Readings for this section
Petrucci: Chapter 8
Newtonian physics deals with macroscopic (bigger than microscopic) objects and their interactions. It can deal with such things as inertia, gravity, collisions between large objects, etc. We are generally familiar with macroscopic physics concepts as described by Newton.
At the atomic level, Newtonian physics doesn't work. Atoms are made of small (sub atomic) particles that do not obey Newtonian physics. Over the first half of this century, the theory now referred to as Quantum Mechanics, a.k.a., quantum chemistry, was developed. There are now several kinds of quantum mechanics theories. The earliest ones are now referred to as Classical Quantum Mechanics as opposed to more recent theories like Relativistic Quantum Mechanics. The most fundamental of these sub atomic particles, that we are interested in, is the electron. It's thought to be indivisible. All of Quantum mechanics is based on this premise. In a recent issue of New Scientist, a report was published of an experiment which successfully split an electron into two smaller particles. If this report holds up under scrutiny, then Quantum Mechanics as we know it will need to be replaced with a new theory which allows for this to happen. This is all part of the scientific process, where we take our current models (understanding of reality) and metaphorically speaking, throw rocks at them trying to see if we can knock them down. The failure of a particular model is a good thing as it allows us to then develop new and better models and to know the conditions under which the old model may still be used.
These next few units will explore the various models that we need to understand as a basis to all of chemistry. We'll start with small and very simple models and expand to more and more complex ones describing whole molecules and even macroscopic matter (crystals).
Light has behaviours and properties that can be modelled in several ways, depending on the particular property we are observing or measuring. For example, light behaves as if it is made up of waves, when measured using appropriate experiments. The waves in particular are waves of electric field $\vec{E}$ and magnetic field $\vec{B}$, as illustrated below. Some measureable properties of wave-like properties are the wavelength λ and frequency ν. The frequency and the wavelength are related to the speed of the light in a vacuum, c, according to the equation
λ × ν = c .
The speed of light depends on the medium through which it is passing and it generally slows as it passes through a transparent medium, like clear glass, water or air. The slowing can be thought of on a microscopic level as resulting from the individual packets of light energy being absorbed and re-emitted repeatedly as it encounters the atoms of the material. The slight delay these absorptions and re-emmissions cause 'slows' the progression of the light. The speed of the light in a medium v is related to the speed of light in a vacuum by the index of refraction of the material via
\[n=\frac{c}{v}\]
We don't worry about the index of refraction or the variable speed of light in a medium very much in first-year chemistry but we should still be aware of the concepts.
Figure: One model of light shows waves of magnetic and electric fields alternating in a sine-wave pattern. Each field is oscilating perpendicular to each other. The two alternating fields together make up the light wave. |
Light interacts with material when some property of the light matches a feature of the matter. For example, when the electric field oscillation of the light matches an electric field change in material then light can be absorbed as energy in to the matter. This happens in a microwave oven, where the polar water molecules in the food rotate at a frequency that matches the electromagnetic waves hitting it. The molecules absorb the energy and thus heat up.
light can also be absorbed when the magnetic oscillating field matches some
property of matter. For example, in Magnetic Resonance Imaging, MRI, the
magnetic nuclie of protons, which are held in place the magnetic field of the
big magnet will switch orientations when just the right amount of energy of
light hits it.
We can see that the electromagnetic spectrum consists of a wide range of frequencies from radio-waves with wavelengths on the scale of mountain ranges and continents to gamma rays with wavelengths smaller than an atom. The visible spectrum makes up a very small part of this continuous range of wavelengths. Radio waves cover wavelengths as big as mountains and continents and as small as a person. Microwaves are smaller, generally in the centimeter lengths. Other types of light are shorter still.
Figure: The electromagnetic spectrum includes all types of electromagnetic radiation with wavelengths ranging from very long waves (10^{10} m) to very short waves (10^{-16} m). We generally classify different types of light, depending on the wavelengths of the light. The boundaries separating the different types of light are not always well defined. types of waves are generally classified, from longest to shortest waves as: radio waves, microwaves (µwaves), infrared light (IR), visible light, ultraviolet light (UV), x-rays and γ rays. |
There are two basic types of physical properties that can be used to categorize nature. These are:
Particles.
Objects with mass and possibly charge.
Can always
measure position and momentum but not necessarily at the same time.
Waves.
Periodic function (oscillatory motion)
Cannot exist
at a point, displaced over time and space.
Both matter and light have some properties (behaviours) that can be categorized as "wave-like" and other properties that can be called "particle like".
Electrons can be diffracted like light waves (electron diffraction patterns through metal foils) yet we think of them as particles.
Light waves can behave like particles (photo-electron effect) yet we think of them commonly as waves.
Where do we see wave-like behaviour? Wave-like properties are observable in such experiments as
when we use lenses and mirrors and prisims to manipulate light, we are working with the wave-like properties of the light. Even particals can exhibit wave-like properties. The electron microscope uses high energy electrons to illuminate material so it can be viewed on a very small scale. The wave-like properties of the electrons are being used here. The reason we need to use an electron beam rather than a light beam is that the size of the 'waves' of the electrons is very small compared to visible light and we can 'see' features in the matter that are the same size as the wavelength of the electrons.
Louis de Broglie proposed an equation that connects the momentum of the partical with the wavelength of the particle.
\[\lambda = \frac{h}{p}=\frac{h}{mu}\]
where h is Planc's constant, p is the momentum of the particle, otherwise calculated as mass, m, times speed, u. We use u for speed in this case since the partical microscopic. If we wanted to use this equation on a macroscopic partical (say, a baseball) we might use v for the speed but we would also calculate a wavelength that is substantially smaller than the size of the particle itself and hence would not be meaningful.
The particle-like properties of light is known to exist. The solar system is clear of most interstellar dust and particles because light has momentum (even though it has no mass) and the momentum pushes on the matter in the solar system, sweeping it clear.
Here on earth, we can observe partical like behavior in several ways. Pigments and dies are colored because the matter interacts only with light of particular energies. The fact that we can observe these particular energies means that the light itself has specific energies associate with it. This is not a wave-like behaviour because if we could use waves to describe absorption of energy, then any wavelength of light would do for a given energy need, we would need only allow a long-enough string of light to be absorbed to 'add up' to the required energy. But it doesn't work that way. We see colours, that means the wavelength is connected to the energy of the light and we cannot adjust the amount of energy by 'cutting the string' at different lengths.
To explain the 'particle-like' behaviour, we consider light to be made up of wave packets, each of which can behave in some ways like a particle. The energy of such a packet of light, called a photon, is defined by the equation
E = hν
where h = Planck's constant and ν is the frequency of the light packet. The waves of light, are sine waves. Since sine waves are related to circular motion (yes, there is such a thing as circularly polarised light), we may wish to describe the frequency of light as a function of radians per second, rather than waves per second. This angular frequency ω is defined as
ω = 2π × ν.
Our energy equation, using angular frequency can be written as
\[E=\frac{h\nu}{2\pi}\]
We would like to make this a simpler equation to work with so we define a new physical constant called h-bar as follows
ħ = h/2π
thus we can now write our energy equation as
E = ħω.
A particularly useful example of using the particle like behaviour of light is the photo-electron effect. In this experiment, we observe that when light of sufficient energy strikes metal, electrons are ejected. By measuring the energy of the ejected electrons, we can perform some simple and interesting experiments.
Figure: The photo-electron effect involves a setup where we shine light on the surface of a metal. We can measure the kinetic energy of the electron by adjusting the voltage difference between the grid and the metal. If the voltage is too high, the electrons will be stopped and sent back to the metal. At a particular threshold stoping voltage, V_{s}, the electrons will be just stopped. Any lower voltage will not stop the electrons so we will be able to detect that as a current running through the aparatus. The exact voltage that stops the electrons depends on the frequency of light that we used. |
The electron will generally require some amount of energy just to be extracted from the metal. This is called the work function of the metal (something akin to the ionization energy of a molecule) and is given the symbol φ. If the particular photon that hits the metal and extracts the electron has more energy than the work function, then the excess energy goes into kinetic energy in the electron. The electron's kinetic energy (KE) is measured as the stopping voltage times the electron charge (KE = e×V_{s}). Thus, by using a series of different photon frequencies, we can determine the stopping voltage for each experiment and from that extrapolate to find the point where (KE=0). This is called the threshold frequency (ν_{0}), where the energy of the photon exactly equals the work function of the metal (hν_{0} = φ). At higher energy experiments, we can equate the photon energy to the sum of the work function and the exess kinetic energy
hν = KE + φ
Figure: Graph of the stopping voltage versus the frequency of light used in a photo-electron experiment using an aparatus like the one pictured above. the circled points represent a dat point from a single experiment where a particular frequency of light requires a particular stopping frequency. If we replotted this data with Kinetic energy on the vertical axis, rather than stopping voltage (KE = e×V_{s}) we would get a line with a slope exactly equal to Planck's constant. |
We normally experience the macroscopic world (larger than a microscope) where our observations are of measurables that are merely averages of the microscopic state of the matter. For example, we can easily measure the average kinetic energy of a gas (temperature), the momentum of a moving object, etc. Using light, we can probe the quantization inherent in atoms and molecules that we cannot otherwise detect with our own senses.
We begin with the hydrogen atom, the simplest of all atoms and the only one for which we have exact (analytical) equations that describe the energy states.
$\leftarrow$ Hydrogen Spectrum | |
$\leftarrow$ Energy levels with transitions shown lined up with the spectral lines. |
This equation is useful to determine the energy difference between two different energy levels in a hydrogen atom. When an electron jumps from one level (n_{i}) to a different one (n_{f}), there is an energy transfer involved. This energy could be thermal or it could be photon energy. It's easier to measure photon energy on an individual atomic basis since ΔE = hν. Where ν is the frequency (s^{-1}) of the photon emitted or absorbed by the hydrogen atom and h is Planck's constant. Since ν = c/λ, we can use the reciprocal of wavelength (called wave number) as a measure of energy directly. Thus, 1/λ is directly proportional to energy.
\[\Delata E=R_H \left|\frac{1}{n_1^2}-\frac{1}{n_2^2}\right|\] |
This equation gives the energy change when an electron moves from electronic energy level n_{1} to n_{2} or vice versa (note the absolute value signs), for an individual atom of hydrogen. One can easily determine the wavelength of the emitted (or absorbed) photon of light that is associated with this energy level change by dividing by Planc's Constant |
The symbol R_{H} represents the Rydberg constant and has a value of ~2.179×10^{-18} J. The magnitude of the change in energy of the hydrogen atom ΔE is the same as the energy of the photon E_{photon} emitted or absorbed in the process. The absolute value symbol means this equation does not distinguish between an absorption process (n_{1}<n_{2}) and an emission process (n_{1}>n_{2}).
The Rydberg equation is a phenomenological equation. That means that it models the observed phenomenon, the discrete energy pattern observed in the H-atom spectrum (and other one-electron ions); but that there is no theory behind it. It simply works! We need to try to develop models that explain the observed behaviour as described in the Rydberg equation. One such model is the Bohr model.
Bohr proposed a model, which explained the Rydberg equation. (See Reference Here)
Bohr was able to use classical mechanics to describe the energy levels. Using Columbic interactions between the electron and the nucleus and using the concept that the electron's angular momentum is quantized and must be an multiple of h/2π, he was able to calculate the Rydberg constant using fundamental constants.
\[R_H=\frac{m_e e^4}{8\,\varepsilon_0^2\,h^3\,c\left(1+\tfrac{m_e}{m_p}\right)}\times hc\]
The "× hc" at the end of the equation is to convert the units from m^{-1} to J. What Bohr's model did not explain was why the electrons did not simply spiral down to the centre (nucleus) and continuously loose energy. It also fails to accurately calculate energies for anything other than a one-electron atom or ion. We'll also see that it fails on a few more experiments as well.
What the is Energy and wavelength of a photon emitted when an e^{-} drops from the n=4 to n=2 energy level in a H atom?
\[\Delta E=2.179\times10^{-18}\mathrm{J}\left|\frac{1}{4^2}-\frac{1}{2^2}\right|=4.08_{56}\times10^{-19}\;\mathrm{J}\]
\[\Delta E_{\mathrm{photon}}=4.08\times10^{-19}\;\mathrm{J}\]
The wavelength can be calculated easily using the non-rounded value (keep the subscripted digits).
\[\lambda=\frac{hc}{E_{\mathrm{photon}}}\]
\[\lambda=\frac{6.62606957(29) \times 10^{-34}\;\mathrm{J\;s} \times 299,792,458 \mathrm{m/s}}{4.08_{56}\times10^{-19}\;\mathrm{J}}=4.86\times10^{-7}\;\mathrm{m} \]
\[\lambda=486\;\mathrm{nm} \]
Rydberg and Bohr did a good job explaining the hydrogen atom. Unfortunately, their model falls apart for anything else.
While other atoms also show line-type emission spectra, they are much more complex spectra that are not easily explained as was done for hydrogen. This is because there are more electrons and hence the calculations are more complex. To this day, there is no simple equation to describe the pattern of lines for any atom other than hydrogen.
Each atom displays a unique pattern of frequencies. This allows allows for a technique called Atomic Absorption (AA) to detect specific atoms. AA can detect atoms in stars and interstellar space.
A more complete model needs more quantum numbers to fully define all the electrons in an atom:
n : principal quantum number (q.n.)
n = 1,2,3,...,∞
n–1 is the number of
nodes in any orbital in the n^{th} level.
l: orbital (angular momentum) q.n.
l = 0,1,2,...,n-1
l indicates the number of nodes in the orbital that
are angular. The rest must be radial nodes (spherical)
m_{l}: magnetic q.n.
-l ≤ m_{l} ≤ l
m_{l} corresponds to the orientation of the
orbital nodes.
m_{s }: electron spin (magnetic) q.n.
m_{s} = ±1/2
To better understand the concept involved here, and to try to develop a picture of the concept discussed herein, let's look at a series of macroscopic harmonic oscillators and see if we can find any trends.
If the string vibrates with one continuous motion over it's whole length, then it is vibrating in the lowest energy mode. We have a standing wave with length of 2l. If the string is prevented from vibrating in certain positions (nodes) the string will be forced to vibrate in a different mode. Each of these modes differs by the number of nodes in the wave function and in the frequency that results. (Listen). Note that to excite a particular mode of vibration, it is best to pluck the strung near the maximum in the vibrational wave function.
Did you ever listen to a steel drum player? By tapping on different parts of the drum surface, (s)he can make different notes sound out of the instrument. That's because there are carefully placed dents in the surface of the drum that tends to damp out certain vibrations and which set up vibrational modes in the surface with maxima located in different places around the surface. By tapping in the location of a maximum of a particular vibrational mode the player can excite just that one mode and hence sound one note. By tapping a different place, a different vibrational mode is excited and hence a different note. Again the basic principal that the higher the number of nodes, the higher the vibration frequency is found to be true here in 2-d just like in 1-d sound.
Harmonics in 3-d are not quite as easy to relate to musical instruments since most musical instruments are designed to vibrate in 1 or 2 dimensions, not three. Imagine a sound wave in a spherical container. Certain 3-d standing waves would tend to get established with high and low sound intensities at different regions and for different modes of vibration.
The basic types of nodes in the 3-d case are:
It turns out that the properties of standing waves in a spherical system are very well described by a system of mathematics called spherical harmonics. This same mathematics works well to describe the electronic wave functions of hydrogen atoms.
Notice that in all the previous cases, 1-d, 2-d and 3-d the following was true.
The lowest energy vibrational mode had no nodes (mode level 1)
The second level of vibration had one node (level 2) and in higher than 1-d, there were the possibility of more than one type of node.
The third level of vibration had 2 nodes, etc. Using the 3-d example, we can relate the nodes and their types to the quantum numbers discussed earlier. From now on, I'll be discussing spherical harmonics as they relate to electron wave functions and I'll be using the word 'orbital' to mean wave function. In this case, the type of orbital, obviously is a function of the type (or lack) of nodes.
We have now seen that spherical harmonics describe the number of orbitals and also their shape. Let's recap this information and relate it to the symbols commonly used to indicate the type of orbital.
The orbital quantum number l describes the type of orbital. While the number m_{l} details its orientation. The shape of the orbital nodes can be determined from l as follows:
We can also use these numbers to count the total number of orbitals for any given value of the n.
n |
l |
m_{l} | type |
# orbitals |
---|---|---|---|---|
1 | 0 | 0 | 1s | 1 |
2 | 0 | 0 | 2s | 1 |
1 | -1,0,+1 | 2p | 3 | |
3 | 0 | 0 | 3s | 1 |
1 | -1,0,+1 | 3p | 3 | |
2 | -2,-1,0,+1,+2 | 3d | 5 |
Once we try to establish the actual electron count, we need yet one more quantum
number. The electron spin is designated by the quantum number m_{s}
,
which can have a value of +1/2 or -1/2
According to the Pauli Exclusion Principle, no two electrons can exist in an atom with the same set of these four quantum numbers.
Another way of saying it; Every orbital can have at most two electrons in it and these two must have opposite spin.
Explains the electron count in the various shells of the atom
n = 1 | 1 s orbital | | | 2 electrons | ||
n = 2 | 1 s orbital, | 3 p orbitals | | | 8 electrons | |
n = 3 | 1 s orbital, | 3 p orbitals, | 5 d orbitals | | | 18 electrons |
... |
Combining the functions which describe the electron with other energy-calculating functions (hamiltonian) we can calculate the energy expected for any given function. The energy levels for an electron in a hydrogen atom can be calculated. These different calculated energy levels can be enumerated using quantum numbers n and l. If we add q.n. m_{l}, we now have a complete enumeration of the orbitals and q.n. m_{s} finally enumerates the electrons.
The periodic table shows the elements grouped according to the quantum numbers of their outermost valence electron.
the columns correspond
(in groups) to l.
The groups (blocks) of elements in the periodic table are indicated as follows.
To help understand the way the elements are organized in the periodic table, we need to see how electrons are located in the different atoms. We have two different basic concepts we need to work with in order to be able to work out the arrangement of the electrons, the Aufbau principle and the Pauli exclusion principle.
The Aufbau prinicple (or aufbau process) simply states that the electrons in ground-state atoms will always occupy the lowest energy orbitals first and will only occupy higher energy levels when the lower ones are all filled. The energy levels for a multi-electron atom are depicted in the figure below left. In this graphical, we see that the energy of the levels generally goes up as n goes up but also there is an increasing trend as l goes up. As we get higher in n, the differences between the levels becomes smaller such that the higher l levels of one n level often are nearly the same or even higher than the lower l levels of the next higher n level. For example, the 3d energy levels are nearly the same or even slightly higher than the 4s energy levels for atoms that have 20 electrons or more. This is due to a process called shielding.
The Pauli exclusion principal tells us that there can be at most two electrons in a given orbital so we can now begin the process of filling up the electrons into the energy levels of the atom for whatever atom we are given.
We would fill up electrons by placing them (two per orbital) starting with the lowest energy levels and building up the electron configuration. A way to remember the sequence of orbitals without the need to draw the energy levels out in diagram form is to write the orbital identifiers (1s, 2s, etc.) as shown on the right of the diagram above and then draw diagonal arrows as shown in red. Starting at the top, the levels are filled in sequence as directed by the arrows. The number of electrons in any given set of orbitals is given as a superscript (1s^{1} means one electron in the 1s orbital). Remember that some class of orbitals have more than one individual orbital. These are called degenerate (meaning same energy) orbitals . For example, there are three degenerate p orbitals so the set of p orbitals can have up to 6 electrons occupying them. Similarly, there are 5 degenerate d orbitals so there can be up to 10 d electrons and similarly, up to 14 f electrons.
Thus, a 15 electron atom (P), in its ground state, would be filled to give the following electron configuration.
1s^{2} 2s^{2} 2p^{6} 3s^{2} 3p^{3}.
Alternatively, we can follow the rows of the periodic table to determine the order of filling the orbitals. Unfortunately, we don't always have such a reference with us and hence the memory technique is good to know too.
It is always important to recognise that these discussions apply to ground-state atoms only. For example, a hydrogen atom in its ground state will have an electronic configuration of 1s^{1}. However, if the Hydrogen is in an excited state (has more energy), that single electron will occupy a higher energy level. For example, 3d^{1} is a valid electronic configuration for hydrogen. It's just not a valid ground-state electronic configuration. Similarly, 1s^{2},2s^{2},2p^{4} is a valid electronic configuration for the groundstate oxygen atom while 1s^{2},2s^{2},2p^{3},3s^{1} is one of an infinite number of valid excited-state configurations you might encounter for oxygen.
Note that levels 4s and 3d in the multi-electron atoms are very close to each other in energy. This also holds for 5s,4d and 6s,5d combinations. This leads to some exceptions to the rules normally used to assign the ground-state electronic configuration as we shall see below.
H (1e^{-}) 1s^{1}
He (2e^{-}) 1s^{2}
O (8e^{-}) 1s^{2} 2s^{2} 2p^{4}
S (16e^{-}) 1s^{2} 2s^{2} 2p^{6} 3s^{2} 3p^{4}
Ti (22e^{-}) 1s^{2} 2s^{2} 2p^{6} 3s^{2} 3p^{6} 4s^{2} 3d^{2}
Cr (24e^{-}) 1s^{2} 2s^{2} 2p^{6} 3s^{2} 3p^{6}
4s^{2} 3d^{4}
If we strictly follow only Hund's Rule and
the Aufbau process, this is what we get. Experiment shows this to be
incorrect. The correct electronic configuration for Cr is
1s^{2} 2s^{2} 2p^{6} 3s^{2} 3p^{6}
4s^{1} 3d^{5}
or we can write it with the 3d and 4s
reversed, as some people seem to prefer because after the Hund's rule
stabilization occurs, the 3d are actually lower than the 4s energy levels.
1s^{2} 2s^{2} 2p^{6} 3s^{2} 3p^{6} 3d^{5}
4s^{1}
Cr is one of the exceptions. The 3d shell prefers to be half filled (5 electrons) since this is a perfectly spherical configuration. There is significant relaxing of the energy levels in this configuration, such that the energy for the 3d electrons actually drops below the 4s energy. This type of situation arises whenever one can exactly half-fill or completely fill the d-shell.
Exactly filled or half-filled shells are spherically symmetrical and are more stable. In the case of the d-shell, since the s electrons of the next period are so close in energy, it is possible to promote an electron from the s shell to the d shell of the previous period, thus (half) filling the d shell. This filled (or half-filled) state is more stable and the d shell becomes lower in energy than the s shell of the next higher n level. Hence, In these cases, the normal sequence of filling the orbitals is changed.
Shells | Half-filled | Filled |
s | 1 | 2 |
p | 3 | 4 |
d | 5 | 10 |
To illustrate these cases, we use box diagrams. A box diagram uses small boxes to represent the orbitals in an atom and arrows in the boxes to represent the electrons. The direction of the arrow (up or down) represents the spin of the electron (up spin or down spin; m_{s} = +1/2 or -1/2). At this stage, we need to introduce one more principle, Hund's rule, to better understand the occupancy of the electrons in the orbitals.
Hunds Rule states that the lowest energy configuration for a multi-electron is one where the total electron spin is highest (for a given occupancy level of orbitals). Thus, if there are multiple orbitals with the same nominal energies (a set of p orbitals or a set of d orbitals, for example) then the electrons will occupy the orbitals one at a time with the electron spins parallel. After all the degenerate energy levels are half filled then if there are any further electrons to add, they will occupy the same orbitals, with the spins opposite from the first ones. We see Hund's rule coming into play in the table of box diagrams below in atoms of O and Cr. Actually, the Cr seems to break the rules in that even the 4s orbital is half filled.
The Chromium atom has its 3d shell exactly half-filled in its most stable configuration. This can occur because the energy level 4s and 3d are nearly the same so the energy required to promote one 4s electron to the (slightly higher) 3d energy is more than compensated for by the lowering of the five 3d orbitals once Hund's rule kicks in.
We would expect similar exceptions from the sequencing given above in other atoms in the Cr family. Also, exceptions occur in Cu and its family where the d^{10} configuration with one lone s electron is favoured over the alternative where one d orbital is half filled but the s has two electrons. Thus the electron configuration for Cu = [Ar]3d^{10}4s^{1} is lower than [Ar]3d^{9}4s^{2}.
Electronic configurations for the metals in the fourth
row of the periodic table (Ca-Zn). We see the results of applying
Hund's rule here as the total electron spin is kept as high as possible. * exceptions to the normal sequencing are indicated. |
Now that we've seen the way that we can build up the electronic configuration of the atoms and how to organize the atoms into a periodic Table, according to their electronic configurations (quantum numbers) we can now look at some trends
The first trend of import is in the atomic radius. The force of attraction between the outermost electron(s) and the nucleus affects the atomic radius. The force of attraction of two charges is given classically by Coulombs Law.
.
In the case of quantum mechanics, we cannot calculate a value for r exactly. And must rely on some mean value <r> of the distance between the nucleus and the electron. Charges q1 and q2 represent the charge of the electron and the nucleus, respectively. For the purpose of discussing trends it is convenient to use the concept of core charge. The core charge represents the charge experienced by the outermost electrons of an atom, assuming the inner electrons shield the nucleus from their 'view'. For example, in the atom Li there are two electrons in the 'core' shell (1s) and one in the 'valence' shell. The outer electron (2s^{1}) sees the nucleus (Z=3) only through the screen created by the two core electrons. Thus, it sees a core charge of Z - 2 = 1. More generally, the Core charge can be defined as
Core Charge = Z - # inner electrons.
It turns out that, If we ignore the transition metals, we can simply take the column number to be the core charge, for example, Oxygen is in column # 6 and has a core charge of +6. Thus, along a given row, the orbitals are all approximately the same size but the the attraction of the electron for the nucleus (core) in creases from left to right. Since the core charge increases from left to right along any one row, we expect the atoms on the right side to be smaller than those on the left. Similarly, as one descends a given column the core charge remain the same but the size of the orbitals increase.
Core Charge assumes that inner electrons shield the nuclear charge completely from the outer electrons. In reality, the orbitals in which these outer electrons exist actually penetrate the inner orbitals somewhat such that the effective shielding is not 100%. In addition, electrons in the same shell can partially shield each other somewhat. The amount of shielding and the final effective nuclear charge depends on differences in orbitals, and how they interact with each other. For example, s orbitals have more electron density near (or even on) the nucleus than a p orbital with the same principal quantum number and so shields the nucleus better (and is less effected by shielding from other orbitals) than the p.
The First ionization energy of an atom is the energy required to remove one electron from the neutral atom as described by the equation below.
M -----> M^{+} + e^{-} ΔH = ionization energy
Arguments similar to the ones given for atomic size play a roll here. This time, the larger the force of attraction, the larger will be the amount of energy required to pull the electron away. If we plot actual energies as a function of atomic number (or column in the periodic table, we can see this trend more explicitly.
Note how the ionization energy increases as we go from left to right along the different rows of the table. This follows the concept of Coulombic attraction. However, there are a few dips in the curve which bare considering. Be is higher than B (and Mg > Al, Ca > Ga as well). This makes sense since the former of each of these pairs represents the atom with a filled s orbital. The next orbital in the list is a p that is higher in energy (closer to the zero mark called completely removed). Thus the drop in ionization energies even though the force of attraction would be higher according to our first hand-waving discussion.
There is a similar drop in ionization energies as we move from column 5 to column 6. Here, we are transitioning from an exactly half-filled p-shell to one in which one extra electron exists. Since the half-filled shell is particularly stable, we expect a high ionization energy (for N, P, As...) whereas that for O, S, Se will be slightly lower (trend wise).
For second, third, etc, ionizations, the general trend within an atom is that each subsequent ionization is harder than the previous. This makes sense since each subsequent ionization represents the removal of a negatively charged electron from an increasingly positive ion (more attraction for the electron) and each subsequent electron is in a lower orbital on the given atom. For example, the second ionization energy is the energy required to remove the second electron from the atom, i.e., the energy to remove one electron from a +1 cation. Arguments similar to those for the first ionization energy hold when discussing the relative ionization energies of the various atoms.
Lets compare the relative ionizations of Na with Mg. Their first ionizations as plotted in the graph above show that Mg holds it's outermost electron more tightly than Na since φ_{1}(Na) is lower than φ_{1}(Mg). However, when we look at the +1 ions resulting from these ionizations, we see that the Mg^{+1} still has one electron in the 3^{rd} shell (It's isoelectronic with Na) whereas the Na^{+1} has its outer electron in shell 2 (It's isoelectronic with Ne). It's much harder to remove an electron from the second shell than from the third since the second is closer and more strongly held by the nucleus. So while there has been a large jump in difficulty in removing the electron from the Na^{+1}, compared to the neutral, there's only been a small jump in energy required to remove the second third-shell electron from the Mg^{+1}. Hence, the second ionization energy of Na is higher than the second ionization energy of Mg.
It's dangerous to try to carry this type of argument too far into the levels of ionization of all atoms. There are too many factors involved to be able to perfectly explain all relative energy comparisons using any simple theory. More complete atomic orbital calculations would be required to precisely determine these energies.
We can see a similar trend in the electron affinity comparisons. Electron affinity is the energy of attraction of the neutral atom for one extra electron. (How much energy does it take to add one electron to an already neutral atom as given by the formula below.
M + e^{-} -----> M^{-} ΔH = electron affinity
(Note that ΔH can be thought of as negative of the the ionization energy of the anion)
Again, There is interplay between the relative size of the atom and the relative charge of the nucleus. The electron affinities listed here are for the first three rows in the periodic table (excepting the transition metals). We see that the highest affinities are displayed by the elements F and Cl (from the 7^{th} column). These belong to the Halogens. The Halogens as a family have the highest electron affinity of the elements. That also makes sense using Coulomb's law wherein the Halogens experience the highest 'core charge'.
One might ask: 'Why do the Nobel gases not have a higher electron affinity than the Halogens?'. The answer lies in the fact that the Nobel gases have a completely filled outer shell and any extra electron added thereon would have to go onto the next higher shell which is of course higher in energy (not as attractive). These are not even included in the diagram above since they have virtually no tendency to form negative ions.
The reactivity of the elements in any one column (family) will tend to have similarities.