- Entropy (energy dispersal)
The thermodynamic concept of entropy can be described qualitatively as a measure of energy dispersal (energy distribution) at a specific temperature. Changes in
entropy can be quantitatively related to the distribution or the spreading out of theenergy of athermodynamic system divided by its temperature. Similar terms have been in use from early in the history ofclassical thermodynamics , and with the development ofstatistical thermodynamics and quantum theory, entropy changes have been described in terms of the mixing or "spreading" of the total energy of each constituent of a system over its particular quantized energy levels.Such descriptions have tended to be used together with commonly used terms such as disorder and
chaos which have the problems of being ambiguous, and in common usage mean the opposite to the equilibrium they are equated to in thermodynamics. As well as causing confusion, this can hamper understanding. A recently developed method for introducing entropy, particularly in relation tochemistry andbiology , avoids these ambiguous terms, and instead describes entropy in a context of "energy dispersal" with a focus on explaining how energy is involved, and how the greater the energy dispersal.The concept of
thermodynamics involving dispersal of energy, particularly with reference toentropy , goes back to the roots of the science, withWilliam Thomson, 1st Baron Kelvin referring to "dissipation of mechanical energy" in 1852. However, early assumptions about molecules being initially in an ordered state and rapidly proceeding to "the disordered most probable state" led to the subject commonly being introduced in terms of entropy as order and disorder. [Boltzmann. Ludwig, Lectures on Gas Theory (Part II, 1898) translated by Stephen G. Brush. 1964, University of California Press p. 443] While this suggested a concept of an abstraction closely related to probability, the ambiguity of the terms used such as disorder andchaos often led to misunderstandings. Students were being asked to grasp meanings directly contradicting their normal usage, with equilibrium being equated to "perfect internal disorder" and the mixing of milk in coffee from apparent chaos to uniformity being described as a transition from an ordered state into a disordered state.Microsoft Encarta 2006. © 1993–2005 Microsoft Corporation. All rights reserved.] Studies found that few understood what these terms were intended to convey, and that even though microstates and energy levels were emphasised in the course, for most these points were overwhelmed by simplistic notions of randomness or disorder. Many of those learning by practising calculations did not perceive all the intrinsic meanings of equations, and there was a need for qualitative explanations of thermodynamic relationships. [Carson, E. M. and J. R. Watson (Department of Educational and Professional Studies, Kings College, London), " [http://www.rsc.org/pdf/uchemed/papers/2002/p2_carson.pdf Undergraduate students' understandings of entropy and Gibbs Free energy] ", University Chemistry Education - 2002 Papers, Royal Society of Chemistry.] [Sozbilir, Mustafa, PhD studies: Turkey, "A Study of Undergraduates’ Understandings of Key Chemical Ideas in Thermodynamics", PhD Thesis, Department of Educational Studies, The university of York, 2001.]To meet this need, terms such as "energy dispersal" and "spreading of energy" can be used with careful exclusion of references to "disorder" and "chaos" except in the context of explaining misconceptions, always using the new terms in the context of explanations of where and how the energy is dispersing or spreading to emphasise the underlying qualitative meaning.Frank L. Lambert, [http://jchemed.chem.wisc.edu/HS/Journal/Issues/2002/Feb/abs187.html JCE 2002 (79) 187 [Feb] Disorder--A Cracked Crutch for Supporting Entropy Discussions] , updated version at [http://www.entropysite.com/cracked_crutch.html Disorder — A Cracked Crutch For Supporting Entropy Discussions] ] Variations on this approach have been adopted by a significant number of chemistry textbooks, mostly in the
United States . The noted British authorPeter Atkins , who previously wrote of dispersal leading to a disordered state, has revised the 8th edition of his internationally respected textbook "Physical Chemistry" to describe entropy in terms of dispersal of energy, and has discarded 'disorder' as a description. [cite book | last = Atkins | first = Peter | title = The Second Law | publisher = Scientific American Library | year = 1984 | id = ISBN 0-7167-5004-X] [cite book | last = Atkins | first = Peter | coauthors = Julio De Paula | title = Physical Chemistry , 8th edition | publisher = Oxford University Press | year = 2006 | id = ISBN 0-19-870072-5]Historical development of the concept
Although it is difficult to pinpoint the exact origin of "energy dispersal" as a description of entropy change, it is likely that this concept began with the ideas of
William Thomson (Lord Kelvin) who in 1852 published his famous article "On a Universal Tendency in Nature to the Dissipation of Mechanical Energy." [Jensen, William. (2004). " [http://jchemed.chem.wisc.edu/Journal/Issues/2004/May/abs639_2.html Entropy and Constraint of Motion] ." "Journal of Chemical Education" (81) 693, May] In this article, Thomson makes a distinction between two types or "stores" of mechanical energy: "statical" and "dynamical". He discusses how these two types of energy can change, from one form to the other, during a thermodynamic transformation and that whenheat is created by any unreversible process (such as friction) or when heat is diffused by conduction, there is a dissipation of mechanical energy, and a full restoration of it to its primitive condition is impossible. [Thomson, William (1852). " [http://zapatopi.net/kelvin/papers/on_a_universal_tendency.html On a Universal Tendency in Nature to the Dissipation of Mechanical Energy] ." Proceedings of the Royal Society of Edinburg, April 19.] [Thomson, William (1874). " [http://digicoll.library.wisc.edu/cgi-bin/HistSciTech/HistSciTech-idx?type=turn&entity=HistSciTech001202440005&isize=M Kinetic Theory of the Dissipation of Energy] ", "Nature, IX. pp 441-444" (April 9).]In the mid 1950s, with the development of quantum theory, researchers began speaking about entropy changes in terms of the mixing or "spreading" of the total energy of each constituent of a system over its particular quantized energy levels, such as by the the
reactant s andproduct s of achemical reaction .cite book | last = Denbigh | first = Kenneth | title = The Principles of Chemical Equilibrium, 4th Ed. | publisher = Cambridge University Press | year = 1981 | id = ISBN 0-521-28150-4]In 1984, Oxford physical chemist
Peter Atkins in his popular book "The Second Law", written for non-scientists, presents a non-mathematical interpretation of what he called the “infinitely incomprehensible entropy” in simple terms, describing the second law of thermodynamics as "energy tends to disperse", but then writes in terms of a collapse intochaos and the corruption of the quality of energy terms which can be confusing and problematic. His analogies include the concept of an intelligent being called “Boltzmann’s Demon ” who relentlessly runs around re-organizing and dispersing energy to shows how Boltzmann’s “"W"” from his probability equation relates to energy dispersion, transmitted via atomic vibrations and collisions and other verbal arguments. He states: “each atom carries kinetic energy, and the spreading of the atoms spreads the energy…the Boltzmann equation therefore captures the aspect of dispersal: the dispersal of the entities that are carrying the energy.” [cite book | last = Atkins | first = Peter | title = The Second Law | publisher = Scientific American Library | year = 1984 | id = ISBN 0-7167-5004-X] While the book had limited impact, Atkins continued to describe entropy as energy dispersal leading to a disordered state in his influential "Physical Chemistry", until discarding 'disorder' as a description in the 8th edition of 2006.Stanley Sandler in "Chemical and Engineering Thermodynamics" of 1989 described how a quantity TS, in a
thermodynamic process , can be interpreted as the amount ofmechanical energy that has been converted intothermal energy viscous dissipation, dispersion, and other system irreversibilities. [cite book | last = Sandler | first = Stanley, I. | title = Chemical and Engineering Thermodynamics | publisher = John Wiley & Sons | year = 1989 | id = ISBN 0-471-83050-X] In another example, John Wrigglesworth in 1997 described spatial particle distributions as being represented in terms of distributions of energy states. In this direction, according to thesecond law of thermodynamics , isolated systems will have the tendency to redistribute the energy of the system to that of a more probable arrangement or a maximum probability of energy distribution, i.e. from that of being concentrated to that of being spread out. In this process, the total energy does not change, as per thefirst law of thermodynamics , but rather the energy tends to disperse from a coherent to a more incoherent state. [cite book | last = Wrigglesworth | first = John | title = Energy and Life (Modules in Life Sciences) | publisher = CRC | year = 1997 | id = ISBN 0-7484-0433-3 [http://books.google.com/books?vid=ISBN0748404333&id=YAZhYwyf5xgC&pg=PA5&lpg=PA5&dq=entropy+energy+dispersal&sig=wcJw3AVjnFrruPZJE22QWYcUnL4 (see excerpt)] ]Other authors using variations on these terms included Cecie Starr and Andrew Scott. [cite book | last = Starr | first = Cecie | coauthors = Taggart, R. | title = Biology - the Unity and Diversity of Life | publisher = Wadsworth Publishing Co. | year = 1992 | id = ISBN 0-534-16566-4] [cite book | last = Scott | first = Andrew | title = 101 Key ideas in Chemistry | publisher = Teach Yourself Books | year = 2001 | id = ISBN 0-07-139665-9] In the 1999 book "Statistical Thermodynamics", M.C. Gupta defined entropy as a function which measures how energy disperses when a system changes from one state to another. [cite book | last = Gupta | first = M.C. | title = Statistical Thermodynamics | publisher = New Age Publishers | year = 1999 | id = ISBN 81-224-1066-9 [http://books.google.com/books?vid=ISBN8122410669&id=GvsKJKsjXEoC&pg=PA62&lpg=PA62&dq=entropy+energy+dispersal&sig=M1VQkDIyIW2j0zS26Cl7ZYV3wLs (see excerpt)] ]
In 1996 the Physicist
Harvey S. Leff developed a theoretical foundation for the concept which he called "Thermodynamic entropy: The spreading and sharing of energy". [Leff, H. S. Am. J. Phys. 1996, 64, 1261-1271] Another physicist, ProfessorDaniel F. Styer , had an article published which showed that “entropy as disorder” was inadequate. [Styer D. F., Am. J. Phys. 2000, 68, 1090-1096] In an article published in the Journal of Chemical Education in 2002, Professor EmeritusFrank L. Lambert contended that the confusing portrayal of entropy as "disorder" should be abandoned, and went on to develop detailed resources for chemistry instructors implementing the concept of entropy increase as measuring the spontaneous dispersal of energy: how much energy is spread out in a process, or how widely spread out it becomes – at a specific temperature. Frank L. Lambert, [http://www.entropysite.com/students_approach.html A Student’s Approach to the Second Law and Entropy] ] By early in 2006 the majority of new editions of US first-year university texts had adopted this approach: see list below.Introductory approach to entropy
The description of entropy as amounts of "mixedupness" or "disorder" and the abstract nature of statistical mechanics can lead to confusion and considerable difficulty for those beginning the subject. [Frank L. Lambert, [http://www.secondlaw.com/six The Second Law of Thermodynamics (6)] ] An approach to instruction emphasising the qualitative simplicity of entropy has been published and made available online.Frank L. Lambert, [http://www.entropysite.com/entropy_is_simple/ Entropy Is Simple, Qualitatively] ]
In this approach, the
second law of thermodynamics is introduced as "Energy spontaneously disperses from being localized to becoming spread out if it is not hindered from doing so." in the context of common experiences such as a rock falling, a hot frying pan cooling down, iron rusting, air leaving a punctured tire and ice melting in a warm room. Entropy is then depicted as a sophisticated kind of "before and after" yardstick — measuring how much energy is spread out/T as a result of a process such as heating a system, or how widely spread out the energy is after something happens in comparison with its previous state, in a process such as gas expansion or fluids mixing (at a constant temperature). The equations are explored with reference to the common experiences, with emphasis that in chemistry the energy that entropy measures as dispersing is internal energy, which beginners can most clearly understand as “motional energy”, the translational and vibrational and rotational energy of molecules.By giving concrete examples, this approach is effective in explaining entropy to assist those who have great difficulty in grasping mathematical abstractions. The statistical interpretation is related to
quantum mechanics in describing the way that energy is distributed (quantized) amongst molecules on specific energy levels, with all the energy of the macrostate always in only one Microstate at one instant. Entropy is described as measuring the energy dispersal for a system by the number of accessible microstates, the number of different arrangements of all its energy at the next instant. Thus, an increase in entropy means a greater number of microstates for the Final state than for the Initial, and hence more choices for the arrangement of a system's total energy at any one instant. Here, the greater 'dispersal of the total energy of a system' means the existence of so many possibilities. [Frank L. Lambert, [http://www.entropysite.com/entropy_is_simple/index.html#microstate The Molecular Basis for Understanding Simple Entropy Change] ] Continuous movement and molecular collisions visualised as being like bouncing balls blown by air as used in a lottery can then lead on to showing the possibilities of many Boltzmann distributions and continually changing "distribution of the instant", and so on to the idea that when the system changes, dynamic molecules will have a greater number of accessible microstates. In this approach, all everyday spontaneous physical happenings and chemical reactions are depicted as involving some type of energy flows from being localized or concentrated to becoming spread out to a larger space, always to a state with a greater number of microstates.
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