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Atomic Structure, the Periodic Table, and Nuclear Radiation The Electromagnetic Spectrum Basics of Periodic Table • Each box on the table represents an element. • In each box… – an element symbol – the element’s atomic number – the element’s average atomic mass • Elements arranged in order of increasing atomic number. Isotope symbol (neutral) Mass number (#p + #n) Atomic number (#P) 14 6 Isotope name carbon-14 C Isotope symbol (charged) 32 15 P 3− Average Atomic Mass • The masses found on the periodic table are called average atomic masses. • They represent the weighted average of all the isotopes found in a sample of the element – Isotopes are atoms of the same element with different numbers of neutrons Example The atomic masses of the two stable isotopes of boron, boron-10 (19.78%) and boron-11 (80.22 %), are 10.0129 amu and 11.0093 amu, respectively. Calculate the average atomic mass of boron. Remember… • Electron configuration…ie. Shorthand – Should be able to do shorthand w/o diagonal rule • Aufbau principle – electrons fill energy levels and sublevels in order of increasing energy • Pauli Exclusion principle – no two electrons can have the same set of four quantum numbers (which means no two electrons can be in the same place at the same time) • Hund’s rule – when adding electrons to sublevels with more than one orbital, each orbital gets its own electron first before pairing s orbitals p orbitals d orbitals f orbitals • Metalloids are on the stair step • Metals to the left of the stair step • Nonmetals to the right of the stair step (plus H) Quantum Numbers • Just as a point on an xy-graph needs a set of two coordinates, each electron has a unique set of four coordinates. • These four coordinates represent shell (energy level), subshell (sublevel), orbital, and spin direction of the electron. Principal Quantum number • Represented by n • Corresponds to the rows of the periodic table • Therefore n = 1, 2, 3, and so on • Tells the size of the electron cloud 2nd Quantum number • Represented by l • Called the angular momentum quantum number • Describes the shape of the orbital • l can have the values from 0 to n-1 0 = s sublevel 1 = p sublevel 2 = d sublevel 3 = f sublevel 3rd Quantum Number • Called the magnetic quantum number • Describes the orientation in space of the orbital – Whether the path of the electron lies on the x, y, or z axis • Represented by ml • ml can have values from –l to +l – if l = 2, then ml = -2, -1, 0, +1, +2 4th Quantum Number • • • • Corresponds to the spin of an electron Represented by ms Clockwise represented by +1/2 Counterclockwise represented by -1/2 Therefore • Mg (3, 0, 0, -1/2) • Bi (6, 1, +1, +1/2) • Co (3, 2, -1, -1/2) • Cf (5, 3, -1, -1/2) Diamagnetism/Paramagnetism • Diamagnetic elements have all of their electrons spin paired. – Which means they have complete sublevels. – Are not affected by a magnetic field • Paramagnetic elements do not have all of their electrons spin paired. – Strongly affected by a magnetic field Ground State vs Excited State • In a ground state atom, all electrons are in the lowest available sublevels. • For an atom in the excited state, one or more electrons have absorbed enough energy to jump to higher energy levels. – As soon as possible, those excited electrons will release that energy in the form of a photon, possibly as colored light. Shorthand for ions Ca2+ K+ ClS2P3- 1s22s22p63s23p6 1s22s22p63s23p6 1s22s22p63s23p6 1s22s22p63s23p6 1s22s22p63s23p6 All of these ions have the same configuration as argon and are isoelectronic. Periodic Trends • You can make predictions about certain behavior patters of an atom and its electrons based on the position of the atom in the periodic table. • All the periodic trends can be understood in terms of three basic rules. 1. Electrons are attracted to the protons in the nucleus of an atom. – The closer an electron is to the nucleus, the more strongly it is attracted. – The more protons in a nucleus, the more strongly an electron is attracted. 2. Electrons are repelled by other electrons in an atom. So, if other electrons are between a valence electron and the nucleus, the valence electron will be less attracted to the nucleus. That’s called shielding. 3. Completed energy levels (and to a lesser extent, completed sublevels) are very stable. Atoms prefer to add or subtract valence electrons to create complete shells if possible. Atomic Radius • Atomic radius is the approximate distance from the nucleus of an atom to its valence electrons – Atomic radius decreases left to right – Atomic radius increases top to bottom • Cations are metals that lose electrons. – The cation is smaller than the original atom. • Anions are nonmetals that gain electrons – The anion is larger than the original atom. Ionization Energy • The energy required to remove an electron from an atom is called ionization energy. – The energy required to remove the next electron is called the second ionization energy • IE increases as you go left to right – There will be some peaks and valleys • IE decreases as you go down a group • For each element, when the valence shell is empty, the next electron must come from a shell that is full….much more energy required. – For example….aluminum. Al has 3 valence electrons. After those first 3 electrons have been removed, it takes a lot more energy to remove the 4th electron which comes from the core. Electron Affinity • Electron affinity is a measure of the change in energy of an atom when an electron is added to it. – If the addition of an electron makes the atom more stable, energy is given off. – When the addition of an electron makes the atom less stable, energy must be added. • This happens to the alkaline earth metals and the noble gases Electronegativity • Electronegativity refers to how strongly the nucleus of an atom attracts the electrons of other atoms in a bond (stinginess). • Moving from left to right across a period, electronegativity decreases (noble gases, generally, do not have electronegativities) • Moving down a group, electronegativity decreases. Notice that the noble gases are missing….just know that Kr and Xe have an electronegativity and they can bond with fluorine to make stable compounds. Shielding Effect • Shielding effect is the result of full energy levels separating the outer electrons from the nucleus. – Going down a group, the shielding effect increases due to the increased number of energy levels “shielding” the outer electrons from the nucleus. – Going across a row, the shielding effect remains the same. Summary of Periodic Trends Remains the same Shielding Effect Increases Ionization Energy, Electronegativity, Electron affinity Decreases Atomic size, Ion size Decreases Increases Ionization Energy Electron affinity Electronegativity Nuclear Charge Atomic size Shielding Effect Ion size Nuclear Decay • A nucleus is held together by a nonelectrical, nongravitational force called the nuclear force. • Some nuclei are more stable than others. • When a nucleus is unstable, it can attempt to increase its stability by altering its number of neutrons and/or protons. • This is the process of radioactive decay. Alpha Emission • In alpha decay, the nucleus emits a particle that looks just like a helium nucleus. – 2 protons and 2 neutrons • Alpha particles are not very penetrating – They can be stopped by paper, skin • Usually emitted by large nuclei 4 2 4 2 He= α • When a nucleus undergoes alpha decay – Subtract 4 from the mass number – Subtract 2 from the atomic number • Example of alpha decay 238 92 4 2 234 90 U → He+ Th Beta Emission • A beta particle is identical to an electron • A nucleus that has too many neutrons, changes a neutron into a proton and an electron and emits the electron. 1 0 0 −1 1 1 n→ e + p • Symbol for beta particle can be either 0 −1 e or 0 −1 β • Need a sheet of metal or plastic to shield it • When a nucleus undergoes beta decay – The mass number remains the same – The atomic number goes up by 1 • Example of beta decay 14 6 0 −1 14 7 C → e+ N Positron Emission • A positron is like an electron with a positive charge. • In positron emission, the nucleus changes a proton into a neutron and a positron and emits the positron. 1 1 0 +1 1 0 p → e+ n • Symbol for positron can be either 0 +1 e or 0 +1 β • A nucleus does not have enough neutrons • When a nucleus undergoes positron emission – The mass number remains the same – The atomic number drops by 1 • Example of positron emission 8 5 0 +1 8 4 B→ e+ Be Electron capture • In electron capture, the nucleus does not have enough neutrons • Its nucleus captures a low energy electron and combines it with a proton to form a neutron. 0 −1 1 1 1 0 e+ p→ n • When a nucleus undergoes electron capture – The mass number remains the same – The atomic number drops by one • Example of electron capture 16 9 0 −1 16 8 F + e→ O Gamma Rays • Gamma rays are electromagnetic radiation that have no mass and no charge. • Gamma rays usually accompany other forms of nuclear decay and are the most penetrating of all. – Need 2-3 inches of lead or 6-9 feet of concrete to be shielded from gamma rays • Think of those needing to give off a gamma ray as having too much pent up energy. – Once they emit the gamma ray, they feel much better. • Example of gamma emission (m means metastable) 90 m 43 0 0 90 43 Tc→ γ + Tc • Notice that the element does not change Nuclear Stability • Nuclei undergo decay to achieve greater stability. You can use the periodic table to predict the kind of decay that an isotope will undergo. – If an isotope’s mass number is greater than its atomic mass, the nucleus will try to gain protons and lose neutrons….therefore beta decay. – If an isotope’s mass number is less than its atomic mass, the nucleus will try to lose protons and gain neutrons….therefore either positron emission or electron capture – Alpha emission is for the large nuclei, usually with atomic numbers of 80 or greater. Stability Graph Fusion • Fusion involves combining two small nuclei into one larger nucleus. – This occurs on our sun and other stars. – The product is usually not radioactive. – Fusion occurs at very high temperatures. – Need a magnetic field to contain the plasma required for fusion to occur. – Researchers have not as yet been able to control a magnetic field on Earth. If they could, then we could have fusion reactors instead of fission reactors. Fission • Fission involves the splitting of one large nucleus into two smaller nuclei. – This occurs in nuclear power plants. – The products are highly radioactive. – Three fissionable nuclei. • U-235, Pu-239, and Cf-252 – Fission occurs when one of the above nuclei are bombarded with neutrons. Samples of fission reactions 235 92 1 0 90 38 143 54 1 0 U + n→ Sr + Xe +3 n 7 x 108 yr 235 92 1 0 28.1 yr 511 msec 92 36 141 56 1 0 U + n→ Kr + Ba +3 n 1.84 sec 235 92 1 0 132 51 18.3 min 101 41 1 0 U + n→ Sb + Nb +3 n 2.79 min 7.1 sec Mass Defect and Binding Energy • When protons and neutrons come together to form a nucleus, the mass of the nucleus is less than the sum of the masses of its constituent protons and neutrons. – This difference is mass is called the mass defect. – The mass lost is this process is released in the form of energy • If we reverse the process, this is the same amount of energy, called the binding energy, required to decompose the nucleus back into protons and neutrons. • The relationship between mass and energy is given by Einstein’s equation E = mc2 where E = energy in Joules m = mass in kg c = speed of light, 3 x 108 m/sec Half-life • Half-life is the time required for ½ of a radioactive isotope to decay – Some half-lives are very short and are useful in medicine. – Some half-lives are very long and are useful in dating artifacts. – Each radioactive isotope has its own half-life which never changes….it is like a finger print Half-life problems • Half-life problems concern themselves with four ideas – Total time – the overall time covered by the problem – Half-life – symbol is t1/2 – Beginning mass (or beginning # of particles) – Ending mass (or ending # of particles) • Two examples…. Example 1 Phosphorus-32 has a half-life of 28 days. How much time is needed for 84 g of the phosphorus-32 to decay to 5.25 g? Example 2 Hydrogen-3 has a half-life of 12.3 years. If you begin with 100 g of hydrogen-3, how much is left after 36.9 years?