1.1 System and Environment
Thermodynamics is a study of the interaction of a system with its environment. A system is part of the universe contained within a prescribed boundary that we deal with. Everything outside the boundary is called the environment. Thus, the system and its environment constitute the universe.
The boundary of a system may be a real physical boundary or could be imaginary. The boundary may be of arbitrary shape and could move when the volume within the boundary changes such as when the system expands or contracts when interacting with the environment.
An isolated system has a boundary that does not permit mass or energy exchange across it. For a closed system, the boundary permits only energy exchange. If mass as well as energy is exchanged across the boundary, the system is called an open system.
1.2 State of a System
The state of a system is defined by a set of measurable macroscopic parameters. The state can be measured only if the variables defining the state are invariant with respect to time and space within the system; that is, the system is in equilibrium. It is the equilibrium state of a system that is defined by the state variables of a system.
State variables that depend on the mass of the system are called extensive variables, for example, energy and volume. State variables that are independent of the mass are called intensive variables, for example, pressure, density and temperature. The specific value of an extensive property is the extensive property divided by the amount of substance, for example, specific volume , where V is the volume and m is the mass.
1.3 Simple Systems
We shall be dealing mostly with simple systems. A simple system is one which is homogeneous, isotropic and chemically inert. It is sufficiently large in that surface effects can be neglected. In other words, we may define its energy without considering the surface energy due to the boundary separating the system from the environment. The external forces arising from electromagnetic, gravitational and similar environmental effects are also not considered in contributing to the energy of the simple system. So the simple system can generally be defined solely by its energy U, volume V and amount of mass in the system, that is, (U, V, mi) where mi is the mass of the different chemical components “i” in the system.
1.4 Mass, Molecular Mass and Moles in a System
The mass of a system is the number of molecules N contained in the system multiplied by the mass of each of the molecules in it. Since the mass of a molecule is very small, it is measured in terms of the mass of a standard particle that is chosen to have a mass one-twelfth the mass of an isotope of carbon . The mass of the standard particle , known as the atomic mass unit (a.m.u.), is 1.661×10−24 g.
The mass of a molecule of a substance is therefore expressed in units of the standard atomic mass unit m0, namely, mass of the molecule m divided by , that is, . M is called the molecular mass.
As an example, the molecular mass of a hydrogen molecule is given as , where is the mass of the hydrogen molecule and is the mass of the standard particle. It is also spoken of as molecular weight since almost all experiments are carried out in the vicinity of the Earth’s surface where the gravitational constant is the same. We will use the words molecular mass and molecular weight without differentiating between them.
The number of molecules in a macroscopic system is, in general, very large, and we therefore measure it in the unit of mole. A mole is defined as the number of standard particles N0 in 1 g of it, that is, , N0 is called Avogadro number.
The number of the moles of a substance comprising of N molecules is .
We can write the molecular mass as
(1.1)
since = 1 g.
The molecular mass M therefore equals mN0 in unit of grams and is the mass of 1 mole of the substance in grams. Thus, 1 mole of hydrogen has a mass equal to 2 g, and 1 mole of nitrogen is 28 g and so on. Similarly, the number of moles n of a substance of mass m g is m/M.
For a mixture of gases consisting of N different constituents, the mole fraction of the ith constituent in it is
where mole is the number of moles of the ith constituent in it and is the total number of moles in the mixture.
Similarly, if the mass of the ith constituent is mi, the mass concentration of the ith constituent is
The sum of the mole fractions and mass fractions is unity, namely,