LECTURE 1
1.1 Introduction


Thermo: heat
dynamics: force

Energy: Engineers
Properties of matter: Scientists

Energy
- Efficiency
- Environmental benignancy

Although the principles of thermodynamics have been in existence since the creation of the universe, thermodynamics did not emerge as a science until about 1700 when the first attempts to build a steam engine were made in England by T. Savery and T. Newcomen. These engines were very slow and inefficient, but they opened the way for the development of a new science.

The term thermodynamics was first used in a publication by Lord Kelvin in 1849.

The first thermodynamics textbook was written in 1859, by W. Rankine, a professor at the University of Glasgow.

The greatest progress in thermodynamics was made in the early 1900s when it was stripped of all the erroneous theories and developed into a mature science.

Thermodynamics
Approaches
Descriptions
Macroscopic Approach
(Classical Thermodynamics)
- is concerned with the overall behavior of a system.
- no model of the structure of matter at the molecular, atomic, and subatomic levels is directly used.
Microscopic Approach
(Statistical Thermodynamics)
- is concerned directly with the structure of matter.
- characterizes, by statistical means, the average behavior of the particles making up a system of interest and relate this information to the observed macroscopic behavior of the system.

 

1.2 Definitions

System: the subject of the analysis.
Surroundings: everything external to the system.
Boundary: the surface that separates the system from its surroundings.

 

1.2.1 Systems

Types of
Systems
Descriptions
Closed Systems (Control Mass)
- A fixed quantity of matter.
- There can be no transfer of mass across its boundary. But energy, in the form of heat or work, can cross the boundary.
- The volume of a closed system does not have to be fixed.
Open Systems (Control Volumes)

- A fixed volume in space through which mass may flow.
- It usually encloses a device which involves mass flow such as a compressor, turbine, or nozzle.


Examples
Closed Systems
(Control Mass)

Open Systems
(Control Volumes)








1.2.2 Properties


Properties: macroscopic characteristics of a system, to which numerical values can be assigned at a given time without knowledge of history of the system.

Examples: mass, volume, energy, pressure and temperature.

Types of Properties
Descriptions
Examples
Extensive Properties
- Dependent on the size or extent of a system.
- For a quantity, if its value for an overall system is the sum of its values for the parts into which the system is divided.
Mass and Volume
Intensive
Properties
- Independent of the size or extent of a system.
- The values are not additive.
Pressure and Temperature


1.2.3 State


State: the condition of a system as described by its properties.

 

1.2.4 Process


Process: a transformation from one equilibrium state to another.

At a given state, each property has a definite value that can be assigned without knowledge of how the system arrived at that state. Therefore, the change in value of a property as the system is altered from one state to another is determined solely by the two end states and is independent of the particular way the change of state occurred. The change is independent of the details, or history, of the process.

A quantity is a property if, and only if, its change in value between two states is independent of the process.

 

1.2.5 Phase

Phase: a quantity of matter that is homogeneous throughout in both chemical composition and physical structure.

Homogeneity in physical structure means that the matter is all solid, all liquid, or all vapor (gas).

A system can contain one or more phases.

Examples:
water and vapor, water and oil (2 phases)
water and alcohol, oxygen and nitrogen (1 phase)

1.2.6 Pure Substance

 

Pure substance:one that is uniform and invariable in chemical composition.

A pure substance can exist in more than one phase.

A uniform mixture of gases can be regarded as a pure substance provided it remains a gas and does not react chemically.


Example of Pure Substance (Water)
in Two Phases (Solid and Liquid)

 

1.2.7 Equilibrium


Equilibrium: a state of balance.
In an equilibrium state there are no unbalanced potentials (or driving forces) within the system. A system which is in equilibrium experiences no changes when it is isolated from its surroundings.

There are many types of equilibrium, and a system is not in thermodynamic equilibrium unless the conditions of all the relevant types of equilibrium are satisfied.

Types of Equilibrium
Descriptions
Thermal Equilibrium
- The system involves no temperature differentials, which is the driving force for heat flow.
Mechanical Equilibrium
- No change in pressure at any point in the system with time.
-The pressure may vary within the system with elevation as a result of gravitational effect.
Phase Equilibrium
- If the mass of each phase reaches an equilibrium level and stays there.
Chemical Equilibrium
- If chemical composition does not change with time, i.e., no chemical reactions occur.

 

1.2.8 Process Path

Process Path : the series of equilibrium states through which a system passes during a process.

To describe a process completely, one should specify the initial and final states of the process, as well as the path it follows, and the interactions with the surroundings.


1.2.9 Quasi-Equilibrium

Quasi-Equilibrium : When a process proceeds in such a manner that the system remains infinitesimally close to an equilibrium state at all times, it is called a quasi-equilibrium process.

A quasi-equilibrium process can be viewed as a sufficiently slow process which allows the system to adjust itself internally so that properties in one part of the system do not change any faster than those at other parts.


An example of quasi-equilibrium process is shown in the above animation.


For non-quasi-equilibrium process, we are not able to specify the states through which the system passes during the process and so we cannot speak of a process path.

A quasi-equilibrium process is an idealized process and is not a true representation of an actual process. But many actual processes closely approximate it, and they can be modeled as quasi-equilibrium with negligible errors.

Reasons for using quasi-equilibrium approximation

1. Easy to analyze
2. Work-producing devices deliver the most work when they operates on quasi-equilibrium processes. Therefore, quasi-equilibrium processes serve as standards to which actual processes can be compared.

 

1.2.10 Steady State


Steady state: properties of the system does not change with time.

 

1.2.11 Cycle


Cycle: a sequence of processes that begins and ends at the same state.