| Chem 109 |
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Spring 2009 |
| Lecture Notes:: 30 January |
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| PREVIOUS |
These various laws imply that matter is made up of small discreet units, which we call atoms. The earliest "successful" theory of atoms is that of John Dalton (1803). Dalton's atomic theory states:
All of these statements are close to reality, and nearly describe chemical behavior. But there are exceptions. Thus atoms can be created and destroyed via nuclear processes. They consist of different forms called isotopes. Atoms are not the smallest particles, etc.
Look at the Periodic Chart.
Terms etc.:
Periodic Table of the ElementsIA IIA IIIA IVA VA VIA VIIA VIIIA H He Li Be B C N O F Ne Na Mg IIIB IVB VB VI VIIB VIIIB IB IIB Al Si P S Cl Ar K Ca Ti V Cr Mn Fe Co Ni Cu Zn Ga Ge As Se Br Kr Rb Sr Ag Cd Sn I Xe Cs Ba W Pt Au Hg Pb
First, let's look at the the elements that you should learn the names of, as listed on the web:
The common ions and acids and bases are summarized on the handout and the web:
Note that formulae are more or less written with the elements ordered by electronegativity (elements on the right side precede those on the left).
Atoms are now known to consist of three different types of particles: electrons, protons and neutrons (the common form of one very important atom, hydrogen, has only two kinds: a proton and an electron). The protons and neutrons reside in a small inner portion called the nucleus while the electrons reside in a relatively large cloud centered on the nucleus. Important properties of these particles are listed in the table below:
Particle |
Charge |
Relative Mass |
Mass |
| Electron (e-) | -1 | 1/1840 | 9.11 x 10-28g |
| Proton (p or H+) | +1 | ª1 | 1.67 x 10-24g |
| Neutron (n) | 0 | ª1 | 1.67 x 10-24g |
Some important terms which you must know are:
Isotopes are forms of elements which differ only in the number of neutrons. This means different isotopes of the same element have essentially the same chemical properties but slightly different physical properties. They can also differ substantially in terms of their nuclear stability. Let's look at some examples of isotopes:
| Symbol | Z | A | p | n | e- |
| 14C | 6 | 14 | 6 | 8 | 6 |
| 238U6+ | 92 | 238 | 92 | 146 | 86 |
| 35Cl- | 17 | 35 | 17 | 18 | 18 |
| 18O2- | 8 | 18 | 8 | 10 | 10 |
You should be able to fill in the blanks in a table like this with, the aid of a periodic table, on a quiz.
FYI - Classical Characterization and Descriptions of AtomsDuring the latter half of the 19th century we began to actually characterize what these "atoms" might be like. There were two main lines of experimental work:
When two electrodes are placed in an evacuated tube and a high voltage placed across them a stream of negatively charged particles flows between the electrodes (from the negative cathode to the positive anode). Since they come off of the cathode they are called cathode rays, and the evacuated tube a cathode ray tube (the ancestor of todays TV or computer monitor cathode ray tube or "CRT"). These rays can be diverted with magnets or charged plates outside the tube. In fact by careful manipulation 19th century physicists were able to determine the ratio of the mass to the charge of the cathode rays. (The cathode ray is also known as the electron.) In the early 20th century Milliken determined the charge on the electron by watching the rate of fall of tiny oil drops between two charged plates. The droplets had been ionized (charged) by exposure to x-rays. He noted that the droplets behaved like they had a multiple of some smallest charge on them, and determined this charge to be that of a single electron. Thus Milliken determined the charge on a single electron by making the assumption that the stepwise charge on the oil drops was due to single electron differences = -1.6 x 10-19 Coulomb. With Thompson's determination of the charge/mass ratio for cathode rays (electrons), the mass of the electron could be calculated as = 9.11 x 10-28g. Goldstein used a modified Crook's tube with the cathode in the middle with a hole in the center and found positive rays, which he called "canal rays." These particles had positive charges in multiples of +1.6 x 10-19 C, but variable charge to mass ratios! Thus matter consists of electrons and positively charged particles to make neutral matter. Thompson proposed an atom based on this information (c. 1890) called the "plum pudding model" in which the atom is a positively charged mass with negative electrons distributed through it like raisins in a pudding. However, this model was destroyed by the next great bit of experimental evidence. Rutherford used a source of a-rays and aimed them at a thin foil of metal (1911). By the plum pudding model he expected that these particles would be slowed or deflected. He was very surprised to find that nearly all of the particles passed through the foil unobstructed, while some were deflected a lot, even being essentially reflected back to the source! So what does this mean for the description of the atom? It must consist of mostly empty space, with the positively charged portion confined to a very small space, a nucleus, in the center. |
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© R A Paselk
Last modified 31 Janaury 2009