Chapter 1: Matter and Measurement
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Transcript Chapter 1: Matter and Measurement
A Call For Volunteers
• I have been approached by the special needs
department here at the university requesting
a student interested in helping another
student in class by taking notes.
• Anyone interested in this should see me
after class to make arrangements.
Slide 1 of 25
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
What about a supersaturated solution?
• Consider a supersaturated salt solution.
• Because it is a mixture it is chemically
heterogeneous (salt and water)
• Because there is dissolved and undissolved
salt in the beaker, there are two phases of
the salt making it physically heterogeneous
(two different phases).
Slide 2 of 25
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
General Chemistry
Principles and Modern Applications
Petrucci • Harwood • Herring
8th Edition
Chapter 2: Atoms and the Atomic Theory
Slide 3 of 25
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
Contents
•
•
•
•
•
Early chemical discoveries
Electrons and the Nuclear Atom
Chemical Elements
Atomic Masses
The Mole (save this for Friday)
Slide 4 of 25
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
Early Discoveries
Antoine Lavoisier
Law of conservation of mass
Before reaction = 0.455 g Mg + 2.315 g O2 = 2.770 g
After reaction = ? g MgO + 2.015 g O2 = 2.770 g
0.755 g MgO
Proust 1799
Slide 5 of 25
Law of constant composition
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
Early Discoveries
Lavoisier 1774
Law of conservation of mass
Before reaction = 0.455 g Mg + 2.315 g O2 = 2.770 g
After reaction = ? g MgO + 2.015 g O2 = 2.770 g
0.755 g MgO
Proust 1799
Law of constant composition
Sample A
Composition
10.000 g
Slide 6 of 25
Sample B
27.000 g
1.119 g H
% H = 11.19
3.021 g H
8.881 g O
% O = 88.81
23.979 g O
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
Dalton’s Atomic Theory (1803-1808)
Each element is composed of small
particles called atoms.
Atoms are neither created nor destroyed
in chemical reactions.
All atoms of a given element are identical.
Compounds are formed when atoms of
more than one element combine.
Slide 7 of 25
Chemistry 140 Fall 2002 Dutton
John Dalton
(1766-1844)
Prentice-Hall © 2002
Consequences of Dalton’s theory
Law of Definite Proportions: combinations of elements are
in ratios of small whole numbers.
In forming carbon monoxide, 1.33 g
of oxygen combines with 1.0 g of
carbon.
In the formation of carbon dioxide
2.66 g of oxygen combines with 1.0 g
of carbon.
Slide 8 of 25
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
Behavior of charges
Like charges repel each other
Opposite charges attract
Oppositely charged
particles are deflected
in opposite directions
by a magnetic field.
Slide 9 of 25
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
Cathode ray tube (Discovery of Electrons)
Slide 10 of 25
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
Properties of cathode rays
Electric Field
Magnetic Field
Electron m/e = -5.6857 x 10-9 g coulomb-1
Slide 11 of 25
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
Charge on the electron
From 1906-1914 Robert Millikan showed ionized oil drops
can be balanced against the pull of gravity by an electric field.
The charge is an integral multiple of the electronic charge, e.
Slide 12 of 25
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
Radioactivity
Radioactivity is the spontaneous emission of radiation
from a substance.
X-rays and g-rays are high-energy light.
a-particles are a stream of helium nuclei, He2+.
b-particles are a stream of high speed electrons
that originate in the nucleus.
Slide 13 of 25
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
The nuclear atom
Geiger and
Rutherford
1909
To study
Thompson’s model
of the atom
1. Majority of α-particles penetrated undeflected.
2. Some α-particles experienced slight deflections.
3. A few (1/20000) suffered serious deflections.
4. A few didn’t penetrate but deflected back from where they came.
Slide 14 of 25
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
The a-particle experiment
Most of the mass and all of the
positive charge is concentrated in a
small region called the nucleus .
What actually
happened
What was expected
Slide 15 of 25
There are as many electrons outside
the nucleus as there are units of
positive charge on the nucleus
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
The nuclear atom
Rutherford
1. Most of the mass and all
of the positive charge are protons 1919
centered in a very small
region called the nucleus.
2. The magnitude of the
positive charge is
different for different
atoms and is ½ of the
atomic weight.
3. The atom as a whole is
electrically neutral.
Protons = electrons.
Slide 16 of 25
James Chadwick
neutrons 1932
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
Nuclear Structure
Atomic Diameter 10-8 cm
Nuclear diameter 10-13 cm
1Å
Particle
Electron
Proton
Neutron
Slide 17 of 25
Mass
kg (SI)
9.109 x 10-31
1.673 x 10-27
1.675 x 10-27
amu
0.000548
1.00073
1.00087
Chemistry 140 Fall 2002 Dutton
Charge
Coulombs (SI)
–1.602 x 10-19
+1.602 x 10-19
0
(e)
–1
+1
0
Prentice-Hall © 2002
Scale of Atoms
The heaviest atom has a mass of only 4.8 x 10-22 g
and a diameter of only 5 x 10-10 m.
Useful units:
1 amu (atomic mass unit) = 1.66054 x 10-24 kg
1 pm (picometer) = 1 x 10-12 m
1 Å (Angstrom) = 1 x 10-10 m = 100 pm = 1 x 10-8 cm
Biggest atom is 240 amu and is 50 Å across.
Typical C-C bond length 154 pm (1.54 Å)
Molecular models are 1 Å /inch or about 0.4 Å /cm
Slide 18 of 25
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
Isotopes, atomic numbers and mass numbers
To represent a particular atom we use the symbolism:
A= mass number
Slide 19 of 25
Z = atomic number
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002
Measuring atomic masses
Slide 20 of 25
Chemistry 140 Fall 2002 Dutton
Prentice-Hall © 2002