ФЕДЕРАЛЬНОЕ АГЕНТСТВО ПО ОБРАЗОВАНИЮ

ВОЛЖСКИЙ ПОЛИТЕХНИЧЕСКИЙ ИНСТИТУТ (ФИЛИАЛ)

ВОЛГОГРАДСКОГО ГОСУДАРСТВЕННОГО ТЕХНИЧЕСКОГО УНИВЕРСИТЕТА

КАФЕДРА ИНОСТРАННЫХ ЯЗЫКОВ

СЕМЕСТРОВАЯ РАБОТА

(10000 ЗНАКОВ)

 

Выполнила:

студент гр. ВАУ-227

Гранкина Н.В.

Проверила:

ст. преподаватель

Галицына Т.А.

ВОЛЖСКИЙ 2008

THERMODYNAMICS AND THERMOCHEMISTRY Thermodynamics and Energy.

The energy of a body may be defined broadly as its capacity for doing work. This energy may take various forms, such as kinetic energy of a body in motion, potential energy due to position, heat energy as measured by the temperature, electrical energy, chemical energy, etc. Chemical and physical processes are almost invariably accompanied by energy changes, and results of considerable importance have been obtained studying the laws underlying these changes. It is this study of energy transformation which constitutes the subject matter of thermodynamics. Although thermodynamics may appear to be somewhat theoretical in nature, the two laws have led to results of fundamental importance to chemistry, as well as to physics.

Conservation of Energy: The First Law of Thermodynamics.

Many attempts have been made from time to time to realize "perpetual motion", that is, the continuous production of mechanical work without supplying an equivalent amount of energy from another source. The failure of all such efforts has led to the universal acceptance of the principle of conservation of energy. This principle has been stated in many forms, but essentially they amount to the fact that although energy can be converted from one form to another, it cannot be created or destroyed or, alternatively, whenever a quantity of one kind of energy is produced, an exactly equivalent amount of other kinds must disappear. It is evident that perpetual motion, in the generally accepted sense of the term, would be contrary to this principle, for it would involve the creation of energy. Further, the exact equivalence of mechanical or electrical work and heat, as found by Joule and others, is a necessary consequence of the same principle.

The law of conservation of energy is purely the result of experience, no exception to it having as yet been found. The assumption that it is of universal applicability is the basis of the first law of thermodynamics. This law can be stated in any of the ways given above for the principle of the conservation of energy, or else it may be put in the following form. The total energy of a system and its surroundings must remain constant, although it may be changed from one form, to another.

Heat Changes in Chemical Reactions.

The subject of thermochemistry deals with the heat changes accompanying chemical reactions. As will be seen shortly the laws of thermochemistry are based-largely on the principle of the conservation of energy or the first law of thermodynamics. Different substances have different amounts of internal (chemical) energy, and so the total energy of the products of a reaction is generally different from that of the reactants; hence, the chemical change will be accompanied by the liberation or absorption of energy, which may appear in the form of heat. If heat is liberated in the reaction the process is said to be exothermic, but if heat is absorbed it is described as endothermic. The majority of, although not all, chemical reactions which go to virtual completion at ordinary temperatures are exothermic in character, since they are accompanied by an evolution of heat. If a chemical reaction is associated with a volume change, as is particularly the case for many processes involving the combination of gases, the magnitude of the heat change will depend on whether the reaction is carried out at constant pressure or at constant volume. Since many reactions normally occur at constant (atmospheric) pressure it is the usual practice to record heat changes by quoting the value of qp, the heat absorbed at constant pressure; this may, of course, be identified with ΔH , the increase of heat content under the same conditions. This quantity is often referred to as the heat of reaction; it represents the difference in the heat contents of the reaction products and of the reactants, at constant pressure and at definite temperature, with every substance in a definite physical state. From the value of qp (or ΔH) the value of gv (or ΔE) can be readily determined if the volume change ΔV at the constant pressure P is known as will be seen below.

The heat change accompanying a reaction, for example, that between solid carbon (graphite) and gaseous oxygen to yield carbon dioxide gas, is represented in the form of a thermochemical equation, as follows:

C(s) + 02(g) = C02 (g) ΔH = -94.00 kcal.

This means that when 12.01 grams of solid carbon (graphite) and 32 grams of gaseous oxygen react completely to yield 44.01 grams of gaseous carbon dioxide, at constant pressure, there is a decrease in heat content, since ΔH is negative, of 94 kilocalories (kcal.), i. e. , 94,000 calories. It is the general practice in modern thermochemical work to express results in kilocalories because the statement of heat changes in calories implies an accuracy greater than is usually attainable experimentally. It should be noted, incidentally, that the ΔH (or ΔE) values always refer to completed reactions, appropriate allowance having been made, if necessary, if the process does not normally go to completion.

The symbols g, /, and s, placed in parentheses after the formula indicate whether the substance taking part in the reaction is gas, liquid or solid. ............