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ECE - Thermodynamics

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DarkMagician637_ECE

 

THERMODYNAMICS

In science, thermodynamics (from the Greek θέρμη therme, meaning "heat" and δύναμις, dynamis, meaning force) is the study of energy conversion between heat and mechanical work, and subsequently the macroscopic variables such as temperature, volume and pressure. The first to give a concise definition of the subject was Scottish physicist William Thomson who in 1854 stated that:

Thermo-dynamics is the subject of the relation of heat to forces acting between contiguous parts of bodies, and the relation of heat to electrical agency.”

Two derivatives of thermodynamics to emerge in the decades to follow include: statistical thermodynamics (or statistical mechanics) (1860), a subject concerned with statistical predictions of the collective motion of particles from their microscopic behavior, and chemical thermodynamics (1873), a subject concerned with the nature of the role of entropy in the process of chemical reaction. Historically, thermodynamics developed out of a need to increase the efficiency of early steam engines, particularly through the work of French physicist Nicolas Léonard Sadi Carnot (1824) who believed that engine efficiency was the key that could help France win the Napoleonic Wars.



History of thermodynamics
Laws of thermodynamics

Thermodynamic:

  • Boundary
    Boundary (thermodynamic)
    In thermodynamics, a boundary is a real or imaginary volumetric demarcation region drawn around a thermodynamic system across which quantities such as heat, mass, or work can flow. In short, a thermodynamic boundary is a division between a system and its surroundings. A boundary may be adiabatic,...

  • Component
  • Conjugate variables
    • Temperature / Entropy
      Entropy
      Entropy is a concept of information maintaining great importance in physics, chemistry, and information theory...

    • Pressure / Volume
      Volume
      The volume of any solid, liquid, gas, plasma, theoretical object, or vacuum is how much three-dimensional space it occupies, often quantified numerically. One-dimensional figures and two-dimensional shapes are assigned zero volume in the three-dimensional space...

    • (Stress / Strain)
    • Chemical potential / Particle number
      Particle number
      The particle number, N, is the number of constituent particles in a thermodynamical system. The particle number is a fundamental parameter in thermodynamics and it is conjugate to the chemical potential....

  • Constant:
    • Avogadro's NA
    • Boltzmann k
    • Ideal gas
      Gas constant
      The gas constant is a physical constant which is featured in a large number of fundamental equations in the physical sciences, such as the ideal gas law and the Nernst equation...

       R
    • Stefan-Boltzmann σ
  • Critical line
    Critical line (thermodynamics)
    In thermodynamics, a critical line is the higher-dimensional equivalent of a critical point . It is thelocus of contiguous critical points in a phase diagram. These lines cannot occur for...

  • Cycle
    Thermodynamic cycle
    A thermodynamic cycle is a series of thermodynamic processes transferring heat and work, while varying pressure, temperature, and other state variables, eventually returning a system to its initial state. State Properties depend only on the thermodynamic state and cumulative variation of such...

    • External combustion engine
    • Internal combustion engine
    • Atkinson
      Atkinson cycle
      The Atkinson-cycle engine is a type of internal combustion engine invented by James Atkinson in 1882. The Atkinson cycle is designed to provide efficiency at the expense of power density and is beginning to see use in modern hybrid electric applications....

    • Bell Coleman
    • Brayton
      Brayton cycle
      The Brayton cycle is a thermodynamic cycle that describes the workings of the gas turbine engine, basis of the jet engine and others. It is named after George Brayton , the American engineer who developed it, although it was originally proposed and patented by Englishman John Barber in 1791. It is...

    • Carnot
      Carnot cycle
      Every thermodynamic system exists in a particular state. When a system is taken through a series of different states and finally returned to its initial state, a thermodynamic cycle is said to have occurred. In the process of going through this cycle, the system may perform work on its...

    • Combined
      Combined cycle
      A combined cycle is characteristic of a power producing engine or plant that employs more than one thermodynamic cycle. Heat engines are only able to use a portion of the energy their fuel generates . The remaining heat from combustion is generally wasted...

    • Diesel
      Diesel cycle
      The Diesel cycle is the thermodynamic cycle which approximates the pressure and volume of the combustion chamber of the Diesel engine, invented by Rudolph Diesel in 1897. It is assumed to have constant pressure during the first part of the "combustion" phase , v2 to v3 in the diagram...

    • Ericsson
      Ericsson cycle
      The Ericsson cycle is named after inventor John Ericsson, who designed and built many unique heat engines based on various thermodynamic cycles. He is credited with inventing two unique heat engine cycles and developing practical engines based on these cycles...

    • Hampson-Linde
      Hampson-Linde cycle
      The Hampson-Linde cycle is based on the Joule-Thomson effectand is used in the liquefaction of gases. W. Hampson and Carl von Linde independently filed for patent of the cycle in 1895.-External links:*...

    • Heat engine
      Heat engine
      A heat engine is a physical or theoretical device that converts thermal energy to mechanical output. The mechanical output is called work, and the thermal energy input is called heat. Heat engines typically run on a specific thermodynamic cycle...

      • Carnot
        Carnot heat engine
        A Carnot heat engine is a hypothetical engine that operates on the reversible Carnot cycle. The basic model for this engine was developed by Nicolas Léonard Sadi Carnot in 1824...

    • HEHC
      High-Efficiency Hybrid Cycle
      The High-Efficiency Hybrid Cycle is a new 4-stroke thermodynamic cycle combining elements of the Otto cycle, Diesel cycle, Atkinson cycle and Rankine cycle.-High-Efficiency Hybrid Cycle Engines:...

    • Hot air engine
      Hot air engine
      Hot air engine is a catch-all term for any heat engine which uses the expansion and contraction of air under the influence of a temperature change to convert thermal energy into mechanical work...

    • Heat pump & refrigeration
      Heat pump and refrigeration cycle
      Thermodynamic heat pump and refrigeration cycles are the models for heat pumps and refrigerators. The difference between a heat pump and a normal air conditioner is that a heat pump can be used to heat a home as well as cool it. Even though the heat pump can heat, it still uses the same basic...

    • Kalina
      Kalina cycle
      The Kalina cycle is a thermodynamic cycle for converting thermal energy to mechanical power, optimized for use with thermal sources which are at a relatively low temperature compared to the heat sink temperature...

    • Kleemenko
      Kleemenko cycle
      The Kleemenko cycle or one-flow cascade cycle is a single-stream mixed-refrigerant technique used to cool or liquify gases. The term Kleemenko Cycle is used in refrigeration if multi-component refrigerants are used in a cycle....

    • Lenoir
      Lenoir cycle
      The Lenoir cycle is an idealized thermodynamic cycle often used to model a pulse jet engine. It is based on the operation of an engine patented by Jean Joseph Etienne Lenoir in 1860. This engine is often thought of as the first commercially produced internal combustion engine...

    • Miller
      Miller cycle
      In engineering, the Miller cycle is a combustion process used in a type of four-stroke internal combustion engine. The Miller cycle was patented by Ralph Miller , an American engineer, in the 1940s.- Overview :...

    • Mixed/Dual
      Mixed/Dual Cycle
      Dual Combustion Cycle is a thermal cycle that is a combination of the Otto cycle and the Diesel cycle. Heat is added partly at constant volume and partly at constant pressure, the advantage of which is that more time is available for the fuel to completely combust...

    • Otto
    • Rankine
      Rankine cycle
      The Rankine cycle is a thermodynamic cycle which converts heat into work. The heat is supplied externally to a closed loop, which usually uses water as the working fluid. This cycle generates about 80% of all electric power used throughout the world, including virtually all solar thermal, biomass,...

    • Regenerative
      Regenerative cooling
      Regenerative cooling in rockets is where some or all of the propellant is passed through tubes, channels or otherwise in a jacket around the combustion chamber or nozzle to cool the engine because the fuel in particular and sometimes the oxidizer are good coolants...

    • Siemens
      Siemens cycle
      The Siemens cycle is a technique used to cool or liquefy gases.. A gas is compressed, leading to an increase in its temperature . The compressed gas is then cooled by a heat exchanger, then the cool, compressed gas is allowed to decompress, further cooling it...

    • Stirling
      Stirling cycle
      The Stirling cycle is a thermodynamic cycle that describes the general class of Stirling devices. This includes the original Stirling engine that was invented, developed and patented in 1816 by Reverend Dr...

    • Stoddard
      Stoddard engine
      Elliott J. Stoddard invented and patented two versions of the Stoddard engine, the first in 1919 and the second in 1933. The general engine classification is an external combustion engine with valves and single-phase gaseous working fluid...

  • Ensemble
    Statistical ensemble (mathematical physics)
    In mathematical physics, especially as introduced into statistical mechanics and thermodynamics by J. Willard Gibbs in 1878, an ensemble is an idealization consisting of a large number of mental copies of a system, considered all at once, each of which represents a possible state that the real...

    • Canonical
      Canonical ensemble
      A canonical ensemble in statistical mechanics is a statistical ensemble representing a probability distribution of microscopic states of the system...

    • Grand canonical
      Grand canonical ensemble
      In statistical mechanics, a grand canonical ensemble is an imaginary collection of model systems put together to mirror the calculated probability distribution of microscopic states of a given physical system which is being maintained in a given macroscopic state...

    • Isoenthalpic-isobaric
    • Isothermal-isobaric
    • Microcanonical
      Microcanonical ensemble
      In statistical physics, the microcanonical ensemble is a theoretical tool used to describe the thermodynamic properties of an isolated system. In such a system, the possible states of the system all have the same energy and the probability for the system to be in any given state is the same.-...

  • Equations
    Thermodynamic equations
    In thermodynamics, there are a large number of equations relating the variousthermodynamic quantities. In chemical thermodynamics, which is a sub-branch of thermodynamics, for example, there are millions of useful equations. In particular, the structure of chemical thermodynamics is based on the...

    • Boltzmann
      Boltzmann equation
      The Boltzmann equation, also often known as the Boltzmann transport equation, devised by Ludwig Boltzmann, describes the statistical distribution of one particle in a fluid...

    • Bridgman
      Bridgman's thermodynamic equations
      In thermodynamics, Bridgman's thermodynamic equations are a basic set of thermodynamic equations, derived using a method of generating a large number of thermodynamic identities involving a number of thermodynamic quantities. The equations are named after the American physicist Percy Williams...

    • Churchill-Bernstein
    • Clausius-Clapeyron relation
    • Debye-Hückel
    • Equation of state
      Equation of state
      In physics and thermodynamics, an equation of state is a relation between state variables. More specifically, an equation of state is a thermodynamic equation describing the state of matter under a given set of physical conditions...

    • Exact differential
      Exact differential
      A mathematical differential dQ is said to be exact, as contrasted with an inexact differential, if the differentiable function Q exists. However, if dQ is chosen arbitrarily, a corresponding Q might not exist.-Overview:...

    • Gibbs-Duhem
      Gibbs-Duhem equation
      The Gibbs-Duhem equation in thermodynamics describes the relationship between changes in chemical potential for components in a thermodynamical system :...

    • Gibbs-Helmholtz
      Gibbs-Helmholtz equation
      The Gibbs–Helmholtz equation is a thermodynamic equation useful for calculating changes in the Gibbs energy of a system as a function of temperature. It is named after Josiah Willard Gibbs and Hermann von Helmholtz:With:...

    • Green-Kubo relations
      Green-Kubo relations
      Green–Kubo relations give exact mathematical expression for transport coefficients in terms of integrals of time correlation functions.-Thermal and mechanical transport processes:...

    • Maxwell relations
      Maxwell relations
      Maxwell's relations are a set of equations in thermodynamics which are derivable from the definitions of the thermodynamic potentials. The Maxwell relations are statements of equality among the second derivatives of the thermodynamic potentials. They follow directly from the fact that the order of...

    • Onsager reciprocal relations

  • Equilibrium
    Thermodynamic equilibrium
    In thermodynamics, a thermodynamic system is said to be in thermodynamic equilibrium when it is in thermal equilibrium, mechanical equilibrium, radiative equilibrium, and chemical equilibrium. Classical thermodynamics deals with dynamic equilibrium states...

    • Chemical
      Chemical equilibrium
      In a chemical process, chemical equilibrium is the state in which the chemical activities or concentrations of the reactants and products have no net change over time. Usually, this would be the state that results when the forward chemical process proceeds at the same rate as their reverse reaction...

    • Dynamic
      Dynamic equilibrium
      A system in dynamic equilibrium is a particular example of a system in a steady state. In a steady state the rate of inputs is equal to the rate of outputs so that the composition of the system is unchanging in time...

    • Local
    • Phase
      Gibbs' phase rule
      Gibbs' phase rule, was proposed by Josiah Willard Gibbs in the 1870s as the equalitywhere P is the number of phases in thermodynamic equilibrium with each other and C is the number of components. Typical phases are solids, liquids and gases. A system involving one pure chemical is an example of a...

  • History
    History of thermodynamics
    The history of thermodynamics is a fundamental strand in the history of physics, the history of chemistry, and the history of science in general...

  • Instruments
    Thermodynamic instruments
    A thermodynamic instrument is any device which facilitates the quantitative measurement of thermodynamic systems. In order for a thermodynamic parameter to be truly defined, a technique for its measurement must be specified. For example, the ultimate definition of temperature is "what a thermometer...

    • Barometer
      Barometer
      A barometer is an instrument used to measure atmospheric pressure. It can measure the pressure exerted by the atmosphere by using water, air, or mercury. Pressure tendency can forecast short term changes in the weather...

    • Calorimeter
      Calorimeter
      A calorimeter is a device used for calorimetry, the science of measuring the heat of chemical reactions or physical changes as well as heat capacity. The word calorimeter is derived from the Latin word calor, meaning heat. Differential scanning calorimeters, isothermal microcalorimeters, titration...

    • Dynamometer
      Dynamometer
      A dynamometer or "dyno" for short, is a device for measuring force or power. For example, the power produced by an engine, motor or other rotating prime mover can be calculated by simultaneously measuring torque and rotational speed ....

    • Thermometer
      Thermometer
      A thermometer is a device that measures temperature or temperature gradient using a variety of different principles. A thermometer has two important elements: the temperature sensor A thermometer (from the Greek θερμός (thermo) meaning "warm" and meter, "to measure") is a device that measures...

  • Laws
    Laws of thermodynamics
    The laws of thermodynamics, in principle, describe the specifics for the transport of heat and work in thermodynamic processes. Since their inception, however, these laws have become some of the most important in all of physics and other types of science associated with thermodynamics.It is wise to...

    :
    • Zeroth
      Zeroth law of thermodynamics
      The zeroth law of thermodynamics is a generalization about the thermal equilibrium among bodies, or thermodynamic systems, in contact. It results from the definition and properties of temperature.It can be stated as:...

    • First
      First law of thermodynamics
      The first law of thermodynamics, an expression of the principle of conservation of energy, states that energy can be transformed , but cannot be created or destroyed. Alternatively:-Description:...

    • Second
      Second law of thermodynamics
      The second law of thermodynamics is an expression of the universal principle of entropy, stating that the entropy of an isolated system which is not in equilibrium will tend to increase over time, approaching a maximum value at equilibrium, and that the entropy change dS of a system undergoing any...

    • Third
      Third law of thermodynamics
      The third law of thermodynamics is a statistical law of nature regarding entropy and the impossibility of reaching absolute zero of temperature...

    • Charles's
      Charles's law
      Charles's law is an experimental gas law which describes how gases tend to expand when heated. It was first published by French natural philosopher Joseph Louis Gay-Lussac in 1802, although he credits the discovery to unpublished work from the 1780s by Jacques Charles...

    • Dulong-Petit
    • Fundamental relation
    • Gas laws
      Gas laws
      This article outlines the historical development of the laws describing ideal gases. For a detailed description of the ideal gas laws and their further development, see Ideal gas, Ideal gas law and Gas...

      • Ideal gas
        Ideal gas law
        The Ideal gas law is the equation of state of a hypothetical ideal gas. It is a good approximation to the behaviour of many gases under many conditions, although it has several limitations. It was first stated by Émile Clapeyron in 1834 as a combination of Boyle's law and Charles's law...

    • Joule's
    • Onsager reciprocal relations
    • Stefan-Boltzmann
      Stefan-Boltzmann law
      The Stefan–Boltzmann law, also known as Stefan's law, states that the total energy radiated per unit surface area of a black body in unit time , j*, is directly proportional to the fourth power of the black body's thermodynamic temperature...

  • Limit
    Thermodynamic limit
    In physics and physical chemistry, the thermodynamic limit is reached as the number of particles in a system, N, approaches infinity — or in practical terms, one mole or Avogadro's number ≈ 6 x 1023...

  • Material properties
    Material properties (thermodynamics)
    The thermodynamic properties of materials are intensive thermodynamic parameters which are specific to a given material. Each is directly related to a second order differential of a thermodynamic potential...

    • Bulk modulus
      Bulk modulus
      The bulk modulus of a substance measures the substance's resistance to uniform compression. It is defined as the pressure increase needed to cause a given relative decrease in volume. Its base unit is Pascal....

       K
    • Compressibility
      Compressibility
      In thermodynamics and fluid mechanics, compressibility is a measure of the relative volume change of a fluid or solid as a response to a pressure change.where V is volume and p is pressure...

       β
    • Specific heat capacity
      Specific heat capacity
      Specific heat capacity, often shortened to specific heat, is the measure of the heat energy required to increase the temperature of a of a substance by unit degree. The term originated primarily through the work of 18th-century physicist Joseph Black who conducted various heat measurements and...

       c
    • Thermal expansion
      Thermal expansion
      Thermal expansion is the tendency of a matter to change in volume in response to a change in temperature. When a substance is heated, its particles begin moving and become active thus maintaining a greater average separation. Materials which contract with increasing temperature are rare; this...

       α
  • Potential
    • Internal energy
      Internal energy
      In thermodynamics, the internal energy of a thermodynamic system, or a body with well-defined boundaries, denoted by U, or sometimes E, is the total of the kinetic energy due to the motion of molecules and the potential energy associated with the vibrational and electric energy of atoms...

    • Entropy
      Entropy
      Entropy is a concept of information maintaining great importance in physics, chemistry, and information theory...

    • Gibbs free energy
      Gibbs free energy
      In thermodynamics, the Gibbs free energy is a thermodynamic potential that measures the "useful" or process-initiating work obtainable from an isothermal, isobaric thermodynamic system...

    • Grand
      Grand potential
      The grand potential is a quantity used in statistical mechanics, especially for irreversible processes in open systems.Grand potential is defined by...

    • Helmholtz free energy
      Helmholtz free energy
      In thermodynamics, the Helmholtz free energy is a thermodynamic potential which measures the “useful” work obtainable from a closed thermodynamic system at a constant temperature and volume...

  • Process
    • Adiabatic
      Adiabatic process
      In thermodynamics, an adiabatic process or an isocaloric process is a thermodynamic process in which no heat is transferred to or from the working fluid. The term "adiabatic" literally means impassable, coming from the Greek roots ἀ- , διὰ- , and βαῖνειν ; this etymology corresponds here to an...

    • Isenthalpic
      Isenthalpic process
      An isenthalpic process or isoenthalpic process is a process that proceeds without any change in enthalpy, H; or specific enthalpy, h....

    • Isentropic
      Isentropic process
      In thermodynamics, an isentropic process or isoentropic process is one during which the entropy of the system remains constant...

    • Isobaric
      Isobaric process
      An isobaric process is a thermodynamic process in which the pressure stays constant: The term derives from the Greek isos, meaning "equal," and barus, "heavy." The heat transferred to the system does work but also changes the internal energy of the system:According to the first law of...

    • Isochoric
      Isochoric process
      An isochoric process, also called a constant-volume process, an isovolumetric process, or an isometric process, is a thermodynamic process during which the volume of the closed system undergoing such process remains constant...

    • Isothermal
      Isothermal process
      An isothermal process is a change in which the temperature of the system stays constant: ΔT = 0. This typically occurs when a system is in contact with an outside thermal reservoir , and the change occurs slowly enough to allow the system to continually adjust to the temperature of the...

    • Quasistatic
      Quasistatic process
      In thermodynamics, a quasistatic process is a thermodynamic process that happens infinitely slowly. In practice, such processes can be approximated by performing them "very slowly"....

    • Spontaneous
      Spontaneous process
      A spontaneous process is the time-evolution of a system in which it releases free energy and moves to a lower, more thermodynamically stable, energy state...

    • Steady state
      Steady state
      A system in a steady state has numerous properties that are unchanging in time. The concept of steady state has relevance in many fields, in particular thermodynamics. Steady state is a more general situation than dynamic equilibrium. If a system is in steady state, then the recently observed...

  • State
    Thermodynamic state
    A thermodynamic state is a set of values of properties of a thermodynamic system that must be specified to reproduce the system. The individual parameters are known as state variables, state parameters or thermodynamic variables. Once a sufficient set of thermodynamic variables have been...

    • Excited
      Excited state
      Excitation is an elevation in energy level above an arbitrary baseline energy state. In physics there is a specific technical definition for energy level which is often associated with an atom being excited to an excited state....

    • Function
      State function
      In thermodynamics, a state function, state quantity, or a function of state, is a property of a system that depends only on the current state of the system, not on the way in which the system acquired that state. A state function describes the equilibrium state of a system...

    • Ground
      Stationary state
      In quantum mechanics, a stationary state is an eigenstate of a Hamiltonian, or in other words, a state of definite energy. It is called stationary because the corresponding probability density has no time dependence....

    • Standard
      Standard state
      In chemistry, the standard state of a material is a reference point used to calculate its properties under different conditions. In principle, the choice of standard state is arbitrary, although the International Union of Pure and Applied Chemistry recommends a conventional set of standard states...

    • Stationary
      Stationary state
      In quantum mechanics, a stationary state is an eigenstate of a Hamiltonian, or in other words, a state of definite energy. It is called stationary because the corresponding probability density has no time dependence....

    • Steady
      Steady state
      A system in a steady state has numerous properties that are unchanging in time. The concept of steady state has relevance in many fields, in particular thermodynamics. Steady state is a more general situation than dynamic equilibrium. If a system is in steady state, then the recently observed...

  • System
    Thermodynamic system
    In thermodynamics, a thermodynamic system, originally called a working substance, is defined as that part of the universe that is under consideration. A hypothetical boundary separates the system from the rest of the universe, which is referred to as the environment, surroundings, or reservoir...

    • Closed
      Closed system
      A closed system is a system in the "state of being isolated from its surrounding environment." The term often refers to an idealized system in which closure is perfect. In reality no system can be completely closed; there are only varying degrees of closure....

    • Dissipative
      Dissipative system
      A dissipative system is a thermodynamically open system which is operating far from thermodynamic equilibrium in an environment with which it exchanges energy and matter.- Overview :...

    • Isolated
      Isolated system
      In the natural sciences an isolated system, as contrasted with a open system, is a physical system that does not interact with its surroundings. It obeys a number of conservation laws: its total energy and mass stay constant. They cannot enter or exit, but can only move around inside...

  • Temperature
    Thermodynamic temperature
    Thermodynamic temperature is the absolute measure of temperature and is one of the principal parameters of thermodynamics. Thermodynamic temperature is an “absolute” scale because it is the measure of the fundamental property underlying temperature: its null or zero point, absolute zero, is the...

    • Negative
      Negative temperature
      In physics, certain systems can achieve negative temperatures; that is, their thermodynamic temperature can be of a negative quantity. Negative temperatures can be expressed as negative numbers on the kelvin scale....

    • Range
      Temperature range
      Temperature range is the numerical difference between the minimum and maximum values of temperature observed in a system, such as atmospheric temperature in a given location.-Atmospheric temperature range:...



Variable:
  • Chemical potential
    Chemical potential
    Chemical potential, symbolized by μ, is a quantity first described by the American engineer, chemist and mathematical physicist Josiah Williard Gibbs...

     μ
  • Density
    Density
    The density of a material is defined as its mass per unit volume. The symbol of density is ρ .- Formula :Mathematically:where: is the density, is the mass, is the volume....

  • Energy
    Energy
    In physics, energy is a scalar physical quantity that describes the amount of work that can be performed by a force, an attribute of objects and systems that is subject to a conservation law...

    • Conservation of
      Conservation of energy
      The law of conservation of energy states that the total amount of energy in a closed system remains constant. A consequence of this law is that energy cannot be created nor destroyed...

    • Conversion efficiency
      Energy conversion efficiency
      Energy conversion efficiency is the ratio between the useful output of an energy conversion machine and the input, in energy terms. The useful output may be electric power, mechanical work, or heat. Energy conversion efficiency is not defined uniquely, but instead depends on the usefulness of the...

    • Electrical
    • Free
      Thermodynamic free energy
      In thermodynamics, the term thermodynamic free energy refers to the amount of work that can be extracted from a system, and is helpful in engineering applications...

    • Gibbs free
      Gibbs free energy
      In thermodynamics, the Gibbs free energy is a thermodynamic potential that measures the "useful" or process-initiating work obtainable from an isothermal, isobaric thermodynamic system...

       G
    • Helmholtz free
      Helmholtz free energy
      In thermodynamics, the Helmholtz free energy is a thermodynamic potential which measures the “useful” work obtainable from a closed thermodynamic system at a constant temperature and volume...

       A
    • Internal
      Internal energy
      In thermodynamics, the internal energy of a thermodynamic system, or a body with well-defined boundaries, denoted by U, or sometimes E, is the total of the kinetic energy due to the motion of molecules and the potential energy associated with the vibrational and electric energy of atoms...

       U
    • Kinetic
      Kinetic energy
      The kinetic energy of an object is the extra energy which it possesses due to its motion. It is defined as the work needed to accelerate a body of a given mass from rest to its current velocity. Having gained this energy during its acceleration, the body maintains this kinetic energy unless its...

    • Potential
      Potential energy
      Potential energy is energy stored within a physical system as a result of the position or configuration of the different parts of that system. It is called potential energy because it has the potential to be converted into other forms of energy, such as kinetic energy, and to do work in the process...

    • Specific
      Specific energy
      Specific energy is defined as the energy per unit mass. Common metric units are J/kg or, in basic SI units: m2/s2. It is an intensive property. Contrast this with energy, which is an extensive property. There are two main types of specific energy: field strength and strength...

  • Enthalpy
    Enthalpy
    In thermodynamics and molecular chemistry, the enthalpy is a thermodynamic property of a thermodynamic system. It can be used to calculate the heat transfer during a quasistatic process taking place in a closed thermodynamic system under constant pressure...

     H
  • Entropy
    Entropy
    Entropy is a concept of information maintaining great importance in physics, chemistry, and information theory...

     S
    • & information theory
      Entropy in thermodynamics and information theory
      There are close parallels between the mathematical expressions for the thermodynamic entropy, usually denoted by S, of a physical system in the statistical thermodynamics established by Ludwig Boltzmann and J. Willard Gibbs in the 1870s; and the information-theoretic entropy, usually expressed as...

    • As energy dispersal
    • Introduction to
      Introduction to entropy
      In thermodynamics, entropy is a measure of certain aspects of energy in relation to absolute temperature. In thermodynamics, entropy is one of the three basic thermodynamic potentials: U , S and A...

    • Residual
      Residual entropy
      Residual entropy is physically significant entropy, which is present even after a substance is cooled arbitrarily close to absolute zero. That is, if a material is reduced to its ground state, residual entropy occurs if the material can exist in multiple different ground states that have the same...

    • Shannon
    • Statistical
  • Exergy
    Exergy
    In thermodynamics, the exergy of a system is the maximum work possible during a process that brings the system into equilibrium with a heat reservoir. When the surroundings are the reservoir, exergy is the potential of a system to cause a change as it achieves equilibrium with its environment. ...

    • Efficiency
      Exergy efficiency
      Exergy efficiency computes the efficiency of a process taking the second law of thermodynamics into account.-Motivation:...

  • Mass
    Mass
    In physics, mass commonly refers to any of three properties of matter, which have been shown experimentally to be equivalent: inertial mass, active gravitational mass and passive gravitational mass...

  • Mole (unit)
    Mole (unit)
    The mole is a unit of amount of substance: it is an SI base unit, and one of the few units used to measure this physical quantity. The name "mole" was coined in German by Wilhelm Ostwald in 1893, although the related concept of equivalent mass had been in use at least a century earlier...

  • Particle number
    Particle number
    The particle number, N, is the number of constituent particles in a thermodynamical system. The particle number is a fundamental parameter in thermodynamics and it is conjugate to the chemical potential....

     N
  • Pressure
    Pressure
    Pressure is the force per unit area applied in a direction perpendicular to the surface of an object. Gauge pressure is the pressure relative to the local atmospheric or ambient pressure.- Definition :...

     P
  • Temperature
    Thermodynamic temperature
    Thermodynamic temperature is the absolute measure of temperature and is one of the principal parameters of thermodynamics. Thermodynamic temperature is an “absolute” scale because it is the measure of the fundamental property underlying temperature: its null or zero point, absolute zero, is the...

     T
  • Volume
    Volume
    The volume of any solid, liquid, gas, plasma, theoretical object, or vacuum is how much three-dimensional space it occupies, often quantified numerically. One-dimensional figures and two-dimensional shapes are assigned zero volume in the three-dimensional space...

     V
  • Work
    Work (thermodynamics)
    In thermodynamics, work performed by a system is the quantity of energy transferred by the system to another due to changes in the external parameters of the system. If these changes happen in a reversible way, then the performed work does not lead to a change of the entropy. It is a...

     W
    • Mechanical
      Mechanical work
      In physics, mechanical work is the amount of energy transferred by a force acting through a distance. Like energy, it is a scalar quantity, with SI units of joules...



Theorem:
  • Carnot's
  • Clausius
    Clausius theorem
    The Clausius theorem states that in a cyclic processThe equality holds in the reversible case and the '<' is in the irreversible case. The reversible case is used to introduce the function state entropy...

  • Equipartition
    Equipartition theorem
    In classical statistical mechanics, the equipartition theorem is a general formula that relates the temperature of a system with its average energies. The equipartition theorem is also known as the law of equipartition, equipartition of energy, or simply equipartition...

  • Bolzmann's H
    H-theorem
    In thermodynamics, the H-theorem, introduced by Ludwig Boltzmann in 1872, describes the increase in the entropy of an ideal gas in an irreversible process, by considering the Boltzmann equation....

  • Nernst heat
    Nernst heat theorem
    The Nernst heat theorem was formulated by Walther Nernst early in the twentieth century and was used in the development of the third law of thermodynamics.- The theorem :...

  • Virial
    Virial theorem
    In mechanics, the virial theorem provides a general equation relating the average over time of the total kinetic energy, , of a stable system, bound by potential forces, with that of the total potential energy, , where angle brackets represent the average over time of the enclosed quantity...


Other Related Topics
Heat
Heat
In physics and thermodynamics, heat is the process of energy transfer from one body or system due to thermal contact, which in turn is defined as an energy transfer to a body in any other way than due to work performed on the body....

:
  • Critical heat flux
    Critical heat flux
    Critical heat flux describes the thermal limit of a phenomenon where a phase change occurs during heating , which suddenly decreases the efficiency of heat transfer, thus causing localised overheating of the heating surface.The Critical heat flux for ignition is the lowest thermal load per unit...

  • Heat of combustion
    Heat of combustion
    The heat of combustion is the energy released as heat when one mole of a compound undergoes complete combustion with oxygen. The chemical reaction is typically a hydrocarbon reacting with oxygen to form carbon dioxide, water and heat...

  • Heat transfer
    Heat transfer
    Heat transfer is the transition of thermal energy from a hotter object to a cooler object...

    • Convective
  • Latent heat
    Latent heat
    The expression latent heat refers to the amount of energy released or absorbed by a chemical substance during a change of state that occurs without changing its temperature, meaning a phase transition such as the melting of ice or the boiling of water...

  • Mechanical equivalent
    Mechanical equivalent of heat
    In the history of science, the mechanical equivalent of heat was a concept that had an important part in the development and acceptance of the conservation of energy and the establishment of the science of thermodynamics in the 19th century....

  • Theory of heat
    Theory of heat
    In the history of science, the theory of heat or mechanical theory of heat was a theory, introduced predominantly in 1824 by the French physicist Sadi Carnot, that heat and mechanical work are equivalent. It is related to the mechanical equivalent of heat...

  • Volumetric heat capacity
    Volumetric heat capacity
    Volumetric heat capacity describes the ability of a given volume of a substance to store internal energy while undergoing a given temperature change, but without undergoing a phase change. It is different from specific heat capacity in that the VHC depends on the volume of the material, while the...



Thermal:
  • Analysis
    Thermal analysis
    Thermal analysis is a branch of materials science where the properties of materials are studied as they change with temperature. Several methods are commonly used - these are distinguished from one another by the property which is measured:...

  • Conductivity
    Thermal conductivity
    In physics, thermal conductivity, , is the property of a material that indicates its ability to conduct heat. It appears primarily in Fourier's Law for heat conduction.-Measurement:...

  • Contact
    Thermal contact
    In heat transfer and thermodynamics, a thermodynamic system is said to be in thermal contact with another system if it can exchange energy with it through the process of heat. Perfect thermal isolation is an idealization as real systems are always in thermal contact with their environment to some...

  • Efficiency
    Thermal efficiency
    In thermodynamics, the thermal efficiency is a dimensionless performance measure of a thermal device such as an internal combustion engine, a boiler, or a furnace, for example. The input, , to the device is heat, or the heat-content of a fuel that is consumed. The desired output is mechanical...

  • Energy
  • Equilibrium
  • Expansion
    Thermal expansion
    Thermal expansion is the tendency of a matter to change in volume in response to a change in temperature. When a substance is heated, its particles begin moving and become active thus maintaining a greater average separation. Materials which contract with increasing temperature are rare; this...

    • Negative
      Negative thermal expansion
      Negative Thermal Expansion is a physicochemical process in which some materials contract upon heating rather than expanding as most materials do. Materials which undergo this unusual process have a range of potential engineering, photonic, electronic, and structural applications...

  • Mass
    Thermal mass
    Thermal mass is the capacity of a body to store heat. It is typically measured in units of J/°C or J/K . If the body consists of a homogeneous material with sufficiently known physical properties, the thermal mass is simply the amount of material present times the specific heat capacity of that...

  • Motion
  • Radiation
    Thermal radiation
    Thermal radiation is electromagnetic radiation emitted from the surface of an object which is due to the object's temperature. An example of thermal radiation is the infrared radiation emitted by a common household radiator or electric heater. A person near a raging bonfire will feel the radiated...

  • Science
    Thermal science
    Thermal science is the combined study of thermodynamics, fluid mechanics, heat transfer, and combustion. This umbrella-subject is typically designed for non-engineering students and functions to provide a general introduction to each of three core heat-related subjects.-Overview:Introductory...


Physical chemistry
Physical chemistry
Physical chemistry is the explanation of macroscopic, microscopic, atomic, subatomic, and particulate phenomena in chemical systems in terms of physical concepts; sometimes using the principles, practices and concepts of physics like thermodynamics, quantum chemistry, statistical mechanics and...

:
  • Autocatalytic reactions and order creation
  • Boiling point
    Boiling point
    The boiling point of an element or a substance is the temperature at which the vapor pressure of the liquid equals the environmental pressure surrounding the liquid....

  • Calorimetry
    Calorimetry
    Calorimetry is the science of measuring the heat of chemical...

  • Chemical energetics
  • Chemical kinetics
    Chemical kinetics
    Chemical kinetics, also known as reaction kinetics, is the study of rates of chemical processes. Chemical kinetics includes investigations of how different experimental conditions can influence the speed of a chemical reaction and yield information about the reaction's mechanism and transition...

  • Endergonic reaction
    Endergonic reaction
    In chemical thermodynamics, an endergonic reaction is a chemical reaction in which the standard change in free energy is positive, and energy is absorbed...

  • Endothermic
    Endothermic
    In thermodynamics, the word endothermic "within-heating" describes a process or reaction that absorbs energy in the form of heat. Its etymology stems from the Greek prefix endo-, meaning “inside” and the Greek suffix –thermic, meaning “to heat”. The opposite of an endothermic process is an...

  • Exothermic
    Exothermic
    In thermodynamics, the term exothermic describes a process or reaction that releases energy usually in the form of heat, but also in the form of light , electricity , or sound. Its etymology stems from the Greek prefix ex- and the Greek word thermein...

  • Gibbs phase rule
  • Melting point
    Melting point
    The melting point of a solid is the temperature range at which it changes state from solid to liquid. At the melting point the solid and liquid phase exist in equilibrium. When considered as the temperature of the reverse change from liquid to solid, it is referred to as the freezing point...

  • Phase diagram
    Phase diagram
    A phase diagram in physical chemistry, engineering, mineralogy, and materials science is a type of chart used to show conditions at which thermodynamically-distinct phases can occur at equilibrium...

    • Calphad
  • Phase transition
    Phase transition
    A phase transition is a natural physical process. It has the characteristic of taking a given medium with given properties and transforming some or all of that medium, into a new medium with new properties. Phase transitions occur frequently and are found everywhere in the natural world...

  • Thermodynamic databases for pure substances
    Thermodynamic databases for pure substances
    Thermodynamic databases contain information about thermodynamic properties for substances, the most important being enthalpy, entropy, and Gibbs free energy. Numerical values of these thermodynamic properties are collected as tables or are calculated from thermodynamic datafiles...

  • Triple point
    Triple point
    In thermodynamics, the triple point of a substance is the temperature and pressure at which three phases of that substance coexist in thermodynamic equilibrium...

  • Vapor-liquid equilibrium
    Vapor-liquid equilibrium
    Vapor-liquid equilibrium, abbreviated as VLE by some, is a condition where a liquid and its vapor are in equilibrium with each other, a condition or state where the rate of evaporation equals the rate of condensation on a molecular level such that there is no net vapor-liquid interconversion...



Statistical Mechanics
Statistical mechanics
Statistical mechanics is the application of probability theory, which includes mathematical tools for dealing with large populations, to the field of mechanics, which is concerned with the motion of particles or objects when subjected to a force...

:
  • Boltzmann distribution
    Boltzmann distribution
    In physics and mathematics, the Boltzmann distribution is a certain distribution function or probability measure for the distribution of the states of a system. It underpins the concept of the canonical ensemble, providing its underlying distribution...

  • Boltzmann distribution law
  • Boltzmann factor
    Boltzmann factor
    In physics, the Boltzmann factor is a weighting factor that determines the relative probability of a state in a multi-state system in thermodynamic equilibrium at temperature .Where is Boltzmann's constant, and is the energy of state...

  • Bose-Einstein condensate
  • Bose-Einstein statistics
  • Brownian motion
    Brownian motion
    Brownian motion is the seemingly random movement of particles suspended in a fluid or the mathematical model used to describe such random movements, often called a particle theory....

  • Configuration integral
    Configuration integral
    The classical configuration integral, more commonly called the partition function, andsometimes referred to asthe configurational partition function,for a system withparticlesis defined as follows:whereisthe volume enclosing theparticles,...

  • Degeneracy
    Degeneracy
    Degeneracy , from the Latin de-generare "to depart from its kind or genus, to fall from its proper or ancestral quality" can refer to:*In science and mathematics:...

  • Degrees of freedom
    Degrees of freedom
    Degrees of freedom can mean:* Degrees of freedom * Degrees of freedom * Degrees of freedom...

  • Fermi-Dirac statistics
    Fermi-Dirac statistics
    Fermi-Dirac statistics is a part of the science of physics that describes the energies of single particles in a system comprising many identical particles that obey the Pauli Exclusion Principle...

  • Fluctuations
  • Gibbs paradox
    Gibbs paradox
    Originally considered by Josiah Willard Gibbs in his paper On the Equilibrium of Heterogeneous Substances, the Gibbs paradox applies to thermodynamics. It involves the discontinuous nature of the entropy of mixing...

  • Ideal gas
    Ideal gas
    An ideal gas is a theoretical gas composed of a set of randomly-moving point particles that interact only through elastic collisions. The ideal gas concept is useful because it obeys the ideal gas law, a simplified equation of state, and is amenable to analysis under statistical mechanics.At...

  • Irreversibility
    Irreversibility
    In science, a process that is not reversible is called irreversible. This concept arises most frequently in thermodynamics, as applied to processes...

  • Kinetic theory
    Kinetic theory
    Kinetic theory is the theory that gases are made up of a large number of small particles , all of which are in constant, random motion. The rapidly moving particles constantly collide with each other and with the walls of the container...

  • Macrostate
  • Maxwell-Boltzmann statistics
  • Microstate
    Microstate (statistical mechanics)
    In statistical mechanics, a microstate describes a specific detailed microscopic configuration of a thermodynamic system that the system visits in the course of its thermal fluctuations....

  • Molecular chaos
    Molecular chaos
    In kinetic theory in physics, molecular chaos is the assumption that the velocities of colliding particles are uncorrelated, and independent of position...

  • Partition function
    Partition function (statistical mechanics)
    In statistical mechanics, the partition function Z is an important quantity that encodes the statistical properties of a system in thermodynamic equilibrium. It is a function of temperature and other parameters, such as the volume enclosing a gas...



Thermoelectricity
Thermoelectricity
Thermoelectricity refers to a class of phenomena in which a temperature difference creates an electric potential or an electric potential creates a temperature difference. In modern technical usage, the term almost always refers collectively to the Seebeck effect, Peltier effect, and the Thomson...

:
  • Nernst effect
    Nernst effect
    In physics and chemistry, the Nernst Effect is a thermoelectric phenomenon observed when a sample allowing electrical conduction is subjected to a magnetic field and a temperature gradient normal to each other...

  • Peltier effect
  • Seebeck effect
  • Thermionic emission
    Thermionic emission
    Thermionic emission is the heat-induced flow of charge carriers from a surface or over a potential-energy barrier. This occurs because the thermal energy given to the carrier overcomes the forces restraining it. The charge carriers can be electrons or ions, and in older literature are sometimes...

  • Thermoelectric effect
    Thermoelectric effect
    The thermoelectric effect is the direct conversion of temperature differences to electric voltage and vice versa. A thermoelectric device creates a voltage when there is a different temperature on each side. Conversely when a voltage is applied to it, it creates a temperature difference...

  • Thermoelectricity
    Thermoelectricity
    Thermoelectricity refers to a class of phenomena in which a temperature difference creates an electric potential or an electric potential creates a temperature difference. In modern technical usage, the term almost always refers collectively to the Seebeck effect, Peltier effect, and the Thomson...

  • Thermogenerator
    Thermogenerator
    Thermogenerators are devices which convert heat directly into electrical energy. For the most part, this term is synonymous with "thermoelectric generator" and rarely used in English. Essentially they work on the principle of the Seebeck effect, with typical efficiencies of around 5-10%...

  • Thermophotovoltaic
    Thermophotovoltaic
    Thermophotovoltaic energy conversion is a direct conversion process from heat differentials to electricity via photons. A basic thermophotovoltaic system consists of a thermal emitter and a photovoltaic diode cell....

  • Thermopower
    Thermopower
    The thermopower, or thermoelectric power of a material is a measure of the magnitude of an induced thermoelectric voltage in response to a temperature difference across that material...

  • Thomson effect


Sundry:

  • Absolute zero
    Absolute zero
    Absolute zero is a temperature marked by a 0 entropy configuration. It is the coldest temperature theoretically possible and cannot be reached by artificial or natural means, because it is impossible to decouple a system fully from the rest of the universe...

  • Arrow of time
    Arrow of time
    In the natural sciences, arrow of time, or time’s arrow, is a term coined in 1927 by British astronomer Arthur Eddington used to distinguish a direction of time on a four-dimensional relativistic map of the world, which, according to Eddington, can be determined by a study of organizations of...

  • Black body
    Black body
    In physics, a black body is an idealized object that absorbs all electromagnetic radiation that falls on it. No electromagnetic radiation passes through it and none is reflected. Because no light is reflected or transmitted, the object appears black when it is cold. However, a black body emits a...

  • Dissipation
    Dissipation
    In physics, dissipation embodies the concept of a dynamical system where important mechanical modes, such as waves or oscillations, lose energy over time, typically due to the action of friction or turbulence. The lost energy is converted into heat, raising the temperature of the system...

  • Ettingshausen effect
  • Extensive quantity
  • Intensive quantity
  • Legendre transformation
    Legendre transformation
    In mathematics, the Legendre transformation or Legendre transform, named after Adrien-Marie Legendre, is an operation that transforms one real-valued function of a real variable into another...

  • Loschmidt's paradox
    Loschmidt's paradox
    Loschmidt's paradox, also known as the reversibility paradox, is the objection that it should not be possible to deduce an irreversible process from time-symmetric dynamics...

  • Mass-energy equivalence
    Mass-energy equivalence
    In physics, mass–energy equivalence is the concept that the mass of a body is a measure of its energy content. The mass of a body as measured on a scale is always equal to the total energy inside, multiplied by a constant c2 that changes the units appropriately:where E is energy, m is...

  • Physical information
    Physical information
    In physics, physical information refers generally to the information that is contained in a physical system. Its usage in quantum mechanics is important, for example in the concept of quantum entanglement to describe effectively direct or causal relationships between apparently distinct or...

  • Piezoelectric effect
  • Pressure volume diagram
    Pressure volume diagram
    A pressure volume diagram ) is used to describe a thermal cycle involving the following two variables:* Volume * Pressure...

  • Pyroelectric effect
  • Quality of a fluid
    Quality (physics)
    In physics, quality has several different meanings.- Thermodynamics :The quality of a fluid is the percentage of mass that is vapor; i.e. saturated vapor has a "quality" of 100%, and saturated liquid has a "quality" of 0%...

  • Refrigeration
    Refrigeration
    Refrigeration is the process of removing heat from an enclosed space, or from a substance, and moving it to a place where it is unobjectionable. The primary purpose of refrigeration is lowering the temperature of the enclosed space or substance and then maintaining that lower temperature.The term...

    • Gas asbsorption
    • Cycle
      Heat pump and refrigeration cycle
      Thermodynamic heat pump and refrigeration cycles are the models for heat pumps and refrigerators. The difference between a heat pump and a normal air conditioner is that a heat pump can be used to heat a home as well as cool it. Even though the heat pump can heat, it still uses the same basic...

    • Thermoelectric cooling
    • Vapor compression
  • Standard conditions for temperature and pressure
  • Thermodynamic paradox
    Thermodynamic paradox
    The thermodynamic paradox is an argument attempting to use thermodynamics to make deductions about the nature of the universe, specifically it attempts to argue against the steady state model of the universe using reductio ad absurdum....

  • T-symmetry
    T-symmetry
    T Symmetry is the symmetry of physical laws under a time reversal transformation —Although in restricted contexts one may find this symmetry, the observable universe itself does not show symmetry under time reversal, due to the second law of thermodynamics.Hence time asymmetries are generally...

  • Two dimensional gas
SAMPLE PROBLEMS

Timeline of thermodynamics

Before 1800

  • 1650 — Otto von Guericke builds the first vacuum pump
  • 1660 — Robert Boyle experimentally discovers Boyle's Law, relating the pressure and volume of a gas (published 1662)
  • 1665 — Robert Hooke stated: "Heat being nothing else but a very brisk and vehement agitation of the parts of a body."
  • 1669 — J.J. Becher puts forward a theory of combustion involving combustible earth (Latin terra pinguis).
  • 1676–1689 — Gottfried Leibniz develops the concept of vis viva, a limited version of the conservation of energy
  • 1679 — Denis Papin designed a steam digester which inspired the development of the piston-and-cylinder steam engine.
  • 1694–1734 — Georg Ernst Stahl names Becher's combustible earth as phlogiston and develops the theory
  • 1698 — Thomas Savery patented an early steam engine
  • 1702 — Guillaume Amontons introduces the concept of absolute zero, based on observations of gases
  • 1738 — Daniel Bernoulli publishes Hydrodynamica, initiating the kinetic theory
  • 1761 — Joseph Black discovers that ice absorbs heat without changing its temperature when melting
  • 1772 — Black's student Daniel Rutherford discovers nitrogen, which he calls phlogisticated air, and together they explain the results in terms of the phlogiston theory
  • 1776 — John Smeaton publishes a paper on experiments related to power, work, momentum, and kinetic energy, supporting the conservation of energy
  • 1777 — Carl Wilhelm Scheele distinguishes heat transfer by thermal radiation from that by convection and conduction
  • 1783 — Antoine Lavoisier discovers oxygen and develops an explanation for combustion; in his paper "Réflexions sur le phlogistique", he deprecates the phlogiston theory and proposes a caloric theory
  • 1784 — Jan Ingenhousz describes Brownian motion of charcoal particles on water
  • 1791 — Pierre Prévost shows that all bodies radiate heat, no matter how hot or cold they are
  • 1798 — Count Rumford (Benjamin Thompson) performs measurements of the frictional heat generated in boring cannons and develops the idea that heat is a form of kinetic energy; his measurements refute caloric theory, but are imprecise enough to leave room for doubt

1800–1847

  • 1802 — Joseph Louis Gay-Lussac publishes Charles's law, discovered (but unpublished) by Jacques Charles around 1787; this shows the dependency between temperature and volume. Gay-Lussac also formulates the law relating temperature with pressure (the pressure law, or Gay-Lussac's law)
  • 1804 — Sir John Leslie observes that a matte black surface radiates heat more effectively than a polished surface, suggesting the importance of black body radiation
  • 1805 — William Hyde Wollaston defends the conservation of energy in On the Force of Percussion
  • 1808 — John Dalton defends caloric theory in A New System of Chemistry and describes how it combines with matter, especially gases; he proposes that the heat capacity of gases varies inversely with atomic weight
  • 1810 — Sir John Leslie freezes water to ice artificially
  • 1813 — Peter Ewart supports the idea of the conservation of energy in his paper On the measure of moving force; the paper strongly influences Dalton and his pupil, James Joule
  • 1819 — Pierre Louis Dulong and Alexis Thérèse Petit give the Dulong-Petit law for the specific heat capacity of a crystal
  • 1820 — John Herapath develops some ideas in the kinetic theory of gases but mistakenly associates temperature with molecular momentum rather than kinetic energy; his work receives little attention other than from Joule
  • 1822 — Joseph Fourier formally introduces the use of dimensions for physical quantities in his Theorie Analytique de la Chaleur
  • 1822 — Marc Séguin writes to John Herschel supporting the conservation of energy and kinetic theory
  • 1824 — Sadi Carnot analyzes the efficiency of steam engines using caloric theory; he develops the notion of a reversible process and, in postulating that no such thing exists in nature, lays the foundation for the second law of thermodynamics, and initiating the science of thermodynamics
  • 1827 — Robert Brown discovers the Brownian motion of pollen and dye particles in water
  • 1831 — Macedonio Melloni demonstrates that black body radiation can be reflected, refracted, and polarised in the same way as light
  • 1834 — Émile Clapeyron popularises Carnot's work through a graphical and analytic formulation. He also combined Boyle's Law, Charles's Law, and Gay-Lussac's Law to produce a Combined Gas Law. PV/T = k
  • 1841 — Julius Robert von Mayer, an amateur scientist, writes a paper on the conservation of energy, but his lack of academic training leads to its rejection
  • 1842 — Mayer makes a connection between work, heat, and the human metabolism based on his observations of blood made while a ship's surgeon; he calculates the mechanical equivalent of heat
  • 1842 — William Robert Grove demonstrates the thermal dissociation of molecules into their constituent atoms, by showing that steam can be disassociated into oxygen and hydrogen, and the process reversed
  • 1843 — John James Waterston fully expounds the kinetic theory of gases, but is ridiculed and ignored
  • 1843 — James Joule experimentally finds the mechanical equivalent of heat
  • 1845 — Henri Victor Regnault added Avogadro's Law to the Combined Gas Law to produce the Ideal Gas Law. PV = nRT
  • 1846 — Karl-Hermann Knoblauch publishes De calore radiante disquisitiones experimentis quibusdam novis illustratae
  • 1846 — Grove publishes an account of the general theory of the conservation of energy in On The Correlation of Physical Forces
  • 1847 — Hermann von Helmholtz publishes a definitive statement of the conservation of energy, the first law of thermodynamics

1848–1899

  • 1848 — William Thomson extends the concept of absolute zero from gases to all substances
  • 1849 — William John Macquorn Rankine calculates the correct relationship between saturated vapour pressure and temperature using his hypothesis of molecular vortices
  • 1850 — Rankine uses his vortex theory to establish accurate relationships between the temperature, pressure, and density of gases, and expressions for the latent heat of evaporation of a liquid; he accurately predicts the surprising fact that the apparent specific heat of saturated steam will be negative.
  • 1850 — Rudolf Clausius gives the first clear joint statement of the first and second law of thermodynamics, abandoning the caloric theory, but preserving Carnot's principle.
  • 1851 — Thomson gives an alternative statement of the second law.
  • 1852 — Joule and Thomson demonstrate that a rapidly expanding gas cools, later named the Joule–Thomson effect or Joule–Kelvin effect
  • 1854 — Helmholtz puts forward the idea of the heat death of the universe
  • 1854 — Clausius establishes the importance of dQ/T (Clausius's theorem), but does not yet name the quantity.
  • 1854 — Rankine introduces his thermodynamic function, later identified as entropy
  • 1856 — August Krönig publishes an account of the kinetic theory of gases, probably after reading Waterston's work
  • 1857 — Clausius gives a modern and compelling account of the kinetic theory of gases in his On the nature of motion called heat
  • 1859 — James Clerk Maxwell discovers the distribution law of molecular velocities
  • 1859 — Gustav Kirchhoff shows that energy emission from a black body is a function of only temperature and frequency
  • 1862 — "Disgregation," a precursor of entropy, was defined in 1862 by Rudolf Clausius as the magnitude of the degree of separation of molecules of a body
  • 1865 — Clausius introduces the modern macroscopic concept of entropy
  • 1865 — Josef Loschmidt applies Maxwell's theory to estimate the number-density of molecules in gases, given observed gas viscosities.
  • 1867 — Maxwell asks whether Maxwell's demon could reverse irreversible processes
  • 1870 — Clausius proves the scalar virial theorem
  • 1872 — Ludwig Boltzmann states the Boltzmann equation for the temporal development of distribution functions in phase space, and publishes his H-theorem
  • 1874 — Thomson formally states the second law of thermodynamics.
  • 1876 — Josiah Willard Gibbs publishes the first of two papers (the second appears in 1878) which discuss phase equilibria, statistical ensembles, the free energy as the driving force behind chemical reactions, and chemical thermodynamics in general.[citation needed]
  • 1876 — Loschmidt criticises Boltzmann's H theorem as being incompatible with microscopic reversibility (Loschmidt's paradox).
  • 1877 — Boltzmann states the relationship between entropy and probability.
  • 1879 — Jožef Stefan observes that the total radiant flux from a blackbody is proportional to the fourth power of its temperature and states the Stefan–Boltzmann law.
  • 1884 — Boltzmann derives the Stefan–Boltzmann blackbody radiant flux law from thermodynamic considerations.
  • 1888 — Henri-Louis Le Chatelier states his principle that the response of a chemical system perturbed from equilibrium will be to counteract the perturbation.
  • 1889 — Walther Nernst relates the voltage of electrochemical cells to their chemical thermodynamics via the Nernst equation.
  • 1889 — Svante Arrhenius introduces the idea of activation energy for chemical reactions, giving the Arrhenius equation.
  • 1893 — Wilhelm Wien discovers the displacement law for a blackbody's maximum specific intensity.

1900–1944

  • 1900 — Max Planck suggests that light may be emitted in discrete frequencies, giving his law of black-body radiation
  • 1905 — Albert Einstein argues that the reality of quanta would explain the photoelectric effect
  • 1905 — Einstein mathematically analyzes Brownian motion as a result of random molecular motion
  • 1906 — Nernst presents a formulation of the third law of thermodynamics
  • 1907 — Einstein uses quantum theory to estimate the heat capacity of an Einstein solid
  • 1909 — Constantin Carathéodory develops an axiomatic system of thermodynamics
  • 1910 — Einstein and Marian Smoluchowski find the Einstein—Smoluchowski formula for the attenuation coefficient due to density fluctuations in a gas
  • 1911 — Paul Ehrenfest and Tatjana Ehrenfest—Afanassjewa publish their classical review on the statistical mechanics of Boltzmann, Begriffliche Grundlagen der statistischen Auffassung in der Mechanik
  • 1912 — Peter Debye gives an improved heat capacity estimate by allowing low-frequency phonons
  • 1916 — Sydney Chapman and David Enskog systematically develop the kinetic theory of gases.
  • 1916 — Einstein considers the thermodynamics of atomic spectral lines and predicts stimulated emission
  • 1919 — James Jeans discovers that the dynamical constants of motion determine the distribution function for a system of particles
  • 1920 — Megh Nad Saha states his ionization equation
  • 1923 — Debye and Erich Huckel publish a statistical treatment of the dissociation of electrolytes
  • 1924 — Satyendra Nath Bose introduces Bose–Einstein statistics, in a paper translated by Einstein
  • 1926 — Enrico Fermi and Paul Dirac introduce Fermi–Dirac statistics for fermions
  • 1927 — John von Neumann introduces the density matrix representation and establishes quantum statistical mechanics
  • 1928 — John B. Johnson discovers Johnson noise in a resistor
  • 1928 — Harry Nyquist derives the fluctuation-dissipation relationship for a resistor to explain Johnson noise
  • 1929 — Lars Onsager derives the Onsager reciprocal relations
  • 1938 — Anatoly Vlasov proposes the Vlasov equation for a correct dynamical description of ensembles of particles with collective long range interaction.
  • 1939 — Nikolay Krylov and Nikolay Bogolyubov give the first consistent microscopic derivation of the Fokker-Planck equation in the single scheme of classical and quantum mechanics.
  • 1942 — Joseph Leo Doob states his theorem on Gauss–Markov processes
  • 1944 — Lars Onsager gives an analytic solution to the 2-dimensional Ising model, including its phase transition

1945–present

  • 1945–1946 — Nikolay Bogoliubov develops a general method for a microscopic derivation of kinetic equations for classical statistical systems using BBGKY hierarchy.
  • 1947 — Nikolay Bogoliubov and Kirill Gurov extend this method for a microscopic derivation of kinetic equations for quantum statistical systems.
  • 1948 — Claude Elwood Shannon establishes information theory.
  • 1957 — Aleksandr Solomonovich Kompaneets derives his Compton scattering Fokker–Planck equation.
  • 1957 — Ryogo Kubo derives the first of the Green-Kubo relations for linear transport coefficients.
  • 1957 — Edwin T. Jaynes gives MaxEnt interpretation of thermodynamics from information theory.
  • 1960–1965 — Dmitry Zubarev develops the method of non-equilibrium statistical operator, which becomes a classical tool in the statistical theory of non-equilibrium processes.
  • 1972 — Jacob Bekenstein suggests that black holes have an entropy proportional to their surface area.
  • 1974 — Stephen Hawking predicts that black holes will radiate particles with a black-body spectrum which can cause black hole evaporation

 

 

 

ELECTRONIC AND COMMUNICATION ENGINEERING

is an engineering discipline which uses the scientific knowledge of the behavior and effects of electrons to develop components, devices, systems, or equipment (as in electron tubes, transistors, integrated circuits, and printed circuit boards) that uses electricity as part of its driving force. Both terms denote a broad engineering field that encompasses many sub fields including those that deal with power, instrumentation engineering, telecommunications, semiconductor circuit design, and many others.

- http://en.wikipedia.org/wiki/Electronic_engineering

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