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"An excellent text, highly recommended." — Choice
When it was first published, this first-year chemistry text revolutionized the teaching of chemistry by presenting it in terms of unifying principles instead of as a body of unrelated facts. Those principles included modern theories of atomic and molecular structure, quantum mechanics, statistical mechanics, and thermodynamics. In addition, Dr. Pauling attempted to correlate the theories with descriptive chemistry, the observed ...
"An excellent text, highly recommended." — Choice
When it was first published, this first-year chemistry text revolutionized the teaching of chemistry by presenting it in terms of unifying principles instead of as a body of unrelated facts. Those principles included modern theories of atomic and molecular structure, quantum mechanics, statistical mechanics, and thermodynamics. In addition, Dr. Pauling attempted to correlate the theories with descriptive chemistry, the observed properties of substances, to introduce the student to the multitude of chemical substances and their properties.
In this extensively revised and updated third edition, the Nobel Prize–winning author maintains an excellent balance between theoretical and descriptive material, although the amount of descriptive chemistry has been decreased somewhat, and the presentation of the subject, especially in relation to the nonmetals, has been revised in such a way as to permit greater correlation with the electronic structure of atoms, especially electronegativity.
The principles of quantum mechanics are discussed on the basis of the de Broglie wavelength of the electron. The quantized energy levels of a particle in a box are derived by means of a simple assumption about the relation of the de Broglie waves to the walls of the box. No attempt is made to solve the Schrödinger wave equation for other systems, but the wave functions of hydrogen-like electrons are presented and discussed in some detail, and the quantum states for other systems are also covered. Statistical mechanics is introduced before thermodynamics, and the discussion of thermodynamics is based on it. This arrangement reflects the author's belief that beginning students can understand statistical mechanics better than chemical thermodynamics.
Aimed at first-year college students who plan to major in chemistry or closely related fields, the book is written in a logical, clear, and understandable style. In addition, many excellent figures are included, along with numerous problems and 75 pages of appendices covering such topics as symmetry of molecules and crystals, hybrid bond orbitals, and magnetic properties of substances.
The Nature and Properties of Matter
1-1. Matter and Chemistry
The universe is composed of matter and radiant energy. Matter (from the Latin materia, meaning wood or other material) may be defined as any kind of mass-energy (see Section 1-2) that moves with velocities less than the velocity of light, and radiant energy as any kind of mass-energy that moves with the velocity of light.
The different kinds of matter are called substances. Chemistry is the science of substances—their structure, their properties, and the reactions that change them into other substances.
This definition of chemistry is both too narrow and too broad. It is too narrow because the chemist in his study of substances must also study radiant energy, in its interaction with substances. He may be interested in the color of substances, which is produced by the absorption of light. Or he may be interested in the atomic structure of substances, as determined by the diffraction of x-rays (Section 3-7 and Appendix IV) or by the absorption or emission of radiowaves by the substances.
On the other hand, the definition is too broad, in that almost all of science could be included within it. The astrophysicist is interested in the substances that are present in stars and other celestial bodies, or that are distributed, in very low concentration, through interstellar space. The nuclear physicist studies the substances that constitute the nuclei of atoms. The biologist is interested in the substances that are present in living organisms. The geologist is interested in the substances, called minerals, that make up the earth. It is hard to draw a line between chemistry and other sciences.
1-2. Mass and Energy
Matter has mass, and any portion of matter on the earth is attracted toward the center of the earth by the force of gravity; this attraction is called the weight of the portion of matter. For many years scientists thought that matter and radiant energy could be distinguished through the possession of mass by matter and the lack of possession of mass by energy. Then, early in the present century (1905), it was pointed out by Albert Einstein (1879-1955) that energy also has mass, and that light is accordingly attracted by matter through gravitation. This was verified by astronomers, who found that a ray of light traveling from a distant star to the earth and passing close by the sun is bent toward the sun by its gravitational attraction. The observation of this phenomenon was made during a solar eclipse, when the image of the star could be seen close to the sun.
The amount of mass associated with a definite amount of energy is given by an important equation, the Einstein equation, which is an essential part of the theory of relativity:
E = mc2 (1-1)
In this equation E is the amount of energy (J), m is the mass (kg), and c is the velocity of light (m s-1). The velocity of light, c, is one of the fundamental constants of nature; its value is 2.9979 × 108 meters per second.
Until the present century it was also thought that matter could not be created or destroyed, but could only be converted from one form into another. In recent years it has, however, been found possible to convert matter into radiant energy, and to convert radiant energy into matter. The mass m of the matter obtained by the conversion of an amount E of radiant energy or convertible into this amount of radiant energy is given by the Einstein equation. Experimental verification of the Einstein equation has been obtained by the study of processes involving nuclei of atoms. The nature of these processes will be described in later chapters in this book.
Until early in the present century scientists made use of a law of conservation of matter and a law of conservation of energy. These two conservation laws were then combined into a single one, the law of conservation of mass, in which the mass to be conserved includes both the mass of the matter in the system and the mass of the radiant energy in the system.
1-3. The International System of Units
The metric system of units of length, mass, force, and other physical quantities was developed during the French Revolution. Because of their greater convenience and simplicity, metric units have replaced native units (such as the foot and the pound) in scientific work everywhere and have been formally accepted for practical use in many countries (all except the United States, Canada, and some African countries). An extended and improved form of the metric system, called the International System (IS, or sometimes SI, for Systéme International ), was formally adopted by the General Conference of Weights and Measures in 1960.
The symbols of the basic IS units and of the prefixes for fractions and multiples and those for some derived IS units are given in Appendix I. If you have made use of the MKS system (meter-kilogram-second system) in your study of physics the IS system will be familiar to you, for the most part, but if you have made use of the cgs system (centimeter-gram-second system) you will have to learn some new units.
The IS unit of mass, the kilogram, is defined as the mass of a standard object made of a platinum-iridium alloy and kept in Paris. One pound is equal approximately to 453.59 g, and hence 1 kg is equal approximately to 2.205 lb. (Note that it has become customary for the abbreviation of units in the metric system to be written without periods.) There is at the present time a flaw in the International System, in that the name for the unit of mass involves a prefix, kilo. This flaw will remain until agreement about a new name and symbol has been reached. In the meantime we must remember that 1 milligram (symbol 1 mg, not 1 ?kg) is one millionth of the unit of mass, not one thousandth, as indicated by the prefix milli.
The IS unit of length, the meter (m), is equal to about 39.37 inches (1 inch equals exactly 2.54 cm). The meter was formerly defined as the distance between two engraved lines on a standard platinum-iridium bar kept in Paris by the International Bureau of Weights and Measures; in 1960 it was redefined, by international agreement, as 1,650,763.73 wavelengths of the orange-red spectral line of krypton 86.
The IS unit of time is the second (s). It is defined as the interval occupied by 9,192,631,770 cycles of the microwave line of cesium 133 with wavelength about 3.26 cm. The second was formerly defined as 1/86400th of the mean solar day.
The IS unit of volume is the cubic meter, m3. In chemistry a unit that is much used is the liter, symbol 1, which is 1 × 103 m3. The milliliter, 1 × 10-3 1, is equal to the cubic centimeter: 1 ml = 1 cm3.
The IS unit of force is the newton (N), which is defined as the force needed to accelerate a mass of 1 kg by 1 m s-2. The newton is 105 dyne (the dyne, the unit of force in the cgs system, is the force that accelerates 1 g by 1 cm s-2). The IS unit of energy, the joule (J), is the work done by 1 newton in the distance 1 meter: 1 J = 1 N m = 107 erg = 107 dyne cm.
In chemistry the calorie has been extensively used as the unit of energy. The thermochemical calorie, defined as 4.184 J (Appendix I), is approximately the amount of energy needed to raise the temperature of 1 g of water by 1°C. The large calorie (kcal or Cal) is 103 cal. In this book we shall use the joule in most of the tables and discussions. Since most thermochemical reference books use the calorie or kilocalorie, you will find it worth while to remember the conversion factor:
1 cal = 4.184 J
1 kcal = 1 Cal = 4.184 kJ
Example 1-1. Niagara Falls (Horseshoe) is 160 feet high. How much warmer is the water at the bottom than at the top, as the result of the conversion of potential energy into thermal energy? The standard acceleration of gravity is 9.80665 m s-2.
Solution. The gravitational force on a mass of 1 kg at the earth's surface is 9.80665 N. The change is potential energy of 1 kg over a vertical distance h (in meters) is 9.80665 × h J. In this problem h has the value 0.3048 × 160 = 48.77 m (conversion factor from Appendix I); hence the change in potential energy produces 9.80665 × 48.77 = 478 J of thermal energy. The energy required to raise the temperature of 1 kg of water by 1°C is given above as 1 kcal = 4.184 kJ = 4184 J. Hence the increase in temperature of the water is 478/4184 = 0.114°C.
Example 1-2. When 2 kg of uranium 235 undergoes nuclear fission (as in the detonation of the Hiroshima atomic bomb on 6 August 1945), 1.646 × 1014 J of radiant energy and thermal energy is liberated. What is the mass of the material products of the reaction?
Solution. We can calculate the mass of the liberated energy by the use of the Einstein equation (1-1). Rewriting this equation by dividing each side by c2 and introducing the values of E and c, we obtain
m = E/c2 = 1.646 × 1014J/(2.998 × 108)2 m2s-2 = 0.183 × 10-2 kg
Thus, the material mass of 2 kg has decreased by 0.00183 kg (that is, by 0.0915%), leaving material products of the reaction with mass 1.99817 kg.
The Einstein relation between mass and energy has been verified by the direct measurement of the mass of the products and of the energy emitted in nuclear reactions.
Example 1-3. It is found by experiment that when 1 kg of glyceryl trinitrate (nitroglycerine) is exploded, the amount 8.0 × 106 J of energy is liberated. What is the mass of the products of the explosion?
Solution. This example is to be solved in exactly the same way as the preceding one. The mass of the radiant energy that is produced by the explosion is obtained by dividing the energy, E, by the square of the velocity of light:
m = E/c2 = 8.0 × 106J/(2.998 × 108)2 m2 s-2 = 0.89 × 10-10 kg
Thus we calculate that the mass of the products of the explosion is 0.999999999911 kg.
We see that the mass of the products of this chemical reaction differs very slightly from the mass of the reactant—so slightly that it is impossible to detect the change in a direct way. The change, less than one part in ten billion (1 in 1010), is so small that for practical purposes we may say that there is conservation of mass in ordinary chemical reactions.
If two objects are placed in contact with one another, thermal energy may flow from one object to the other one. Temperature is the quality that determines the direction in which thermal energy flows—it flows from the object at higher temperature to the object at lower temperature.
Temperatures are ordinarily measured by means of a thermometer, such as the ordinary mercury thermometer, consisting of a quantity of mercury in a glass tube. The temperature scale used by scientists is the centigrade or Celsius scale; it was introduced by Anders Celsius (1701-1744), a Swedish professor of astronomy, in 1742. On this scale the temperature of freezing water saturated with air is 0°C and the temperature of boiling water is 100°C at 1 atm pressure.
On the Fahrenheit scale, used in everyday life in English-speaking countries, the freezing point of water is 32°F and the boiling point of water is 212°F. On this scale the freezing point and the boiling point differ by 180°, rather than the 100° of the centigrade scale.
To convert temperatures from one scale to another, you need only remember that the Fahrenheit degree is 100/180 or 5/9 of the centigrade degree, and that 0°C is the same temperature as 32°F.
The Kelvin Temperature Scale
About 200 years ago scientists noticed that a sample of gas that is cooled decreases in volume in a regular way, and they saw that if the volume were to continue to decrease in the same way it would become zero at about—273°C. The concept was developed that this temperature,—273°C (more accurately,—273.15°C), is the minimum temperature, the absolute zero. A new temperature scale was then devised by Lord Kelvin, a great British physicist (1824-1907). The Kelvin scale is defined in such a way as to permit the laws of thermodynamics to be expressed in simple form (see Chapter 10).
The IS temperature scale is the Kelvin scale with a new definition of the degree. The absolute zero is taken to be 0°K and the triple point of water is taken to be 273.16°K. (The triple point of water, the temperature at which pure liquid water, ice, and water vapor are in equilibrium, is discussed in Section 11-9.) With this definition of the degree, the boiling point of water at one atmosphere pressure is 373.15°K and the freezing point of water saturated with air at one atmosphere pressure is 273.15°K. Hence the IS Kelvin temperature is 273.15°K greater than the centigrade temperature.
1-5. Kinds of Matter
We shall first distinguish between objects and kinds of matter. An object, such as a human being, a table, a brass doorknob, may be made of one kind of matter or of several kinds of matter. The chemist is primarily interested not in the objects themselves, but in the kinds of matter of which they are composed. He is interested in the alloy brass, whether it is in a doorknob or in some other object; and his interest may be primarily in those properties of the material that are independent of the nature of the objects containing it.
The word material is used in referring to any kind of matter, whether homogeneous or heterogeneous.
A heterogeneous material is a material that consists of parts with different properties. A homogeneous material has the same properties throughout.
Wood, with soft and hard rings alternating, is obviously a heterogeneous material, as is also granite, in which grains of three different substances (the minerals quartz, mica, and feldspar) can be seen.
A mineral is any chemical element, compound, or other homogeneous material (such as a liquid solution or a crystalline solution) occurring naturally as a product of inorganic processes. Most minerals are solids. Water and mercury are examples of liquid minerals, and air and helium (from rocks or helium wells) are examples ofgaseous minerals. Amalgam (mercury containing dissolved silver and gold) is an example of a solution occurring as a mineral. Rocks are simple minerals (limestone consists of the mineral calcite, which is calcium carbonate) or mixtures of minerals (granite is such a mixture).
A substance is usually defined by chemists as a homogeneous species of matter with reasonably definite chemical composition.
By this definition, pure salt, pure sugar, pure iron, pure copper, pure sulfur, pure water, pure oxygen, and pure hydrogen are representative substances. On the other hand, a solution of sugar in water is not a substance; it is, to be sure, homogeneous, but it does not satisfy the second part of the above definition, inasmuch as its composition is not definite but is widely variable, being determined by the amount of sugar that happens to have been dissolved in a given amount of water. Similarly, the gold of a gold ring or watchcase is not a pure substance, even though it is apparently homogeneous. It is an alloy of gold with other metals, and it usually consists of a crystalline solution of copper in gold. The word alloy is used to refer to a metallic material containing two or more elements: the intermetallic compounds are substances, but most alloys are crystalline solutions or mixtures.
Excerpted from General Chemistry by Linus Pauling. Copyright © 1970 Linus Pauling. Excerpted by permission of Dover Publications, Inc..
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Posted February 21, 2003
Pauling's writing style is engaging, with just the right mix of technical content, historical treatment, and editorial. The problems included with the text reinforce the subject matter without being too facile. The main drawback is that some of the material is now dated. In particular, some of the physical constants in the text are not longer accurate. Keeping this in mind, this work will serve as a wonderful reference, as well as a great introduction to the subject. As with most Dover publications, an excellent value!!
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