693 =  t1/2 so Math note: -ln(1/2) = - (ln 1 – ln 2) = - ( 0 – ln 2) = + ln2 = 0.693

Mean Life = Average Life of an Atom = 1 / l = (1/0.693) t1/2 t = 1.44 t1/2 Q. Why is the mean life longer than the half life?

Isotopes used in Oceanography steady state transient U-Th series are shown on the next page. These tracers have a range of chemistries and half lives. Very useful for applications in oceanography.

Two forms of Helium 3He2 from beta decay of 3H1 (called tritium) and primordial from the mantle 4He2 the product of alpha decay from many elements How would you expect their distributions to vary in the ocean?

Example distributions of 3He

Q. Why is the inside of the earth hot? Q. What is the age of the earth? 5000 years or 5.5 x 109 years

238U decay products in the ocean U – conservative Th – particle reactive Ra – intermediate (like Ca) Rn = conservative Pb – particle reactive Q. What controls the concentration of 238U in SW?

Radon is a health hazzard! Radon source strength from rocks Why are some zones high (red)?

Parent-Daughter Relationships Radioactive Parent (A) Stable Daughter (B) A → B e.g. 14C → 15N (stable) Production of Daughter = Decay of Parent 2-box model l A A B Example: 14C → 15N (stable) t1/2 = 5730 years

Radioactive Parent (A) Radioactive Daughter (B) A → B → 2-box model lA lB A l A B l B source sink mass balance for B solution: solution after assuming NB = 0 at t = 0

Three Limiting Cases 1) t1/2(A) > t1/2(B) or lA < lB one important example: 2) t1/2(A) = t1/2(B) or lA = lB e.g. 226Ra → 222Rn 3) t1/2(A) < t1/2(B) or lA > lB 1600yrs 3.8 days Case #1: long half life of parent = small decay constant of parent SECULAR EQUILIBRIUM Activity of daughter equals activity of parent! Are concentrations also equal???

Q. Are concentrations also equal??? Example: 226Ra and 222Rn

Secular equilibrium (hypothetical) t1/2 daughter = 0.8 hr t1/2 parent =  Total Activity (parent+daughter) Parent doesn’t change Activity of parent and daughter at secular equilibrium daughter Activity (log scale) ! Daughter grows in with half life of the daughter! t1/2 time (hr)

Example: Grow in of 222Rn from 226Ra After 5 half lives Another way to plot After 5 half lives activity of daughter = 95% of activity of parent

Example: Rate of grow in Assume we have a really big wind storm over the ocean so that all the inert gas 222Rn is stripped out of the surface ocean by gas exchange. The activity of the parent of 222Rn, 226Ra, is not affected by the wind. Then the wind stops and 222Rn starts to increase (grows in) due to decay. Q. How many half lives will it take for the activity of 222Rn to equal 50% (and then 95%) of the 226Ra present? Answer: Use the following equation to calculate the activity A at time t

There is considerable exposure due to artificially produced sources! Possibly largest contributor is tobacco which contains radioactive 210Po which emits 5.3 MeV a particles with an half life of T1/2=138.4days.

Was Litvinenko (a former Russian spy) killed by 210Po Was Litvinenko (a former Russian spy) killed by 210Po?? A case study of 210Po Toxicity of Polonium 210 Weight-for-weight, polonium's toxicity is around 106 times greater than hydrogen cyanide (50 ng for Po-210 vs 50 mg for hydrogen cyanide). The main hazard is its intense radioactivity (as an alpha emitter), which makes it very difficult to handle safely - one gram of Po will self-heat to a temperature of around 500°C. It is also chemically toxic (with poisoning effects analogous with tellurium). Even in microgram amounts, handling 210Po is extremely dangerous, requiring specialized equipment and strict handling procedures. Alpha particles emitted by polonium will damage organic tissue easily if polonium is ingested, inhaled, or absorbed (though they do not penetrate the epidermis and hence are not hazardous if the polonium is outside the body). Acute effects The lethal dose (LD50) for acute radiation exposure is generally about 4.5 Sv. (Sv = Sievert which is a unit of dose equivalent). The committed effective dose equivalent 210Po is 0.51 µSv/Bq if ingested, and 2.5 µSv/Bq if inhaled. Since 210Po has an activity of 166 TBq per gram (1 gram produces 166×1012 decays per second), a fatal 4-Sv dose can be caused by ingesting 8.8 MBq (238 microcurie), about 50 nanograms (ng), or inhaling 1.8 MBq (48 microcurie), about 10 ng. One gram of 210Po could thus in theory poison 100 million people of which 50 million would die (LD50).

Body burden limit The maximum allowable body burden for ingested polonium is only 1,100 Bq (0.03 microcurie), which is equivalent to a particle weighing only 6.8 picograms. The maximum permissible concentration for airborne soluble polonium compounds is about 10 Bq/m3 (2.7 × 10-10 µCi/cm3). The biological half-life of polonium in humans is 30 to 50 days. The target organs for polonium in humans are the spleen and liver. As the spleen (150 g) and the liver (1.3 to 3 kg) are much smaller than the rest of the body, if the polonium is concentrated in these vital organs, it is a greater threat to life than the dose which would be suffered (on average) by the whole body if it were spread evenly throughout the body, in the same way as cesium or tritium. Notably, the murder of Alexander Litvinenko in 2006 was announced as due to 210Po poisoning. Generally, 210Po is most lethal when it is ingested. Litvinenko was probably the first person ever to die of the acute α-radiation effects of 210Po , although Irene Joliot-Curie was actually the first person ever to die from the radiation effects of polonium (due to a single intake) in the late 1950s. It is reasonable to assume that many people have died as a result of lung cancer caused by the alpha emission of polonium present in their lungs, either as a radon daughter or from tobacco smoke.