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Jeffrey Mack California State University, Sacramento Chapter 23 Nuclear Chemistry
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Chapter 23 Nuclear Chemistry

Feb 26, 2016

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Chapter 23 Nuclear Chemistry. Nuclear Chemistry. Images of a human heart before and after stress detecting gamma rays from radioactive Tc-99m . Atomic Composition. Protons (+1) electrical charge mass = 1.672623  10  24 g mass = 1.007 atomic mass units ( amu ) Electrons - PowerPoint PPT Presentation
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Page 1: Chapter 23 Nuclear Chemistry

Jeffrey MackCalifornia State University,

Sacramento

Chapter 23

Nuclear Chemistry

Page 2: Chapter 23 Nuclear Chemistry

Images of a human heart before and after stress detecting gamma rays from radioactive Tc-99m

Nuclear Chemistry

Page 3: Chapter 23 Nuclear Chemistry

• Protons– (+1) electrical charge– mass = 1.672623 1024 g– mass = 1.007 atomic mass units (amu)

• Electrons– negative electrical charge– relative mass = 0.0005 amu

• Neutrons– no electrical charge– mass = 1.009 amu

Atomic Composition

Page 4: Chapter 23 Nuclear Chemistry

• Isotopes are atoms of the same element (same Z) but different mass numbers (A).

• Boron-10:5 protons and 5 neutrons: • Boron-11: 5 protons and 6 neutrons:

10B

11B

Isotopes

Page 5: Chapter 23 Nuclear Chemistry

• The isolation and characterization of radium & polonium by Marie Curie was one of milestones of chemistry.

• It is a credit to her skills as a chemist that she was able to isolate only a single gram of radium from 7 tons of uranium ore.

Marie and Pierre Curie

Radioactivity

Page 6: Chapter 23 Nuclear Chemistry

• -particles can be stopped by paper.• -particles require at least a cm of lead (Pb).• -particles require at least 10 cm of lead (Pb).

Energy: > >

Natural Radioactivity

Page 7: Chapter 23 Nuclear Chemistry

Penetrating Ability

Page 8: Chapter 23 Nuclear Chemistry

• Ernest Rutherford isolated Radium forms Radon gas while studying alpha particle emission.

• 1902 Rutherford and Soddy proposed radioactivity was the result of the natural change of the isotope of one element into an isotope of a different element.

Nuclear Reactions

Page 9: Chapter 23 Nuclear Chemistry

Alpha emission

• Nucleons must be conserved in any nuclear reaction.

• In emission, the mass number (A) decreases by 4 and the atomic number (Z) decreases by 2.

Nuclear Reactions

Page 10: Chapter 23 Nuclear Chemistry

Beta emission

In emission, the mass number (A) remains unchanged and the atomic number (Z) decreases by 1.

Nuclear Reactions

Page 11: Chapter 23 Nuclear Chemistry

Radioactive Decay Series

Page 12: Chapter 23 Nuclear Chemistry

Positron (positive electron) emission

207 207

• Positrons have the mass of an electron, but positive charge. They are the antimatter analog of an electron.

• Positron emission arises from “electron capture”.• An inner shell electron is absorbed by the nucleolus

converting a proton into a neutron along with an emitted positron.

Other Types of Nuclear Reactions

Page 13: Chapter 23 Nuclear Chemistry

• H is most abundant element in the universe.• H represents 88.6% of all atoms• He represents 11.3% of all atoms• Together 99.9% of all atom & 99% of mass of

the universe.

Stability of Nuclei

Page 14: Chapter 23 Nuclear Chemistry

• Hydrogen: – 1

1H, protium– 2

1H, deuterium– 3

1H, tritium (radioactive)

• Helium, 42He

• Lithium, 63Li and 7

3Li• Boron, 10

5B and 115B

• Iron– 54

26Fe, 5.82% abundant

– 5626Fe, 91.66%

abundant– 57

26Fe, 2.19% abundant

– 5826Fe, 0.33%

abundant

Isotopes

Page 15: Chapter 23 Nuclear Chemistry

• 209Bi with 83 protons and 126 neutrons is the heaviest naturally occurring non-radioactive isotope.

• There are 83 x 126 = 10,458 possible isotopes.

• Why do so few exist in nature?

Stability of Nuclei

Page 16: Chapter 23 Nuclear Chemistry

• Up to Z = 20 (Ca) stable isotopes often have the same # of neutrons and protons. Only H and He-3 have more protons than neutrons.

• Beyond Ca, the ratio of neutrons to protons is >1.• As Z increases, the n:p ratio deviates further from 1:1• Above Bi all isotopes are radioactive. Fission leads to

smaller particles, the heavier the nucleus the greater the rate.

• Above Ca: elements of EVEN Z have more stable isotopes than ODD Z elements.

• The more stable isotopes have an EVEN number of neutrons.

Stability of Nuclei

Page 17: Chapter 23 Nuclear Chemistry

Out of > 300 stable isotopes:

Even Odd

Odd

Even

ZN

157 52

50 5

3115P

199F

21H, 6

3Li, 105B, 14

7N, 18073Ta

Stability of Nuclei

Page 18: Chapter 23 Nuclear Chemistry

• The trend suggests some PAIRING of NUCLEONS

• There are “nuclear magic numbers”2 He 28 Ni8 O 50 Sn20 Ca 82 Pb

Even Odd

Odd

Even

ZN

157 52

50 5

Stability of Nuclei

Page 19: Chapter 23 Nuclear Chemistry

Band of Stability and Radioactive Decay

Isotopes with low n/p ratio, below band of stability decay, decay by positron emission or electron capture

Page 20: Chapter 23 Nuclear Chemistry

• The energy required to separate the nucleus of an atom into protons and neutrons.

• For deuterium, 21H

21H 1

1p + 10n Eb = 2.15 108 kJ/mol

• Eb per nucleon = Eb/2 nucleons= 1.08 108 kJ/mol nucleons

Binding Energy, Eb

Page 21: Chapter 23 Nuclear Chemistry

For deuterium, 21H: 2

1H 11p + 1

0n

Mass of 21H: = 2.01410 g/mol

Mass of proton: = 1.007825 g/molMass of neutron: = 1.008665 g/mol∆m: = 0.00239 g/molFrom Einstein’s equation: Eb = (∆m)c2

= 2.15 x 108 kJ/molEb per nucleon = Eb/2 nucleons

= 1.08 108 kJ/mol nucleons

Calculate Binding Energy

Page 22: Chapter 23 Nuclear Chemistry

Binding Energy/Nucleon

Page 23: Chapter 23 Nuclear Chemistry

• The HALF-LIFE of an isotope is the time it takes for 1/2 a sample to decay from its initial amount.

• The rate of a nuclear transformation depends only on the “reactant” concentration.

• The decay and half-life for a nuclear reaction follows first order kinetics.

Half-Life

Page 24: Chapter 23 Nuclear Chemistry

After each successive half-life, one half of the original amount remains.

Half-Life

Page 25: Chapter 23 Nuclear Chemistry

Activity (A) = Disintegrations/time = (k)(N) where N is the number of atomsDecay follows first order kinetics:

The half-life of radioactive decay is t1/2 = 0.693/k

Kinetics of Radioactive Decay

Page 26: Chapter 23 Nuclear Chemistry

Willard Libby (1908-1980)Libby received the 1960 Nobel Prize in chemistry for developing carbon-14 dating techniques. He is shown here with the apparatus he used. Carbon-14 dating is widely used in fields such as anthropology and archeology.

Radiocarbon Dating

Page 27: Chapter 23 Nuclear Chemistry

Radioactive C-14 is formed in the upper atmosphere by nuclear reactions initiated by neutrons in cosmic radiation:14N + 1

0n 14C + 1HThe C-14 is oxidized to CO2, which circulates through the biosphere.When a plant dies, the C-14 is not replenished.But the C-14 continues to decay with t1/2 = 5730 years.Activity of a sample can be used to date the sample.

Radiocarbon Dating

Page 28: Chapter 23 Nuclear Chemistry

• New elements or new isotopes of known elements are produced by bombarding an atom with subatomic particles such as a protons or neutrons, or even a heavier particles such as 4He and 11B.

• Reactions using neutrons are called n, reactions because a -ray is usually emitted.

• Radioisotopes used in medicine are often made by n, reactions.

Artificial Nuclear Reactions

Page 29: Chapter 23 Nuclear Chemistry

• An Example of a n, reaction is production of radioactive 32P.

• 32P is used in studies of phosphorous uptake in the body.

Artificial Nuclear Reactions

Page 30: Chapter 23 Nuclear Chemistry

Elements beyond 92 (transuranium) are made via n, reactions.

Transuranium Elements

Page 31: Chapter 23 Nuclear Chemistry

106Sg

Transuranium Elements & Glenn Seaborg

Page 32: Chapter 23 Nuclear Chemistry

Nuclear Fission

Page 33: Chapter 23 Nuclear Chemistry

Fission chain reaction has three general steps:Initiation:

Reaction of a single atom starts the chain (e.g., 235U + neutron)

Propagation:236U fission releases neutrons that initiate other fissions

Termination.Consumption of the fissionable material is completed

Nuclear Fission

Page 34: Chapter 23 Nuclear Chemistry

109Mt

Nuclear Fission & Lise Meitner

Page 35: Chapter 23 Nuclear Chemistry

• Currently about 103 nuclear power plants in the U.S. and about 435 worldwide.

• 17% of the world’s energy comes from nuclear.

Nuclear Fission & Power

Page 36: Chapter 23 Nuclear Chemistry

• Curie: 1 Ci = 3.7 1010 distintegrations/s (dps)

• SI unit is the becquerel: 1 Bq = 1 dps• Rad: measures amount of energy absorbed

1 rad = 0.01 J absorbed/kg tissue• Rem: “roentgen equivalent man” based on

amount and type of radiation. • Quantifies biological tissue damage, usually

represented “millirems”.

Units for Measuring Radiation

Page 37: Chapter 23 Nuclear Chemistry

Effects of Radiation

Page 38: Chapter 23 Nuclear Chemistry

Effects of Radiation

Page 39: Chapter 23 Nuclear Chemistry

Nuclear Medicine: Imaging

Page 40: Chapter 23 Nuclear Chemistry

Technetium-99m is used in more than 85% of the diagnostic scans done in hospitals each year. Synthesized on-site from Mo-99.

99m43Tc decays to 99

43Tc giving off a -ray.The half-life of the radioisotope is 6.01 hrs.Once ingested, the Tc-99m concentrates in areas of high activity such as the thyroid. -ray imagining detects its presence.

Nuclear Medicine: Imaging

Page 41: Chapter 23 Nuclear Chemistry

Imaging of a heart using Tc-99m before and after exercise.

Nuclear Medicine: Imaging

Page 42: Chapter 23 Nuclear Chemistry

• 10B isotope (not 11B) has the ability to capture slow neutrons

• In BNCT, tumor cells preferentially take up a boron compound, and subsequent irradiation by slow neutrons kills the cells via the energetic 10B 7Li neutron capture reaction (that produces a photon and an alpha particle)

• 10B + 1n 7Li + 4He + photon

BNCTBoron Neutron Capture Therapy

Page 43: Chapter 23 Nuclear Chemistry

• Food can be irradiated with rays from 60Co or 137Cs.

• Irradiation retards the growth of bacteria, molds and yeasts.

• Irradiated milk has a shelf life of 3 mo. without refrigeration.

• USDA has approved irradiation of meats and eggs.

Food Irradiation