Chapter 19 Radioactivity and Nuclear Chemistry

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Presentation transcript:

Chapter 19 Radioactivity and Nuclear Chemistry Lecture Presentation Chapter 19 Radioactivity and Nuclear Chemistry Sherril Soman Grand Valley State University

Discovery of Radioactivity: Becquerel Becquerel discovered that certain minerals were constantly producing energy rays that could penetrate matter. Becquerel determined that 1. all the minerals that produced these rays contained uranium, and 2. the rays were produced even though the mineral was not exposed to outside energy. He called them uranic rays because they were emitted from minerals that contained uranium. Like X-rays Not related to phosphorescence

Discovery of Radioactivity: Marie Curie Marie Curie determined the rays were emitted from specific elements. She also discovered new elements by detecting their rays. Radium named for its green phosphorescence Polonium named for her homeland Because these rays were no longer just a property of uranium, she renamed it radioactivity.

Types of Radioactive Decay Rutherford discovered three types of rays: Alpha (a) rays Have a charge of +2 and a mass of 4 amu What we now know to be helium nucleus Beta (b) rays Have a charge of −1 and a negligible mass Electron-like Gamma (g) rays Form of light energy (not a particle like a and b) In addition, some unstable nuclei emit positrons. Like a positively charged electron Some unstable nuclei will undergo electrons capture. A low energy electron is pulled into the nucleus.

The daughter nuclide is the new nucleus that is made. Radioactivity Radioactive nuclei spontaneously decompose into smaller nuclei— radioactive decay. We say that radioactive nuclei are unstable. Decomposing involves the nuclide emitting a particle and/or energy. The parent nuclide is the nucleus that is undergoing radioactive decay. The daughter nuclide is the new nucleus that is made. All nuclides with 84 or more protons are radioactive.

Important Atomic Symbols

We describe nuclear processes with nuclear equations. Atomic numbers and mass numbers are conserved. The sum of the atomic numbers on both sides must be equal. The sum of the mass numbers on both sides must be equal.

Most ionizing, but least penetrating of the types of radioactivity Alpha Decay Occurs when an unstable nucleus emits a particle composed of two protons and two neutrons Most ionizing, but least penetrating of the types of radioactivity Loss of an alpha particle means the atomic number decreases by 2, and the mass number decreases by 4.

Occurs when an unstable nucleus emits an electron Beta Decay Occurs when an unstable nucleus emits an electron About 10 times more penetrating than α, but only about half the ionizing ability When an atom loses a β particle its atomic number increases by 1, and the mass number remains the same.

Gamma Emission Gamma (g) rays are high energy photons of light. No loss of particles from the nucleus No change in the composition of the nucleus Same atomic number and mass number Least ionizing, but most penetrating Generally occurs after the nucleus undergoes some other type of decay and the remaining particles rearrange

Positron Emission Positron has a charge of +1 and a negligible mass. Antielectron Similar to beta particles in their ionizing and penetrating ability When an atom loses a positron from the nucleus, its mass number remains the same, and its atomic number decreases by 1. Positrons result from a proton changing into a neutron.

Electron Capture Occurs when an inner orbital electron is pulled into the nucleus. No particle emission, but atom changes Same result as positron emission When a proton combines with the electron to make a neutron its mass number stays the same, and its atomic number decreases by 1.

Nonmedical Uses of Radioactive Isotopes Smoke detectors Am-241 Smoke blocks ionized air; breaks circuit Insect control Sterilize males Food preservation Radioactive tracers Follow progress of a “tagged” atom in a reaction Chemical analysis Neutron activation analysis

Nonmedical Uses of Radioactive Isotopes Authenticating art object Many older pigments and ceramics were made from minerals with small amounts of radioisotopes. Crime scene investigation Measure thickness or condition of industrial materials Corrosion Track flow through process Gauges in high temp processes Weld defects in pipelines Road thickness

Nuclear Equations In the nuclear equation, mass numbers and atomic numbers are conserved. We can use this fact to determine the identity of a daughter nuclide if we know the parent and mode of decay.

Balance the Following Nuclear Reactions  

N/Z Ratio The ratio of neutrons : protons is an important measure of the stability of the nucleus. If the N/Z ratio is too high, neutrons are converted to protons via b decay. If the N/Z ratio is too low, protons are converted to neutrons via positron emission or electron capture. Or via a decay, though not as efficiently

Valley of Stability For Z = 1 ⇒ 20, stable N/Z ≈ 1. For Z = 20 ⇒ 40, stable N/Z approaches 1.25. For Z = 40 ⇒ 80, stable N/Z approaches 1.5. For Z > 83, there are no stable nuclei. Nuclei above the belt usually undergo beta emission. Nuclei below the belt usually undergo positron emission or electron capture. 19

Decay Series In nature, often one radioactive nuclide changes into another radioactive nuclide. That is, the daughter nuclide is also radioactive. All atoms with Z > 83 are radioactive. All of the radioactive nuclides that are produced one after the other until a stable nuclide is made is called a decay series.

U-238 Decay Series

Rate of Radioactive Decay The rate of change in the amount of radioactivity is constant, and is different for each radioactive “isotope.” Change in radioactivity measured with Geiger counter Counts per minute Each radionuclide had a particular length of time it required to lose half its radioactivity—a constant half-life. We know that processes with a constant half-life follow first order kinetic rate laws. The rate of radioactive change was not affected by temperature. In other words, radioactivity is not a chemical reaction!

Kinetics of Radioactive Decay Rate = kN N = number of radioactive nuclei The shorter the half-life, the more nuclei decay every second; therefore, we say the sample is “hotter.”

Half-Lives of Various Nuclides

Half-Life Half of the radioactive atoms decay each half-life.

Kinetics of Radioactive Decay Radioactive decay is a first order process. Nt = number of radioactive nuclei at time, t N0 = initial number of radioactive nuclei

Radiometric Dating The change in the amount of radioactivity of a particular radionuclide is predictable and not affected by environmental factors. By measuring and comparing the amount of a parent radioactive isotope and its stable daughter, we can determine the age of the object. Using the half-life and the previous equations Mineral (geological) dating Compare the amount of U-238 to Pb-206 in volcanic rocks and meteorites. Dates Earth to between 4.0 and 4.5 billion years old Compare amount of K-40 to Ar-40.

Radiocarbon Dating All things that are alive or were once alive contain carbon. Three isotopes of carbon exist in nature, one of which, C-14, is radioactive. C-14 radioactive with half-life = 5730 years Atmospheric chemistry keeps producing C-14 at nearly the same rate it decays.

Radiocarbon Dating While still living, C-14/C-12 is constant because the organism replenishes its supply of carbon. CO2 in air is the ultimate source of all C in an organism. Once the organism dies the C-14/C-12 ratio decreases. By measuring the C-14/C-12 ratio in a once living artifact and comparing it to the C-14/C-12 ratio in a living organism, we can tell how long ago the organism was alive. The limit for this technique is 50,000 years old. About 9 half-lives, after which radioactivity from C-14 will be below the background radiation