1. Chapter 19 Nuclear Reactions

2. The Nucleus Remember that the nucleus is comprised of the two nucleons, protons and neutrons. The number of protons is the atomic number. The number of protons and neutrons together is effectively the mass of the atom.

3. Isotopes Not all atoms of the same element have the same mass due to different numbers of neutrons in those atoms. There are three naturally occurring isotopes of uranium:  Uranium-234  Uranium-235  Uranium-238

4. Radioactivity It is not uncommon for some nuclides of an element to be unstable, or radioactive. We refer to these as radionuclides. There are several ways radionuclides can decay into a different nuclide.

5. Alpha Decay: Loss of an  -particle (a helium nucleus) He 4242 U 238 92  U 234 90 He 4242 +

6. Beta Decay: Loss of a  -particle (a high energy electron) Where does the  -particle come from?  0−10−1 e 0−10−1 or I 131 53 Xe 131 54  + e 0−10−1

7. Positron Emission: Loss of a positron (a particle that has the same mass as but opposite charge than an electron) Where does the positron come from? e 0101 C 11 6  B 11 5 + e 0101

8. Gamma Emission: Loss of a  -ray (high-energy radiation that almost always accompanies the loss of a nuclear particle)  0000

9. Electron Capture (K-Capture) Addition of an electron to a proton in the nucleus  As a result, a proton is transformed into a neutron. p 1111 + e 0−10−1  n 1010

10. Neutron-Proton Ratios Any element with more than one proton (i.e., anything but hydrogen) will have repulsions between the protons in the nucleus. A strong nuclear force helps keep the nucleus from flying apart.

11. Neutron-Proton Ratios Neutrons play a key role stabilizing the nucleus. Therefore, the ratio of neutrons to protons is an important factor.

12. Neutron-Proton Ratios For smaller nuclei (Z  20) stable nuclei have a neutron-to-proton ratio close to 1:1.

13. Neutron-Proton Ratios As nuclei get larger, it takes a greater number of neutrons to stabilize the nucleus.

14. Stable Nuclei The shaded region in the figure shows what nuclides would be stable, the so- called belt of stability.

15. Stable Nuclei Nuclei above this belt have too many neutrons. They tend to decay by emitting beta particles.

16. Stable Nuclei Nuclei below the belt have too many protons. They tend to become more stable by positron emission or electron capture.

17. Stable Nuclei There are no stable nuclei with an atomic number greater than 83. These nuclei tend to decay by alpha emission.

18. Radioactive Series Large radioactive nuclei cannot stabilize by undergoing only one nuclear transformation. They undergo a series of decays until they form a stable nuclide (often a nuclide of lead).

19. Nuclear Transformations Nuclear transformations can be induced by accelerating a particle and colliding it with the nuclide.

20. Particle Accelerators These particle accelerators are enormous, having circular tracks with radii that are miles long.

21. Kinetics of Radioactive Decay The kinetics of radioactive decay obey this equation: = kt NtN0NtN0 ln The half-life of such a process is: = t 1/2 0.693 k Comparing the amount of a radioactive nuclide present at a given point in time with the amount normally present, one can find the age of an object.

22. Measuring Radioactivity One can use a device like this Geiger counter to measure the amount of activity present in a radioactive sample. The ionizing radiation creates ions, which conduct a current that is detected by the instrument.

23. Energy in Nuclear Reactions There is a tremendous amount of energy stored in nuclei. Einstein’s famous equation, E = mc 2, relates directly to the calculation of this energy. In the types of chemical reactions we have encountered previously, the amount of mass converted to energy has been minimal. However, these energies are many thousands of times greater in nuclear reactions.

24. Energy in Nuclear Reactions For example, the mass change for the decay of 1 mol of uranium-238 is −0.0046 g. The change in energy,  E, is then  E = (  m) c 2  E = (−4.6  10 −6 kg)(3.00  10 8 m/s) 2  E = −4.1  10 11 J

25. Nuclear Fission How does one tap all that energy? Nuclear fission is the type of reaction carried out in nuclear reactors.

26. Bombardment of the radioactive nuclide with a neutron starts the process. Neutrons released in the transmutation strike other nuclei, causing their decay and the production of more neutrons. This process continues in what we call a nuclear chain reaction. Nuclear Fission

27. If there are not enough radioactive nuclides in the path of the ejected neutrons, the chain reaction will die out. Therefore, there must be a certain minimum amount of fissionable material present for the chain reaction to be sustained: Critical Mass.

28. Nuclear Reactors In nuclear reactors the heat generated by the reaction is used to produce steam that turns a turbine connected to a generator.

29. SCRAM The sudden shutting down of a nuclear reactor, usually by rapid insertion of control rods, either automatically or manually by the reactor operator. May also be called a reactor trip. It is actually an acronym for "safety control rod axe man," the worker assigned to insert the emergency rod on the first reactor (the Chicago Pile) in the U.S. http://www.nrc.gov/reading-rm/basic-ref/glossary/scram.html http://www.nrc.gov/reading-rm/basic-ref/glossary/scram.html

30. Nuclear Reactors The reaction is kept in check by the use of control rods. These block the paths of some neutrons, keeping the system from reaching a dangerous supercritical mass.

31. Fissionable Material fissionable isotopes include U-235, Pu- 239, and Pu-240 natural uranium is less than 1% U-235  rest mostly U-238  not enough U-235 to sustain chain reaction to produce fissionable uranium the natural uranium must be enriched in U- 235  to about 7% for “weapons grade”  to about 3% for reactor grade

32. Nuclear Power Plants - Core the fissionable material is stored in long tubes, called fuel rods, arranged in a matrix  subcritical between the fuel rods are control rods made of neutron absorbing material  B and/or Cd  neutrons needed to sustain the chain reaction the rods are placed in a material to slow down the ejected neutrons, called a moderator  allows chain reaction to occur below critical mass

33. Pressurized Light Water Reactor design used in US (GE, Westinghouse) water is both the coolant and moderator water in core kept under pressure to keep it from boiling fuel is enriched uranium  subcritical containment dome of concrete

34. Cooling Tower

35. Nuclear Power Nuclear reactors use fission to generate electricity  About 20% of US electricity  The fission of U-235 produces heat The heat boils water, turning it to steam The steam turns a turbine, generating electricity

36. Nuclear Power Plants vs. Coal-Burning Power Plants Use about 50 kg of fuel to generate enough electricity for 1 million people No air pollution Use about 2 million kg of fuel to generate enough electricity for 1 million people Produces NO 2 and SO x that add to acid rain Produces CO 2 that adds to the greenhouse effect

37. Concerns About Nuclear Power core melt-down  water loss from core, heat melts core  China Syndrome  Chernobyl waste disposal  waste highly radioactive  reprocessing, underground storage?  Federal High Level Radioactive Waste Storage Facility at Yucca Mountain, Nevada transporting waste how do we deal with nuclear power plants that are no longer safe to operate?

38. Fusion + + 2 1H1H 3 1H1H 4 2 He 1 0n0n deuterium + tritiumhelium-4 + neutron

39. Nuclear Fusion Fusion is the combining of light nuclei to make a heavier one The sun uses the fusion of hydrogen isotopes to make helium as a power source Requires high input of energy to initiate the process  Because need to overcome repulsion of positive nuclei Produces 10x the energy per gram as fission No radioactive byproducts Unfortunately, the only currently working application is the H-bomb

40. Nuclear Fusion Fusion would be a superior method of generating power.  The good news is that the products of the reaction are not radioactive.  The bad news is that in order to achieve fusion, the material must be in the plasma state at several million kelvins. Tokamak apparati like the one shown at the right show promise for carrying out these reactions. They use magnetic fields to heat the material.

41. Radiation Exposure

42. Medical Uses of Radioisotopes, Diagnosis radiotracers  certain organs absorb most or all of a particular element  can measure the amount absorbed by using tagged isotopes of the element and a Geiger counter  use radioisotope with short half-life  use radioisotope low ionizing beta or gamma

44. Medical Uses of Radioisotopes, Diagnosis PET scan  positron emission tomography  C-11 in glucose  brain scan and function

45. Medical Uses of Radioisotopes, Treatment - Radiotherapy cancer treatment  cancer cells more sensitive to radiation than healthy cells 1.brachytherapy place radioisotope directly at site of cancer 2.teletherapy use gamma radiation from Co-60 outside to penetrate inside 3.radiopharmaceutical therapy use radioisotopes that concentrate in one area of the body