| Lecture
        #8 | 
    
        | Text: Section 12.15 | 
            
                | CURMUDGEON
                GENERAL'S WARNING. These "slides"
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                academic performance in 09-105. |  | 
    
        | Lecture Outline | The Periodic Table (continued) 
            Ionization energies Second and third ionization energies Electron affinity | 
    
        | The energy needed to remove the easiest-to-remove
        electron from a neutral atom is called the first
        ionization energy. |  | 
    
        | First ionization energies for light elements. Using
        this information, we can estimate the effective nuclear
        charge, Zeff, for the electron being removed.
        Helium as an example. |  | 
    
        | Zeff for lithium |  | 
    
        | Zeff for neon |  | 
    
        | The detailed trend in ionization energies for the
        light elements |  | 
    
        | The n=1 shell filling |  | 
    
        | The n=2 shell filling after which the n=3 shell
        starts |  | 
    
        | Starting the p-subshell causes a break in the smooth
        trend across the row. |  | 
    
        | Starting to pair up electrons after half the
        p-subshell is filled causes a second break, which we
        referred to as the mid-shell dip, in the smooth trend
        across the row. |  | 
    
        | First ionization energies across rows 1 through 3 of
        the Periodic Table |  | 
    
        | Overlapping the 2nd and 3rd row element first
        ionization energies to demonstrate the repeating pattern
        (determined by valence electron configuration) |  | 
    
        | Second ionization energies |  | 
    
        | First, second, and third ionization energies for the
        light elements |  | 
    
        | First, second, and third ionization energies shifted
        to show, again, that valence electron configuration is
        the determining driver |  | 
    
        | Electron affinity is the energy involved in
        adding an electron to a neutral atom to form a negative
        ion. It is numerically equal to minus the ionization
        energy for that negative ion. As such, we should expect
        that the electron affinities also depend on electron
        configuration. |  |