CHAPTER 22 Nuclear Chemistry I. The Nucleus (p. 701 - 704) I. The Nucleus (p. 701 - 704) I IV III II Courtesy Christy Johannesson www.nisd.net/communicationsarts/pages/chem.

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CHAPTER 22 Nuclear Chemistry I. The Nucleus (p ) I. The Nucleus (p ) I IV III II Courtesy Christy Johannesson

Nuclear Binding Energy Unstable nuclides are radioactive and undergo radioactive decay. U x10 8 9x10 8 8x10 8 7x10 8 6x10 8 5x10 8 4x10 8 3x10 8 2x10 8 1x10 8 Fe-56 B-10 Li-6 H-2 He Mass number Binding energy per nucleon (kJ/mol)

CHAPTER 22 Nuclear Chemistry II. Radioactive Decay (p ) II. Radioactive Decay (p ) I IV III II Courtesy Christy Johannesson

Types of Radiation  Alpha particle (  )  helium nucleus paper 2+  Beta particle (  - )  electron 1- lead  Positron (  + )  positron 1+  Gamma (  )  high-energy photon 0 concrete Courtesy Christy Johannesson

Nuclear Decay  Alpha Emission parent nuclide daughter nuclide alpha particle Numbers must balance!! Courtesy Christy Johannesson

Nuclear Decay  Beta Emission electron  Positron Emission positron Courtesy Christy Johannesson

Nuclear Decay  Electron Capture electron  Gamma Emission  Usually follows other types of decay.  Transmutation  One element becomes another. Courtesy Christy Johannesson

Neutrons (A-Z) Protons (Z) Nuclear Decay  Why nuclides decay…  need stable ratio of neutrons to protons DECAY SERIES TRANSPARENCY Courtesy Christy Johannesson  P = N e - capture or e + emission  stable nuclei

Neutrons (A-Z) P = N Protons (Z) stable nuclei e - capture or e + emission   Neutrons (A-Z) P = N Protons (Z) stable nuclei  Why nuclides decay…  need stable ratio of neutrons to protons Nuclear Decay

Half-lifeHalf-life  Half-life (t ½ )  Time required for half the atoms of a radioactive nuclide to decay.  Shorter half-life = less stable. 1/1 1/2 1/4 1/8 1/16 0 Ratio of Remaining Potassium-40 Atoms to Original Potassium-40 Atoms 0 1 half-life half-lives half-lives half-lives 5.2 Time (billions of years) Newly formed rock Potassium Argon Calcium

Half-lifeHalf-life m f :final mass m i :initial mass n:# of half-lives Courtesy Christy Johannesson

Half-lifeHalf-life  Fluorine-21 has a half-life of 5.0 seconds. If you start with 25 g of fluorine-21, how many grams would remain after 60.0 s? GIVEN: t ½ = 5.0 s m i = 25 g m f = ? total time = 60.0 s n = 60.0s ÷ 5.0s =12 WORK : m f = m i (½) n m f = (25 g)(0.5) 12 m f = g Courtesy Christy Johannesson

CHAPTER 22 Nuclear Chemistry III. Fission & Fusion (p ) III. Fission & Fusion (p ) I IV III II Courtesy Christy Johannesson

F ission  splitting a nucleus into two or more smaller nuclei  1 g of 235 U = 3 tons of coal Courtesy Christy Johannesson

F ission  chain reaction - self-propagating reaction  critical mass - mass required to sustain a chain reaction Courtesy Christy Johannesson

FusionFusion  combining of two nuclei to form one nucleus of larger mass  thermonuclear reaction – requires temp of 40,000,000 K to sustain  1 g of fusion fuel = 20 tons of coal  occurs naturally in stars Courtesy Christy Johannesson

Fission vs. Fusion  235 U is limited  danger of meltdown  toxic waste  thermal pollution  fuel is abundant  no danger of meltdown  no toxic waste  not yet sustainable FISSIONFISSION FUSIONFUSION Courtesy Christy Johannesson

CHAPTER 22 Nuclear Chemistry IV. Applications (p ) IV. Applications (p ) I IV III II Courtesy Christy Johannesson

Nuclear Power  Fission Reactors Cooling Tower Courtesy Christy Johannesson

Nuclear Power  Fission Reactors Courtesy Christy Johannesson

Nuclear Power  Fusion Reactors (not yet sustainable) Courtesy Christy Johannesson ITER (International Thermonuclear Experimental Reactor) TOROIDAL FIELD COILS (produces the magnetic field which confines the plasma) BLANKET (provides neutron shielding and converts fusion energy into hot, high pressure fluid) FUSION PLASMA CHAMBER (where the fusion reactions occur) Height100 feet Diameter100 feet Fusion power1100 Megawatts

Nuclear Power  Fusion Reactors (not yet sustainable) Tokamak Fusion Test Reactor Princeton University National Spherical Torus Experiment Courtesy Christy Johannesson

Synthetic Elements  Transuranium Elements  elements with atomic #s above 92  synthetically produced in nuclear reactors and accelerators  most decay very rapidly Courtesy Christy Johannesson

Natural and artificial radioactivity Natural radioactivity Isotopes that have been here since the earth formed. Example - Uranium Produced by cosmic rays from the sun. Example – carbon-14 Man-made Radioisotopes Made in nuclear reactors when we split atoms (fission). Produced using cyclotrons, linear accelerators,…

Copyright © 2007 Pearson Benjamin Cummings. All rights reserved. Positive particle source Alternating voltage Particle beam Vacuum Target

Radioactive Dating  half-life measurements of radioactive elements are used to determine the age of an object  decay rate indicates amount of radioactive material  EX: 14 C - up to 40,000 years 238 U and 40 K - over 300,000 years Courtesy Christy Johannesson

Nuclear Medicine  Radioisotope Tracers  absorbed by specific organs and used to diagnose diseases  Radiation Treatment  larger doses are used to kill cancerous cells in targeted organs  internal or external radiation source Radiation treatment using  -rays from cobalt-60. Courtesy Christy Johannesson

Nuclear Weapons  Atomic Bomb  chemical explosion is used to form a critical mass of 235 U or 239 Pu  fission develops into an uncontrolled chain reaction  Hydrogen Bomb  chemical explosion  fission  fusion  fusion increases the fission rate  more powerful than the atomic bomb Courtesy Christy Johannesson

OthersOthers  Food Irradiation   radiation is used to kill bacteria  Radioactive Tracers  explore chemical pathways  trace water flow  study plant growth, photosynthesis  Consumer Products  ionizing smoke detectors Am Courtesy Christy Johannesson

Simplified diagram of fission bomb Subcritical masses Chemical Explosive Critical mass

Simplified diagram of fission bomb

Subcritical masses

Chemical Explosive

Critical mass Copyright © 2007 Pearson Benjamin Cummings. All rights reserved.