third law of thermodynamics

(noun)

a law which states that the entropy of a perfect crystal at absolute zero is exactly equal to zero

Related Terms

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  • paramagnetic
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Examples of third law of thermodynamics in the following topics:

  • The Third Law

    • According to the third law of thermodynamics, the entropy of a perfect crystal at absolute zero is exactly equal to zero.
    • The third law of thermodynamics is sometimes stated as follows: The entropy of a perfect crystal at absolute zero is exactly equal to zero.
    • The third law was developed by the chemist Walther Nernst during the years 1906-1912.
    • In simple terms, the third law states that the entropy of a perfect crystal approaches zero as the absolute temperature approaches zero.
    • Absolute value of entropy can be determined shown here, thanks to the third law of thermodynamics.
  • The Third Law of Thermodynamics and Absolute Energy

    • The third law of thermodynamics states that the entropy of a system approaches a constant value as the temperature approaches absolute zero.
    • The third law of thermodynamics states that the entropy of a system approaches a constant value as the temperature approaches zero.
    • A more general form of the third law applies to systems such as glasses that may have more than one minimum energy state: the entropy of a system approaches a constant value as the temperature approaches zero.
    • Physically, the law implies that it is impossible for any procedure to bring a system to the absolute zero of temperature in a finite number of steps.
    • The entropy (S) of a substance (compound or element) as a function of temperature (T).
  • The Three Laws of Thermodynamics

    • The laws of thermodynamics define fundamental physical quantities (temperature, energy, and entropy) that characterize thermodynamic systems.
    • The first law of thermodynamics, also known as Law of Conservation of Energy, states that energy can neither be created nor destroyed; energy can only be transferred or changed from one form to another.
    • The second law of thermodynamics says that the entropy of any isolated system always increases.
    • A simple way to think of the second law of thermodynamics is that a room, if not cleaned and tidied, will invariably become more messy and disorderly with time - regardless of how careful one is to keep it clean.
    • The third law of thermodynamics states that the entropy of a system approaches a constant value as the temperature approaches absolute zero.
  • Adiabatic Processes

    • It is impossible to reduce the temperature of any system to zero temperature in a finite number of finite operations.
    • In our Atom on "Adiabatic Processes" (category: the First Law of Thermodynamics), we learned that an adiabatic process is any process occurring without gain or loss of heat within a system.
    • Previously, we learned about the third law of thermodynamics, which states: the entropy of a perfect crystal at absolute zero is exactly equal to zero.
    • According to the third law, the reason that T=0 cannot be reached is explained as follows: Suppose the temperature of a substance can be reduced in an isentropic process by changing the parameter X from X2 to X1.
    • However, going back to the third law, at T=0 there is no entropy difference, and therefore an infinite number of stepswould be needed for this process (illustrated in ).
  • Carnot Cycles

    • We know from the second law of thermodynamics that a heat engine cannot be 100 percent efficient, since there must always be some heat transfer Qc to the environment.
    • The second law of thermodynamics can be restated in terms of the Carnot cycle, and so what Carnot actually discovered was this fundamental law.
    • The second law of thermodynamics (a third form): A Carnot engine operating between two given temperatures has the greatest possible efficiency of any heat engine operating between these two temperatures.
    • What Carnot found was that for a perfect heat engine, the ratio Qc/Qh equals the ratio of the absolute temperatures of the heat reservoirs.
    • (Derivation of the formula is slightly beyond the scope of this atom. ) No real heat engine can do as well as the Carnot efficiency—an actual efficiency of about 0.7 of this maximum is usually the best that can be accomplished.
  • A Review of the Zeroth Law

    • Zeroth law justifies the use of thermodynamic temperature, defined as the shared temperature of three designated systems at equilibrium.
    • The Zeroth Law of Thermodynamics states: If two systems, A and B, are in thermal equilibrium with each other, and B is in thermal equilibrium with a third system, C, then A is also in thermal equilibrium with C.
    • This law was postulated in the 1930s, after the first and second laws of thermodynamics had been developed and named.
    • A brief introduction to the zeroth and 1st laws of thermodynamics as well as PV diagrams for students.
    • Discuss how the Zeroth Law of Thermodynamics justifies the use of thermodynamic temperature
  • The Zeroth Law of Thermodynamics

    • The Zeroth Law of Thermodynamics states that systems in thermal equilibrium are at the same temperature.
    • There are a few ways to state the Zeroth Law of Thermodynamics, but the simplest is as follows: systems that are in thermal equilibrium exist at the same temperature.
    • What the Zeroth Law of Thermodynamics means is that temperature is something worth measuring, because it indicates whether heat will move between objects.
    • However, according to the Zeroth Law of Thermodynamics, if the systems are in thermal equilibrium, no heat flow will take place.
    • There are more formal ways to state the Zeroth Law of Thermodynamics, which is commonly stated in the following manner:
  • The First Law of Thermodynamics

    • The first law of thermodynamics states that energy can be transferred or transformed, but cannot be created or destroyed.
    • The first law of thermodynamics deals with the total amount of energy in the universe.
    • The law states that this total amount of energy is constant.
    • According to the first law of thermodynamics, energy can be transferred from place to place or changed between different forms, but it cannot be created or destroyed.
    • Another useful form of the first law of thermodynamics relates heat and work for the change in energy of the internal system:
  • The Second Law

    • The second law of thermodynamics deals with the direction taken by spontaneous processes.
    • The first law of thermodynamics would allow them to occur—none of those processes violate conservation of energy.
    • The law that forbids these processes is called the second law of thermodynamics .
    • The already familiar direction of heat transfer from hot to cold is the basis of our first version of the second law of thermodynamics.
    • Contrast the concept of irreversibility between the First and Second Laws of Thermodynamics
  • The First Law

    • The 1st law of thermodynamics states that internal energy change of a system equals net heat transfer minus net work done by the system.
    • The first law of thermodynamics is a version of the law of conservation of energy specialized for thermodynamic systems.
    • In equation form, the first law of thermodynamics is
    • The change in the internal energy of the system, ΔU, is related to heat and work by the first law of thermodynamics, ΔU=Q−W.
    • Explain how the net heat transferred and net work done in a system relate to the first law of thermodynamics
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