Thermodynamics is the branch of physics that studies the effects of changes in temperature, pressure and volume of a physical system (a material, a liquid, a set of bodies, etc.), at a macroscopic level. The root "thermo" means heat and dynamics refers to movement, so thermodynamics studies the movement of heat in a body. Matter is composed of different particles that move in a disorderly manner. Thermodynamics studies this messy movement.
The practical importance lies primarily in the diversity of physical phenomena it describes. Consequently, knowledge of this diversity has resulted in enormous technological productivity.
Study of thermodynamics
The main elements we have to study thermodynamics are:
Entropy Entropy is a magnitude that can be defined for any system. Specifically, entropy defines the disorder in which the internal particles that make up matter move.
Enthalpy Enthalpy is a state function of the physical system considered. Actually, the first law of thermodynamics, depending on the enthalpy, takes the form dQ = dH - Vdp, that is, the amount of heat supplied to a system is used to increase enthalpy and do external work - Vdp.
In thermodynamics, the interactions between various thermodynamic systems are studied and classified, leading to the definition of concepts such as thermodynamic systems and their environment. A thermodynamic system is characterized by its thermodynamic properties, related to each other by the state equations. These can be combined to express internal energy and thermodynamic potentials, useful for determining the equilibrium conditions between systems and spontaneous processes.
With these tools, thermodynamics describes how systems respond to changes in their environment.
Laws of thermodynamics
The principles of thermodynamics were enunciated during the nineteenth century, which regulate thermodynamic transformations, their progress, their limits. Actually, they are real axioms based on the experience on which the whole theory of thermodynamics is based.
Specifically, three basic principles can be distinguished, plus a "zero" principle that defines the temperature and is implicit in the other three.
The zero law of thermodynamics states that when two interacting systems are in thermal equilibrium, they share some properties, which can be measured by giving them a precise numerical value. Consequently, when two systems are in thermal equilibrium with a third, they are in equilibrium with each other and the shared property is temperature.
The first law of thermodynamics states that when a body comes into contact with another relatively colder body, a transformation occurs that leads to a state of equilibrium in which the temperatures of the two bodies are equal.
The first principle is, therefore, a principle of conservation of energy. In each thermal machine, a certain amount of energy is transformed into work: there cannot be a machine that produces work without consuming energy.
In short, the first thermodynamic principle is traditionally affirmed as: The variation of the internal energy of a closed thermodynamic system is equal to the difference between the heat supplied to the system and the work done by the system in the environment.
There are several statements of the second law of thermodynamics, all equivalent, and each of the formulations emphasizes a particular aspect. First, he states that "it is impossible to make a cyclic machine that has the sole result of transferring heat from a cold body to a warm body" (Clausius statement).
On the other hand, it can also be stated, in an equivalent way, that “it is impossible to carry out a transformation whose result is only that of converting heat taken from a single source into mechanical work” (Kelvin's statement).
The third principle of the laws of thermodynamics is closely related to the latter, and in some cases it is considered as a consequence of the latter. In this sense, it can be said that "it is impossible to reach absolute zero with a finite number of transformations" and provides a precise definition of the magnitude called entropy.
The thermal efficiency or efficiency of a thermal machine is a coefficient or dimensionless ratio calculated as the ratio of the energy produced (in an operating cycle) and the energy supplied to the machine (so that it manages to complete the thermodynamic cycle). It is designated with the Greek letter η
Depending on the type of thermal machine, the transfer of these energies will be done in the form of heat, Q, or work, W.
Th is the temperature of the hot reservoir;
Tc is the temperature of the cold reservoir.
In conclusion, the thermal efficiency equation suggests that higher levels of efficiency are obtained with a higher temperature gradient between hot and cold fluids. In practice, the hotter the fluid, the greater the efficiency of the engine.
Applications of thermodynamics
Thermodynamics can be applied to a wide variety of science and engineering topics, such as motors, phase transitions, chemical reactions, transport phenomena, and even black holes.
In short, Thermodynamic results are essential for other fields of physics and chemistry, chemical engineering, aerospace engineering, mechanical engineering, cell biology, biomedical engineering, and materials science to name a few.
Historical evolution of thermodynamics
Initially, technological developments, such as so-called steam machines or thermometers, were carried out empirically. But it wasn't until the 19th century when scientists like Carnot and Joule formalized their results and determined the theoretical causes of their operation.
Actually, thermodynamics began to be studied in order to increase the efficiency of the first steam engines.
Last review: September 20, 2019