{"id":3363,"date":"2019-04-23T12:33:57","date_gmt":"2019-04-23T12:33:57","guid":{"rendered":"https:\/\/courses.lumenlearning.com\/suny-introductorychemistry\/chapter\/radioactivity-2\/"},"modified":"2019-04-29T13:12:17","modified_gmt":"2019-04-29T13:12:17","slug":"radioactivity-2","status":"publish","type":"chapter","link":"https:\/\/courses.lumenlearning.com\/suny-introductorychemistry\/chapter\/radioactivity-2\/","title":{"raw":"Radioactivity","rendered":"Radioactivity"},"content":{"raw":"<div id=\"ball-ch15_s01\" class=\"section\" lang=\"en\">\r\n<div id=\"ball-ch15_s01_n01\" class=\"learning_objectives editable block\">\r\n<div class=\"bcc-box bcc-highlight\">\r\n<h3>Learning Objectives<\/h3>\r\n1. Define and give examples of the major types of radioactivity.\r\n\r\n<\/div>\r\n<\/div>\r\n<p id=\"ball-ch15_s01_p01\" class=\"para editable block\">We saw in <a class=\"xref\" href=\"ball-ch03#ball-ch03\">Chapter 3 \"Atoms, Molecules, and Ions\"<\/a> that atoms are composed of subatomic particles\u2014protons, neutrons, and electrons. Protons and neutrons are located in the nucleus and provide most of the mass of an atom, while electrons circle the nucleus in shells and subshells and account for an atom\u2019s size.<\/p>\r\n<p id=\"ball-ch15_s01_p02\" class=\"para editable block\">We also introduced in <a class=\"xref\" href=\"ball-ch03#ball-ch03\">Chapter 3 \"Atoms, Molecules, and Ions\"<\/a> the notation for succinctly representing an isotope of a particular atom:<\/p>\r\n<span class=\"informalequation block\"><sub>6<\/sub><sup>12<\/sup>C<\/span>\r\n<p id=\"ball-ch15_s01_p03\" class=\"para editable block\">The element in this example, represented by the symbol C, is carbon. Its atomic number, 6, is the subscript next to the symbol and is the number of protons in the atom. The mass number, the superscript next to the symbol, is the sum of the number of protons and neutrons in the nucleus of this particular isotope. In this case, the mass number is 12, which means that the number of neutrons in the atom is 12 \u2212 6 = 6 (that is, the mass number of the atom minus the number of protons in the nucleus equals the number of neurons). Occasionally, the atomic number is omitted in this notation because the symbol of the element itself conveys its characteristic atomic number. The two isotopes of hydrogen\u2014<sup class=\"superscript\">2<\/sup>H and <sup class=\"superscript\">3<\/sup>H\u2014are given their own names and symbols: deuterium (D) and tritium (T), respectively.<\/p>\r\n<p id=\"ball-ch15_s01_p04\" class=\"para editable block\">Atomic theory in the nineteenth century presumed that nuclei had fixed compositions. But in 1896, the French scientist Henri Becquerel found that a uranium compound placed near a photographic plate made an image on the plate, even if the compound was wrapped in black cloth. He reasoned that the uranium compound was emitting some kind of radiation that passed through the cloth to expose the photographic plate. Further investigations showed that the radiation was a combination of particles and electromagnetic rays, with its ultimate source being the atomic nucleus. These emanations were ultimately called, collectively, <span class=\"margin_term\"><a class=\"glossterm\">radioactivity<\/a><\/span>.<\/p>\r\n<p id=\"ball-ch15_s01_p05\" class=\"para block\">There are three main forms of radioactive emissions. The first is called an <span class=\"margin_term\"><a class=\"glossterm\">alpha particle<\/a><\/span>, which is symbolized by the Greek letter \u03b1. An alpha particle is composed of two protons and two neutrons and is the same as a helium nucleus. (We often use <sub>2<\/sub><sup>4<\/sup>He\u00a0to represent an alpha particle.) It has a 2+\u00a0charge. When a radioactive atom emits an alpha particle, the original atom\u2019s atomic number decreases by two (because of the loss of two protons), and its mass number decreases by four (because of the loss of four nuclear particles). We can represent the emission of an alpha particle with a chemical equation\u2014for example, the alpha-particle emission of uranium-235 is as follows:<\/p>\r\n<span class=\"informalequation block\"><sub>92<\/sub><sup>235<\/sup>U \u2192\u00a0<sub>2<\/sub><sup>4<\/sup>He+<sub>90<\/sub><sup>231<\/sup>Th<\/span>\r\n<p id=\"ball-ch15_s01_p06\" class=\"para block\">Rather than calling this equation a chemical equation, we call it a <span class=\"margin_term\"><a class=\"glossterm\">nuclear equation<\/a><\/span>\u00a0to emphasize that the change occurs in an atomic nucleus. How do we know that a product of this reaction is<sub>90<\/sub><sup>231<\/sup>Th? We use the law of conservation of matter, which says that matter cannot be created or destroyed. This means we must have the same number of protons and neutrons on both sides of the nuclear equation. If our uranium nucleus loses 2 protons, there are 90 protons remaining, identifying the element as thorium. Moreover, if we lose four nuclear particles of the original 235, there are 231 remaining. Thus we use subtraction to identify the isotope of the Th atom\u2014in this case, <sub>90<\/sub><sup>231<\/sup>Th<span class=\"inlineequation\">.<\/span><\/p>\r\n<p id=\"ball-ch15_s01_p07\" class=\"para block\">Chemists often use the names <span class=\"margin_term\"><a class=\"glossterm\">parent isotope<\/a><\/span>\u00a0and <span class=\"margin_term\"><a class=\"glossterm\">daughter isotope<\/a><\/span>\u00a0to represent the original atom and the product other than the alpha particle. In the previous example,\u00a0<sub>92<\/sub><sup>235<\/sup>U<\/p>\r\n<p id=\"ball-ch15_s01_p08\" class=\"para block\">is the parent isotope, and\u00a0<sub>90<\/sub><sup>231<\/sup>Th\u00a0is the daughter isotope. When one element changes into another in this manner, it undergoes <span class=\"margin_term\"><a class=\"glossterm\">radioactive decay<\/a><\/span>.<\/p>\r\n\r\n<div class=\"textbox shaded\">\r\n<h3 class=\"title\">Example 1<\/h3>\r\n<p id=\"ball-ch15_s01_p09\" class=\"para\">Write the nuclear equation that represents the radioactive decay of radon-222 by alpha particle emission and identify the daughter isotope.<\/p>\r\n<p class=\"simpara\">Solution<\/p>\r\n<p id=\"ball-ch15_s01_p10\" class=\"para\">Radon has an atomic number of 86, so the parent isotope is represented as Th<span class=\"inlineequation\"> <sub>86<\/sub><sup>222<\/sup>Rn.<\/span> We represent the alpha particle as <span class=\"inlineequation\"><sub>2<\/sub><sup>4<\/sup>He<\/span> and use subtraction (222 \u2212 4 = 218 and 86 \u2212 2 = 84) to identify the daughter isotope as polonium:<\/p>\r\n<span class=\"informalequation\"><sub>86<\/sub><sup>222<\/sup>Rn\u00a0<\/span>\u2192\u00a0<sub>2<\/sub><sup>4<\/sup>He +\u00a0<sub>84<\/sub><sup>218<\/sup>Po\r\n<p class=\"simpara\"><em class=\"emphasis bolditalic\">Test Yourself<\/em><\/p>\r\n<p id=\"ball-ch15_s01_p11\" class=\"para\">Write the nuclear equation that represents radioactive decay of polonium-208 by alpha particle emission and identify the daughter isotope.<\/p>\r\n<p class=\"simpara\"><em class=\"emphasis\">Answer<\/em><\/p>\r\n<p id=\"ball-ch15_s01_p12\" class=\"para\"><span class=\"inlineequation\"><sub>84<\/sub><sup>208<\/sup>Po \u2192\u00a0<sub>2<\/sub><sup>4<\/sup>He + <sub>82<\/sub><sup>204<\/sup>Pb;<\/span> daughter isotope:\u00a0<sub>82<\/sub><sup>204<\/sup>Pb<\/p>\r\n\r\n<\/div>\r\n<p id=\"ball-ch15_s01_p13\" class=\"para block\">The second major type of radioactive emission is called a <span class=\"margin_term\"><a class=\"glossterm\">beta particle<\/a><\/span>, symbolized by the Greek letter \u03b2. A beta particle is an electron ejected from the nucleus (not from the shells of electrons about the nucleus) and has a 1\u2212 charge. We can also represent a beta particle as <sub>-1<\/sub><sup>0<\/sup><span class=\"inlineequation\">e.<\/span> The net effect of beta particle emission on a nucleus is that a neutron is converted to a proton. The overall mass number stays the same, but because the number of protons increases by one, the atomic number goes up by one. Carbon-14 decays by emitting a beta particle:<\/p>\r\n<span class=\"informalequation block\"><sub>6<\/sub><sup>14<\/sup>C \u2192 <sub>7<\/sub><sup>14<\/sup>N +<sub>-1<\/sub><sup>0<\/sup><span class=\"inlineequation\">e<\/span><\/span>\r\n<p id=\"ball-ch15_s01_p14\" class=\"para editable block\">Again, the sum of the atomic numbers is the same on both sides of the equation, as is the sum of the mass numbers. (Note that the electron is assigned an \u201catomic number\u201d of \u20131, equal to its charge.)<\/p>\r\n<p id=\"ball-ch15_s01_p15\" class=\"para editable block\">The third major type of radioactive emission is not a particle but rather a very energetic form of electromagnetic radiation called <span class=\"margin_term\"><a class=\"glossterm\">gamma rays<\/a><\/span>, symbolized by the Greek letter \u03b3. Gamma rays themselves do not carry an overall electrical charge, but they may knock electrons out of atoms in a sample of matter and make it electrically charged (for which gamma rays are termed <em class=\"emphasis\">ionizing radiation<\/em>). For example, in the radioactive decay of radon-222, both alpha and gamma radiation are emitted, with the latter having an energy of 8.2 \u00d7 10<sup class=\"superscript\">\u221214<\/sup> J per nucleus decayed:<\/p>\r\n<span class=\"informalequation block\"><span class=\"informalequation\"><sub>86<\/sub><sup>222<\/sup>Rn\u00a0<\/span>\u2192\u00a0<sub>2<\/sub><sup>4<\/sup>He +\u00a0<sub>84<\/sub><sup>218<\/sup>Po + \u03b3<\/span>\r\n<p id=\"ball-ch15_s01_p16\" class=\"para editable block\">This may not seem like much energy, but if 1 mol of Rn atoms were to decay, the gamma ray energy would be 4.9 \u00d7 10<sup class=\"superscript\">7<\/sup> kJ!<\/p>\r\n\r\n<div class=\"textbox shaded\">\r\n<h3 class=\"title\">Example 2<\/h3>\r\n<p id=\"ball-ch15_s01_p17\" class=\"para\">Write the nuclear equation that represents the radioactive decay of boron-12 by beta particle emission and identify the daughter isotope. A gamma ray is emitted simultaneously with the beta particle.<\/p>\r\n<p class=\"simpara\">Solution<\/p>\r\n<p id=\"ball-ch15_s01_p18\" class=\"para\">The parent isotope is <sub>5<\/sub><sup>12<\/sup><span class=\"inlineequation\">B,<\/span> while one of the products is <sub>-1<\/sub><sup>0<\/sup><span class=\"inlineequation\">e<\/span><span class=\"inlineequation\">.<\/span> So that the mass and atomic numbers have the same value on both sides, the mass number of the daughter isotope must be 12, and its atomic number must be 6. The element having an atomic number of 6 is carbon. Thus the complete nuclear equation is as follows:<\/p>\r\n<span class=\"informalequation\"><sub>5<\/sub><sup>12<\/sup><span class=\"inlineequation\">B\u00a0<\/span>\u2192\u00a0<sub>6<\/sub><sup>12<\/sup>C\u00a0+\u00a0<sub>-1<\/sub><sup>0<\/sup><span class=\"inlineequation\">e\u00a0<\/span>+ \u03b3<\/span>\r\n<p id=\"ball-ch15_s01_p19\" class=\"para\">The daughter isotope is carbon-12.<\/p>\r\n<p class=\"simpara\"><em class=\"emphasis bolditalic\">Test Yourself<\/em><\/p>\r\n<p id=\"ball-ch15_s01_p20\" class=\"para\">Write the nuclear equation that represents the radioactive decay of technetium-133 by beta particle emission and identify the daughter isotope. A gamma ray is emitted simultaneously with the beta particle.<\/p>\r\n<p class=\"simpara\"><em class=\"emphasis\">Answer<\/em><\/p>\r\n<p id=\"ball-ch15_s01_p21\" class=\"para\"><span class=\"inlineequation\"><span class=\"informalequation\"><sub>43<\/sub><sup>133<\/sup>Tc\u00a0<\/span>\u2192\u00a0<sub>44<\/sub><sup>133<\/sup>Ru + <sub>-1<\/sub><sup>0<\/sup><span class=\"inlineequation\">e +<\/span>\u00a0\u03b3;<\/span> daughter isotope: ruthenium-133<\/p>\r\n\r\n<\/div>\r\n<p id=\"ball-ch15_s01_p22\" class=\"para editable block\">Alpha, beta, and gamma emissions have different abilities to penetrate matter. The relatively large alpha particle is easily stopped by matter (although it may impart a significant amount of energy to the matter it contacts). Beta particles penetrate slightly into matter, perhaps a few centimeters at most. Gamma rays can penetrate deeply into matter and can impart a large amount of energy into the surrounding matter. <a class=\"xref\" href=\"#ball-ch15_s01_t01\">Table 15.1 \"The Three Main Forms of Radioactive Emissions\"<\/a> summarizes the properties of the three main types of radioactive emissions.<\/p>\r\n\r\n<div id=\"ball-ch15_s01_t01\" class=\"table block\">\r\n<p class=\"title\"><span class=\"title-prefix\">Table 15.1<\/span> The Three Main Forms of Radioactive Emissions<\/p>\r\n\r\n<table style=\"border-spacing: 0px\" cellpadding=\"0\">\r\n<thead>\r\n<tr>\r\n<th>Characteristic<\/th>\r\n<th>Alpha Particles<\/th>\r\n<th>Beta Particles<\/th>\r\n<th>Gamma Rays<\/th>\r\n<\/tr>\r\n<\/thead>\r\n<tbody>\r\n<tr>\r\n<td>symbols<\/td>\r\n<td>\u03b1,\u00a0<sub>2<\/sub><sup>4<\/sup>He<\/td>\r\n<td>\u03b2,\u00a0\u00a0<sub>-1<\/sub><sup>0<\/sup><span class=\"inlineequation\">e<\/span><\/td>\r\n<td>\u03b3<\/td>\r\n<\/tr>\r\n<tr>\r\n<td>identity<\/td>\r\n<td>helium nucleus<\/td>\r\n<td>electron<\/td>\r\n<td>electromagnetic radiation<\/td>\r\n<\/tr>\r\n<tr>\r\n<td>charge<\/td>\r\n<td>2+<\/td>\r\n<td>1\u2212<\/td>\r\n<td>none<\/td>\r\n<\/tr>\r\n<tr>\r\n<td>mass number<\/td>\r\n<td>4<\/td>\r\n<td>0<\/td>\r\n<td>0<\/td>\r\n<\/tr>\r\n<tr>\r\n<td>penetrating power<\/td>\r\n<td>minimal (will not penetrate skin)<\/td>\r\n<td>short (will penetrate skin and some tissues slightly)<\/td>\r\n<td>deep (will penetrate tissues deeply)<\/td>\r\n<\/tr>\r\n<\/tbody>\r\n<\/table>\r\n<\/div>\r\n<p id=\"ball-ch15_s01_p23\" class=\"para editable block\">Occasionally, an atomic nucleus breaks apart into smaller pieces in a radioactive process called <span class=\"margin_term\"><a class=\"glossterm\">spontaneous fission (or fission)<\/a><\/span>. Typically, the daughter isotopes produced by fission are a varied mix of products, rather than a specific isotope as with alpha and beta particle emission. Often, fission produces excess neutrons that will sometimes be captured by other nuclei, possibly inducing additional radioactive events. Uranium-235 undergoes spontaneous fission to a small extent. One typical reaction is<\/p>\r\n<span class=\"informalequation block\"><span class=\"informalequation\"><sub>92<\/sub><sup>235<\/sup>U\u00a0<\/span>\u2192\u00a0<sub>56<\/sub><sup>139<\/sup>Ba \u00a0+ <sub>36<\/sub><sup>94<\/sup>Kr + 2\u00a0<sub>0<\/sub><sup>1<\/sup>n<\/span>\r\n<p id=\"ball-ch15_s01_p24\" class=\"para block\">where <sub>0<\/sub><sup>1<\/sup>n\u00a0is a neutron. As with any nuclear process, the sums of the atomic numbers and mass numbers must be the same on both sides of the equation. Spontaneous fission is found only in large nuclei. The smallest nucleus that exhibits spontaneous fission is lead-208. (Fission is the radioactive process used in nuclear power plants and one type of nuclear bomb.)<\/p>\r\n\r\n<div id=\"ball-ch15_s01_n04\" class=\"key_takeaways editable block\">\r\n<div class=\"bcc-box bcc-success\">\r\n<h3>Key Takeaways<\/h3>\r\n<ul id=\"ball-ch15_s01_l02\" class=\"itemizedlist\">\r\n \t<li>The major types of radioactivity include alpha particles, beta particles, and gamma rays.<\/li>\r\n \t<li>Fission is a type of radioactivity in which large nuclei spontaneously break apart into smaller nuclei.<\/li>\r\n<\/ul>\r\n<\/div>\r\n<div class=\"bcc-box bcc-info\">\r\n<h3>Exercises<\/h3>\r\n<div id=\"ball-ch15_s01_qs01\" class=\"qandaset block\">\r\n<ol id=\"ball-ch15_s01_qs01_qd01\" class=\"qandadiv\">\r\n \t<li id=\"ball-ch15_s01_qs01_qd01_qa01\" class=\"qandaentry\">\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p01\" class=\"para\">Define <em class=\"emphasis\">radioactivity<\/em>.<\/p>\r\n\r\n<\/div><\/li>\r\n \t<li id=\"ball-ch15_s01_qs01_qd01_qa02\" class=\"qandaentry\">\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p03\" class=\"para\">Give an example of a radioactive element. How do you know if it is radioactive?<\/p>\r\n\r\n<\/div><\/li>\r\n \t<li id=\"ball-ch15_s01_qs01_qd01_qa03\" class=\"qandaentry\">\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p05\" class=\"para\">How many protons and neutrons are in each isotope?<\/p>\r\n\r\n<\/div><\/li>\r\n<\/ol>\r\n<span class=\"inlineequation\">a)<sub> \u00a05<\/sub><sup>11<\/sup>B<\/span>\r\n\r\n<span class=\"inlineequation\">b)<sub> \u00a013<\/sub><sup>27<\/sup>Al<\/span>\r\n\r\n<sup class=\"superscript\">c)<\/sup><sup class=\"superscript\"> \u00a056<\/sup>Fe\r\n\r\n<sup class=\"superscript\">d)<\/sup><sup class=\"superscript\">\u00a0224<\/sup>Rn\r\n\r\n&nbsp;\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p06\" class=\"para\">4. \u00a0How many protons and neutrons are in each isotope?<\/p>\r\n<span class=\"inlineequation\"><sub style=\"color: #000000\">a)<\/sub><sub style=\"color: #000000\"> 1<\/sub><sup style=\"color: #000000\">2<\/sup><span style=\"color: #000000\">H<\/span><\/span>\r\n\r\n<span class=\"inlineequation\">b)<sub> \u00a048<\/sub><sup>112<\/sup>Cd<\/span>\r\n\r\n<sup class=\"superscript\">c) \u00a0252<\/sup>Es\r\n\r\n<sup class=\"superscript\">d)<\/sup><sup class=\"superscript\"> \u00a040<\/sup>K\r\n\r\n<\/div>\r\n&nbsp;\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p07\" class=\"para\">5. \u00a0Describe an alpha particle. What nucleus is it equivalent to?<\/p>\r\n\r\n<\/div>\r\n&nbsp;\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p09\" class=\"para\">6. \u00a0Describe a beta particle. What subatomic particle is it equivalent to?<\/p>\r\n\r\n<\/div>\r\n&nbsp;\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p11\" class=\"para\">7. \u00a0What are gamma rays?<\/p>\r\n\r\n<\/div>\r\n&nbsp;\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p13\" class=\"para\">8. \u00a0Why is it inappropriate to refer to gamma rays as \u201cgamma particles\u201d?<\/p>\r\n\r\n<\/div>\r\n&nbsp;\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p15\" class=\"para\">9. \u00a0Plutonium has an atomic number of 94. Write the nuclear equation for the alpha particle emission of plutonium-244. What is the daughter isotope?<\/p>\r\n\r\n<\/div>\r\n&nbsp;\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p17\" class=\"para\">10. \u00a0Francium has an atomic number of 87. Write the nuclear equation for the alpha particle emission of francium-212. What is the daughter isotope?<\/p>\r\n\r\n<\/div>\r\n&nbsp;\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p19\" class=\"para\">11. \u00a0Tin has an atomic number of 50. Write the nuclear equation for the beta particle emission of tin-121. What is the daughter isotope?<\/p>\r\n\r\n<\/div>\r\n&nbsp;\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p21\" class=\"para\">12. \u00a0Technetium has an atomic number of 43. Write the nuclear equation for the beta particle emission of technetium-99. What is the daughter isotope?<\/p>\r\n\r\n<\/div>\r\n&nbsp;\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p23\" class=\"para\">13. \u00a0Energies of gamma rays are typically expressed in units of megaelectron volts (MeV), where 1 MeV = 1.602\u00a0\u00d7\u00a010<sup class=\"superscript\">\u221213<\/sup> J. Using the data provided in the text, calculate the energy in megaelectron volts of the gamma ray emitted when radon-222 decays.<\/p>\r\n\r\n<\/div>\r\n&nbsp;\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p25\" class=\"para\">14. \u00a0The gamma ray emitted when oxygen-19 gives off a beta particle is 0.197 MeV. What is its energy in joules? (See Exercise 13 for the definition of a megaelectron volt.)<\/p>\r\n\r\n<\/div>\r\n&nbsp;\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p27\" class=\"para\">15. \u00a0Which penetrates matter more deeply\u2014alpha particles or beta particles? Suggest ways to protect yourself against both particles.<\/p>\r\n\r\n<\/div>\r\n&nbsp;\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p29\" class=\"para\">16. \u00a0Which penetrates matter more deeply\u2014alpha particles or gamma rays? Suggest ways to protect yourself against both emissions.<\/p>\r\n\r\n<\/div>\r\n&nbsp;\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p31\" class=\"para\">17. \u00a0Define <em class=\"emphasis\">nuclear fission<\/em>.<\/p>\r\n\r\n<\/div>\r\n&nbsp;\r\n<div class=\"question\">\r\n<p id=\"ball-ch15_s01_qs01_p33\" class=\"para\">18. \u00a0What general characteristic is typically necessary for a nucleus to undergo spontaneous fission?<\/p>\r\n\r\n<\/div>\r\n<\/div>\r\n<b>Answers<\/b>\r\n\r\n<strong>1.<\/strong>\r\n\r\nRadioactivity is the spontaneous emission of particles and electromagnetic radiation from nuclei of unstable atoms.\r\n\r\n<strong>3.<\/strong>\r\n\r\na) \u00a05 protons; 6 neutrons\r\n\r\nb) \u00a013 protons; 14 neutrons\r\n\r\nc) \u00a026 protons; 30 neutrons\r\n\r\nd) \u00a086 protons; 138 neutrons\r\n\r\n<strong>5.<\/strong>\r\n\r\nAn alpha particle is a collection of two protons and two neutrons and is equivalent to a helium nucleus.\r\n\r\n<strong>7.<\/strong>\r\n\r\nGamma rays are high-energy electromagnetic radiation given off in radioactive decay.\r\n\r\n<strong>9.<\/strong>\r\n\r\n<span class=\"inlineequation\"><sub>94<\/sub><sup>244<\/sup>Pu\u2192<sub>92<\/sub><sup>240<\/sup>U +<sub>2<\/sub><sup>4<\/sup>He;<\/span> daughter isotope: <sup class=\"superscript\">240<\/sup>U\r\n\r\n<strong>11.<\/strong>\r\n\r\n<span class=\"inlineequation\"><sub>50<\/sub><sup>121<\/sup>Sn\u2192<sub>51<\/sub><sup>121<\/sup>Sb\u00a0+ \u00a0<sub>-1<\/sub><sup>0<\/sup><span class=\"inlineequation\">e<\/span>;<\/span> daughter isotope: <sup class=\"superscript\">121<\/sup>Sb\r\n\r\n<strong>13.<\/strong>\r\n\r\n0.51 MeV\r\n\r\n<strong>15.<\/strong>\r\n\r\nBeta particles penetrate more. A thick wall of inert matter is sufficient to block both particles.\r\n\r\n<strong>17.<\/strong>\r\n\r\nNuclear fission is the breaking down of large nuclei into smaller nuclei, usually with the release of excess neutrons.\r\n\r\n<\/div>\r\n<\/div>\r\n<\/div>","rendered":"<div id=\"ball-ch15_s01\" class=\"section\" lang=\"en\">\n<div id=\"ball-ch15_s01_n01\" class=\"learning_objectives editable block\">\n<div class=\"bcc-box bcc-highlight\">\n<h3>Learning Objectives<\/h3>\n<p>1. Define and give examples of the major types of radioactivity.<\/p>\n<\/div>\n<\/div>\n<p id=\"ball-ch15_s01_p01\" class=\"para editable block\">We saw in <a class=\"xref\" href=\"ball-ch03#ball-ch03\">Chapter 3 &#8220;Atoms, Molecules, and Ions&#8221;<\/a> that atoms are composed of subatomic particles\u2014protons, neutrons, and electrons. Protons and neutrons are located in the nucleus and provide most of the mass of an atom, while electrons circle the nucleus in shells and subshells and account for an atom\u2019s size.<\/p>\n<p id=\"ball-ch15_s01_p02\" class=\"para editable block\">We also introduced in <a class=\"xref\" href=\"ball-ch03#ball-ch03\">Chapter 3 &#8220;Atoms, Molecules, and Ions&#8221;<\/a> the notation for succinctly representing an isotope of a particular atom:<\/p>\n<p><span class=\"informalequation block\"><sub>6<\/sub><sup>12<\/sup>C<\/span><\/p>\n<p id=\"ball-ch15_s01_p03\" class=\"para editable block\">The element in this example, represented by the symbol C, is carbon. Its atomic number, 6, is the subscript next to the symbol and is the number of protons in the atom. The mass number, the superscript next to the symbol, is the sum of the number of protons and neutrons in the nucleus of this particular isotope. In this case, the mass number is 12, which means that the number of neutrons in the atom is 12 \u2212 6 = 6 (that is, the mass number of the atom minus the number of protons in the nucleus equals the number of neurons). Occasionally, the atomic number is omitted in this notation because the symbol of the element itself conveys its characteristic atomic number. The two isotopes of hydrogen\u2014<sup class=\"superscript\">2<\/sup>H and <sup class=\"superscript\">3<\/sup>H\u2014are given their own names and symbols: deuterium (D) and tritium (T), respectively.<\/p>\n<p id=\"ball-ch15_s01_p04\" class=\"para editable block\">Atomic theory in the nineteenth century presumed that nuclei had fixed compositions. But in 1896, the French scientist Henri Becquerel found that a uranium compound placed near a photographic plate made an image on the plate, even if the compound was wrapped in black cloth. He reasoned that the uranium compound was emitting some kind of radiation that passed through the cloth to expose the photographic plate. Further investigations showed that the radiation was a combination of particles and electromagnetic rays, with its ultimate source being the atomic nucleus. These emanations were ultimately called, collectively, <span class=\"margin_term\"><a class=\"glossterm\">radioactivity<\/a><\/span>.<\/p>\n<p id=\"ball-ch15_s01_p05\" class=\"para block\">There are three main forms of radioactive emissions. The first is called an <span class=\"margin_term\"><a class=\"glossterm\">alpha particle<\/a><\/span>, which is symbolized by the Greek letter \u03b1. An alpha particle is composed of two protons and two neutrons and is the same as a helium nucleus. (We often use <sub>2<\/sub><sup>4<\/sup>He\u00a0to represent an alpha particle.) It has a 2+\u00a0charge. When a radioactive atom emits an alpha particle, the original atom\u2019s atomic number decreases by two (because of the loss of two protons), and its mass number decreases by four (because of the loss of four nuclear particles). We can represent the emission of an alpha particle with a chemical equation\u2014for example, the alpha-particle emission of uranium-235 is as follows:<\/p>\n<p><span class=\"informalequation block\"><sub>92<\/sub><sup>235<\/sup>U \u2192\u00a0<sub>2<\/sub><sup>4<\/sup>He+<sub>90<\/sub><sup>231<\/sup>Th<\/span><\/p>\n<p id=\"ball-ch15_s01_p06\" class=\"para block\">Rather than calling this equation a chemical equation, we call it a <span class=\"margin_term\"><a class=\"glossterm\">nuclear equation<\/a><\/span>\u00a0to emphasize that the change occurs in an atomic nucleus. How do we know that a product of this reaction is<sub>90<\/sub><sup>231<\/sup>Th? We use the law of conservation of matter, which says that matter cannot be created or destroyed. This means we must have the same number of protons and neutrons on both sides of the nuclear equation. If our uranium nucleus loses 2 protons, there are 90 protons remaining, identifying the element as thorium. Moreover, if we lose four nuclear particles of the original 235, there are 231 remaining. Thus we use subtraction to identify the isotope of the Th atom\u2014in this case, <sub>90<\/sub><sup>231<\/sup>Th<span class=\"inlineequation\">.<\/span><\/p>\n<p id=\"ball-ch15_s01_p07\" class=\"para block\">Chemists often use the names <span class=\"margin_term\"><a class=\"glossterm\">parent isotope<\/a><\/span>\u00a0and <span class=\"margin_term\"><a class=\"glossterm\">daughter isotope<\/a><\/span>\u00a0to represent the original atom and the product other than the alpha particle. In the previous example,\u00a0<sub>92<\/sub><sup>235<\/sup>U<\/p>\n<p id=\"ball-ch15_s01_p08\" class=\"para block\">is the parent isotope, and\u00a0<sub>90<\/sub><sup>231<\/sup>Th\u00a0is the daughter isotope. When one element changes into another in this manner, it undergoes <span class=\"margin_term\"><a class=\"glossterm\">radioactive decay<\/a><\/span>.<\/p>\n<div class=\"textbox shaded\">\n<h3 class=\"title\">Example 1<\/h3>\n<p id=\"ball-ch15_s01_p09\" class=\"para\">Write the nuclear equation that represents the radioactive decay of radon-222 by alpha particle emission and identify the daughter isotope.<\/p>\n<p class=\"simpara\">Solution<\/p>\n<p id=\"ball-ch15_s01_p10\" class=\"para\">Radon has an atomic number of 86, so the parent isotope is represented as Th<span class=\"inlineequation\"> <sub>86<\/sub><sup>222<\/sup>Rn.<\/span> We represent the alpha particle as <span class=\"inlineequation\"><sub>2<\/sub><sup>4<\/sup>He<\/span> and use subtraction (222 \u2212 4 = 218 and 86 \u2212 2 = 84) to identify the daughter isotope as polonium:<\/p>\n<p><span class=\"informalequation\"><sub>86<\/sub><sup>222<\/sup>Rn\u00a0<\/span>\u2192\u00a0<sub>2<\/sub><sup>4<\/sup>He +\u00a0<sub>84<\/sub><sup>218<\/sup>Po<\/p>\n<p class=\"simpara\"><em class=\"emphasis bolditalic\">Test Yourself<\/em><\/p>\n<p id=\"ball-ch15_s01_p11\" class=\"para\">Write the nuclear equation that represents radioactive decay of polonium-208 by alpha particle emission and identify the daughter isotope.<\/p>\n<p class=\"simpara\"><em class=\"emphasis\">Answer<\/em><\/p>\n<p id=\"ball-ch15_s01_p12\" class=\"para\"><span class=\"inlineequation\"><sub>84<\/sub><sup>208<\/sup>Po \u2192\u00a0<sub>2<\/sub><sup>4<\/sup>He + <sub>82<\/sub><sup>204<\/sup>Pb;<\/span> daughter isotope:\u00a0<sub>82<\/sub><sup>204<\/sup>Pb<\/p>\n<\/div>\n<p id=\"ball-ch15_s01_p13\" class=\"para block\">The second major type of radioactive emission is called a <span class=\"margin_term\"><a class=\"glossterm\">beta particle<\/a><\/span>, symbolized by the Greek letter \u03b2. A beta particle is an electron ejected from the nucleus (not from the shells of electrons about the nucleus) and has a 1\u2212 charge. We can also represent a beta particle as <sub>-1<\/sub><sup>0<\/sup><span class=\"inlineequation\">e.<\/span> The net effect of beta particle emission on a nucleus is that a neutron is converted to a proton. The overall mass number stays the same, but because the number of protons increases by one, the atomic number goes up by one. Carbon-14 decays by emitting a beta particle:<\/p>\n<p><span class=\"informalequation block\"><sub>6<\/sub><sup>14<\/sup>C \u2192 <sub>7<\/sub><sup>14<\/sup>N +<sub>-1<\/sub><sup>0<\/sup><span class=\"inlineequation\">e<\/span><\/span><\/p>\n<p id=\"ball-ch15_s01_p14\" class=\"para editable block\">Again, the sum of the atomic numbers is the same on both sides of the equation, as is the sum of the mass numbers. (Note that the electron is assigned an \u201catomic number\u201d of \u20131, equal to its charge.)<\/p>\n<p id=\"ball-ch15_s01_p15\" class=\"para editable block\">The third major type of radioactive emission is not a particle but rather a very energetic form of electromagnetic radiation called <span class=\"margin_term\"><a class=\"glossterm\">gamma rays<\/a><\/span>, symbolized by the Greek letter \u03b3. Gamma rays themselves do not carry an overall electrical charge, but they may knock electrons out of atoms in a sample of matter and make it electrically charged (for which gamma rays are termed <em class=\"emphasis\">ionizing radiation<\/em>). For example, in the radioactive decay of radon-222, both alpha and gamma radiation are emitted, with the latter having an energy of 8.2 \u00d7 10<sup class=\"superscript\">\u221214<\/sup> J per nucleus decayed:<\/p>\n<p><span class=\"informalequation block\"><span class=\"informalequation\"><sub>86<\/sub><sup>222<\/sup>Rn\u00a0<\/span>\u2192\u00a0<sub>2<\/sub><sup>4<\/sup>He +\u00a0<sub>84<\/sub><sup>218<\/sup>Po + \u03b3<\/span><\/p>\n<p id=\"ball-ch15_s01_p16\" class=\"para editable block\">This may not seem like much energy, but if 1 mol of Rn atoms were to decay, the gamma ray energy would be 4.9 \u00d7 10<sup class=\"superscript\">7<\/sup> kJ!<\/p>\n<div class=\"textbox shaded\">\n<h3 class=\"title\">Example 2<\/h3>\n<p id=\"ball-ch15_s01_p17\" class=\"para\">Write the nuclear equation that represents the radioactive decay of boron-12 by beta particle emission and identify the daughter isotope. A gamma ray is emitted simultaneously with the beta particle.<\/p>\n<p class=\"simpara\">Solution<\/p>\n<p id=\"ball-ch15_s01_p18\" class=\"para\">The parent isotope is <sub>5<\/sub><sup>12<\/sup><span class=\"inlineequation\">B,<\/span> while one of the products is <sub>-1<\/sub><sup>0<\/sup><span class=\"inlineequation\">e<\/span><span class=\"inlineequation\">.<\/span> So that the mass and atomic numbers have the same value on both sides, the mass number of the daughter isotope must be 12, and its atomic number must be 6. The element having an atomic number of 6 is carbon. Thus the complete nuclear equation is as follows:<\/p>\n<p><span class=\"informalequation\"><sub>5<\/sub><sup>12<\/sup><span class=\"inlineequation\">B\u00a0<\/span>\u2192\u00a0<sub>6<\/sub><sup>12<\/sup>C\u00a0+\u00a0<sub>-1<\/sub><sup>0<\/sup><span class=\"inlineequation\">e\u00a0<\/span>+ \u03b3<\/span><\/p>\n<p id=\"ball-ch15_s01_p19\" class=\"para\">The daughter isotope is carbon-12.<\/p>\n<p class=\"simpara\"><em class=\"emphasis bolditalic\">Test Yourself<\/em><\/p>\n<p id=\"ball-ch15_s01_p20\" class=\"para\">Write the nuclear equation that represents the radioactive decay of technetium-133 by beta particle emission and identify the daughter isotope. A gamma ray is emitted simultaneously with the beta particle.<\/p>\n<p class=\"simpara\"><em class=\"emphasis\">Answer<\/em><\/p>\n<p id=\"ball-ch15_s01_p21\" class=\"para\"><span class=\"inlineequation\"><span class=\"informalequation\"><sub>43<\/sub><sup>133<\/sup>Tc\u00a0<\/span>\u2192\u00a0<sub>44<\/sub><sup>133<\/sup>Ru + <sub>-1<\/sub><sup>0<\/sup><span class=\"inlineequation\">e +<\/span>\u00a0\u03b3;<\/span> daughter isotope: ruthenium-133<\/p>\n<\/div>\n<p id=\"ball-ch15_s01_p22\" class=\"para editable block\">Alpha, beta, and gamma emissions have different abilities to penetrate matter. The relatively large alpha particle is easily stopped by matter (although it may impart a significant amount of energy to the matter it contacts). Beta particles penetrate slightly into matter, perhaps a few centimeters at most. Gamma rays can penetrate deeply into matter and can impart a large amount of energy into the surrounding matter. <a class=\"xref\" href=\"#ball-ch15_s01_t01\">Table 15.1 &#8220;The Three Main Forms of Radioactive Emissions&#8221;<\/a> summarizes the properties of the three main types of radioactive emissions.<\/p>\n<div id=\"ball-ch15_s01_t01\" class=\"table block\">\n<p class=\"title\"><span class=\"title-prefix\">Table 15.1<\/span> The Three Main Forms of Radioactive Emissions<\/p>\n<table style=\"border-spacing: 0px\" cellpadding=\"0\">\n<thead>\n<tr>\n<th>Characteristic<\/th>\n<th>Alpha Particles<\/th>\n<th>Beta Particles<\/th>\n<th>Gamma Rays<\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr>\n<td>symbols<\/td>\n<td>\u03b1,\u00a0<sub>2<\/sub><sup>4<\/sup>He<\/td>\n<td>\u03b2,\u00a0\u00a0<sub>-1<\/sub><sup>0<\/sup><span class=\"inlineequation\">e<\/span><\/td>\n<td>\u03b3<\/td>\n<\/tr>\n<tr>\n<td>identity<\/td>\n<td>helium nucleus<\/td>\n<td>electron<\/td>\n<td>electromagnetic radiation<\/td>\n<\/tr>\n<tr>\n<td>charge<\/td>\n<td>2+<\/td>\n<td>1\u2212<\/td>\n<td>none<\/td>\n<\/tr>\n<tr>\n<td>mass number<\/td>\n<td>4<\/td>\n<td>0<\/td>\n<td>0<\/td>\n<\/tr>\n<tr>\n<td>penetrating power<\/td>\n<td>minimal (will not penetrate skin)<\/td>\n<td>short (will penetrate skin and some tissues slightly)<\/td>\n<td>deep (will penetrate tissues deeply)<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<\/div>\n<p id=\"ball-ch15_s01_p23\" class=\"para editable block\">Occasionally, an atomic nucleus breaks apart into smaller pieces in a radioactive process called <span class=\"margin_term\"><a class=\"glossterm\">spontaneous fission (or fission)<\/a><\/span>. Typically, the daughter isotopes produced by fission are a varied mix of products, rather than a specific isotope as with alpha and beta particle emission. Often, fission produces excess neutrons that will sometimes be captured by other nuclei, possibly inducing additional radioactive events. Uranium-235 undergoes spontaneous fission to a small extent. One typical reaction is<\/p>\n<p><span class=\"informalequation block\"><span class=\"informalequation\"><sub>92<\/sub><sup>235<\/sup>U\u00a0<\/span>\u2192\u00a0<sub>56<\/sub><sup>139<\/sup>Ba \u00a0+ <sub>36<\/sub><sup>94<\/sup>Kr + 2\u00a0<sub>0<\/sub><sup>1<\/sup>n<\/span><\/p>\n<p id=\"ball-ch15_s01_p24\" class=\"para block\">where <sub>0<\/sub><sup>1<\/sup>n\u00a0is a neutron. As with any nuclear process, the sums of the atomic numbers and mass numbers must be the same on both sides of the equation. Spontaneous fission is found only in large nuclei. The smallest nucleus that exhibits spontaneous fission is lead-208. (Fission is the radioactive process used in nuclear power plants and one type of nuclear bomb.)<\/p>\n<div id=\"ball-ch15_s01_n04\" class=\"key_takeaways editable block\">\n<div class=\"bcc-box bcc-success\">\n<h3>Key Takeaways<\/h3>\n<ul id=\"ball-ch15_s01_l02\" class=\"itemizedlist\">\n<li>The major types of radioactivity include alpha particles, beta particles, and gamma rays.<\/li>\n<li>Fission is a type of radioactivity in which large nuclei spontaneously break apart into smaller nuclei.<\/li>\n<\/ul>\n<\/div>\n<div class=\"bcc-box bcc-info\">\n<h3>Exercises<\/h3>\n<div id=\"ball-ch15_s01_qs01\" class=\"qandaset block\">\n<ol id=\"ball-ch15_s01_qs01_qd01\" class=\"qandadiv\">\n<li id=\"ball-ch15_s01_qs01_qd01_qa01\" class=\"qandaentry\">\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p01\" class=\"para\">Define <em class=\"emphasis\">radioactivity<\/em>.<\/p>\n<\/div>\n<\/li>\n<li id=\"ball-ch15_s01_qs01_qd01_qa02\" class=\"qandaentry\">\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p03\" class=\"para\">Give an example of a radioactive element. How do you know if it is radioactive?<\/p>\n<\/div>\n<\/li>\n<li id=\"ball-ch15_s01_qs01_qd01_qa03\" class=\"qandaentry\">\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p05\" class=\"para\">How many protons and neutrons are in each isotope?<\/p>\n<\/div>\n<\/li>\n<\/ol>\n<p><span class=\"inlineequation\">a)<sub> \u00a05<\/sub><sup>11<\/sup>B<\/span><\/p>\n<p><span class=\"inlineequation\">b)<sub> \u00a013<\/sub><sup>27<\/sup>Al<\/span><\/p>\n<p><sup class=\"superscript\">c)<\/sup><sup class=\"superscript\"> \u00a056<\/sup>Fe<\/p>\n<p><sup class=\"superscript\">d)<\/sup><sup class=\"superscript\">\u00a0224<\/sup>Rn<\/p>\n<p>&nbsp;<\/p>\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p06\" class=\"para\">4. \u00a0How many protons and neutrons are in each isotope?<\/p>\n<p><span class=\"inlineequation\"><sub style=\"color: #000000\">a)<\/sub><sub style=\"color: #000000\"> 1<\/sub><sup style=\"color: #000000\">2<\/sup><span style=\"color: #000000\">H<\/span><\/span><\/p>\n<p><span class=\"inlineequation\">b)<sub> \u00a048<\/sub><sup>112<\/sup>Cd<\/span><\/p>\n<p><sup class=\"superscript\">c) \u00a0252<\/sup>Es<\/p>\n<p><sup class=\"superscript\">d)<\/sup><sup class=\"superscript\"> \u00a040<\/sup>K<\/p>\n<\/div>\n<p>&nbsp;<\/p>\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p07\" class=\"para\">5. \u00a0Describe an alpha particle. What nucleus is it equivalent to?<\/p>\n<\/div>\n<p>&nbsp;<\/p>\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p09\" class=\"para\">6. \u00a0Describe a beta particle. What subatomic particle is it equivalent to?<\/p>\n<\/div>\n<p>&nbsp;<\/p>\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p11\" class=\"para\">7. \u00a0What are gamma rays?<\/p>\n<\/div>\n<p>&nbsp;<\/p>\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p13\" class=\"para\">8. \u00a0Why is it inappropriate to refer to gamma rays as \u201cgamma particles\u201d?<\/p>\n<\/div>\n<p>&nbsp;<\/p>\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p15\" class=\"para\">9. \u00a0Plutonium has an atomic number of 94. Write the nuclear equation for the alpha particle emission of plutonium-244. What is the daughter isotope?<\/p>\n<\/div>\n<p>&nbsp;<\/p>\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p17\" class=\"para\">10. \u00a0Francium has an atomic number of 87. Write the nuclear equation for the alpha particle emission of francium-212. What is the daughter isotope?<\/p>\n<\/div>\n<p>&nbsp;<\/p>\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p19\" class=\"para\">11. \u00a0Tin has an atomic number of 50. Write the nuclear equation for the beta particle emission of tin-121. What is the daughter isotope?<\/p>\n<\/div>\n<p>&nbsp;<\/p>\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p21\" class=\"para\">12. \u00a0Technetium has an atomic number of 43. Write the nuclear equation for the beta particle emission of technetium-99. What is the daughter isotope?<\/p>\n<\/div>\n<p>&nbsp;<\/p>\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p23\" class=\"para\">13. \u00a0Energies of gamma rays are typically expressed in units of megaelectron volts (MeV), where 1 MeV = 1.602\u00a0\u00d7\u00a010<sup class=\"superscript\">\u221213<\/sup> J. Using the data provided in the text, calculate the energy in megaelectron volts of the gamma ray emitted when radon-222 decays.<\/p>\n<\/div>\n<p>&nbsp;<\/p>\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p25\" class=\"para\">14. \u00a0The gamma ray emitted when oxygen-19 gives off a beta particle is 0.197 MeV. What is its energy in joules? (See Exercise 13 for the definition of a megaelectron volt.)<\/p>\n<\/div>\n<p>&nbsp;<\/p>\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p27\" class=\"para\">15. \u00a0Which penetrates matter more deeply\u2014alpha particles or beta particles? Suggest ways to protect yourself against both particles.<\/p>\n<\/div>\n<p>&nbsp;<\/p>\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p29\" class=\"para\">16. \u00a0Which penetrates matter more deeply\u2014alpha particles or gamma rays? Suggest ways to protect yourself against both emissions.<\/p>\n<\/div>\n<p>&nbsp;<\/p>\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p31\" class=\"para\">17. \u00a0Define <em class=\"emphasis\">nuclear fission<\/em>.<\/p>\n<\/div>\n<p>&nbsp;<\/p>\n<div class=\"question\">\n<p id=\"ball-ch15_s01_qs01_p33\" class=\"para\">18. \u00a0What general characteristic is typically necessary for a nucleus to undergo spontaneous fission?<\/p>\n<\/div>\n<\/div>\n<p><b>Answers<\/b><\/p>\n<p><strong>1.<\/strong><\/p>\n<p>Radioactivity is the spontaneous emission of particles and electromagnetic radiation from nuclei of unstable atoms.<\/p>\n<p><strong>3.<\/strong><\/p>\n<p>a) \u00a05 protons; 6 neutrons<\/p>\n<p>b) \u00a013 protons; 14 neutrons<\/p>\n<p>c) \u00a026 protons; 30 neutrons<\/p>\n<p>d) \u00a086 protons; 138 neutrons<\/p>\n<p><strong>5.<\/strong><\/p>\n<p>An alpha particle is a collection of two protons and two neutrons and is equivalent to a helium nucleus.<\/p>\n<p><strong>7.<\/strong><\/p>\n<p>Gamma rays are high-energy electromagnetic radiation given off in radioactive decay.<\/p>\n<p><strong>9.<\/strong><\/p>\n<p><span class=\"inlineequation\"><sub>94<\/sub><sup>244<\/sup>Pu\u2192<sub>92<\/sub><sup>240<\/sup>U +<sub>2<\/sub><sup>4<\/sup>He;<\/span> daughter isotope: <sup class=\"superscript\">240<\/sup>U<\/p>\n<p><strong>11.<\/strong><\/p>\n<p><span class=\"inlineequation\"><sub>50<\/sub><sup>121<\/sup>Sn\u2192<sub>51<\/sub><sup>121<\/sup>Sb\u00a0+ \u00a0<sub>-1<\/sub><sup>0<\/sup><span class=\"inlineequation\">e<\/span>;<\/span> daughter isotope: <sup class=\"superscript\">121<\/sup>Sb<\/p>\n<p><strong>13.<\/strong><\/p>\n<p>0.51 MeV<\/p>\n<p><strong>15.<\/strong><\/p>\n<p>Beta particles penetrate more. A thick wall of inert matter is sufficient to block both particles.<\/p>\n<p><strong>17.<\/strong><\/p>\n<p>Nuclear fission is the breaking down of large nuclei into smaller nuclei, usually with the release of excess neutrons.<\/p>\n<\/div>\n<\/div>\n<\/div>\n\n\t\t\t <section class=\"citations-section\" role=\"contentinfo\">\n\t\t\t <h3>Candela Citations<\/h3>\n\t\t\t\t\t <div>\n\t\t\t\t\t\t <div id=\"citation-list-3363\">\n\t\t\t\t\t\t\t <div class=\"licensing\"><div class=\"license-attribution-dropdown-subheading\">CC licensed content, Original<\/div><ul class=\"citation-list\"><li><strong>Authored by<\/strong>: Jessie A. 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