The periodic table is organized rather strangely, at first sight. There is a big gap at the top. There is a whole section excerpted and stuck at the bottom. There seems to be a pattern in atomic numbers for the start of a new row, but it does not work for the first row and stops working after the third row. The reason for the weird appearance of the table lies deep in the inner workings of the atoms. There are underlying patterns and we will use our knowledge of basic quantum mechanics, that is, electron configuration, to explore a few of those patterns. In this activity we will use patterns in electron configuration combined with an understanding of the role of the atomic nucleus to describe and explain trends in effective nuclear charge, atomic radius, and first ionization energies.
It will be useful to have a few definitions. First, the effective nuclear charge (Zeff) is the charge due to the nucleus that is not shielded by electrons in shells closer to the nucleus. For example, the electron configuration of lithium (Li) is 1s22s1. The 2s electron is attracted by a +3 charge from the nucleus but repelled by each 1s electron by a –1 charge, each. The net effect is that the nuclear charge is reduced: +3 + (–2) = +1 so that the effective nuclear charge on the valence electron of lithium is +1. Valence electons are the electrons in the electron configuration of the ground state of an atom that are in the shell with the highest value of n, the principal quantum number. These are easy to figure for elements in groups 1, 2, and 13 - 18 (the s-block and p-block elements). The valence electrons are those in the highest s- and/or p-subshells. Core electrons are all electrons in shells with lower value of n. For s-block and p-block elements the core electrons are equivalent to the noble gas core. For d-block or transition metal elements we count as core electrons the ones found in the nd subshell in addition to those in the noble gas core. The only valence electrons are in the (n + 1)s subshell. For example, the element titanium (Ti) has the electron configuration 1s22s22p63s23p63d24s2. Titanium has only two valence electrons, those designated 4s2. The 3d2 electrons are considered core electrons along with the 18 electrons in the argon-core, [Ar], making a total of 20 core electrons. As you go from one element to the next in the d-block you add an additional proton and an additional core electron, making effective nuclear charge constant across a row. (In reality it increases slightly, but for this activity we will make this simplifying assumption.)
Atomic radius is a simple-enough idea. Picturing the atoms as spheres, what are their radiuses? This can be measured in a lab by various methods, including deviation from the ideal gas law to calculate the empirical van der Waals radius. We will use a theoretically calculated atomic radius, based on quantum mechanics. In this activity one goal is to build an understanding of the trends in atomic radius based on electron configuration and the effective nuclear charge felt by valence electrons.
The ionization energy is the energy needed to remove an electron from an atom. The first ionization energy is the energy required to remove the highest-potential-energy electron from an atom. As a chemical equation, this looks like:
X + energy → X+ + e–
It may seem odd at first to say that we are removing the electron with the highest potential energy. Remember, potential energy increases as you get farther from the nucleus. Far away from the nucleus the electron is taken to have zero potential energy. As an electron goes from far away down into the quantum shells of an atom it gives up energy by radiating photons until it ends up at a position with negative potential energy. From here, in order to be ionized, the electron must absorb energy. The farther down inside the atom the electron is found, the more energy will be required to ionize it. And the farther an electron is from the nucleus, the less energy will be required to ionize it.
The first ionization always removes the highest-energy electron: the electron removed will always have the highest value of n and l in the ground state electron configuration of the element. For example, the electron ionized from titanium (Ti) is a 4s subshell electron, not the 3d. Another example is that the 2p electron is the one ionized from boron (B), not a 2s electron.
Explore a few trends in the atomic properties of the elements as they vary from element to element in the periodic table. Specifically, you will explore:
In your Google doc answer the following questions. Copy and paste the questions from this online document so that they are easy to answer.