Ppt on second law of thermodynamics equation

FUEL CELL FUNDAMENTALS (Chapter. 2). Chapter 2. 연료전지 열역학 The purpose of this chapter ◈ 2 장의 목적 √ 열역학 : 한 형태에서 다른 형태로 에너지 변환, 에너지론의 한 분야 √ 연료전지 : 에너지 변환장치.

제 2 법칙 : 열은 100% 일로 변환될 수 없다 열 병목현상 : 연료전지는 열변환 단계 우회 2.1.4. Second Low Chapter 2. Fuel Cell Thermodynamics √ 엔트로피 : 시스템 가능한 미소상태 수, 시스템을 구성하는 가능한 방법 수 √ 엔트로피 : 무질서도 측정 ☞ 가장 간단한 고립 시스템 ◈ The second law of thermodynamics (2.6) Where, 2.1.4. Second Low Chapter 2. Fuel Cell Thermodynamics Figure 2.2. (a) The entropy of this 100 atom perfect crystal is zero because there is only/ Equations 2.81 and 2.82 (2.83) √ The general form of Nernst equation (2.84) ◈ Nernst equation Chapter 2. Fuel Cell Thermodynamics 2/


Chapter 19 Chemical Thermodynamics Lecture Presentation John D. Bookstaver St. Charles Community College Cottleville, MO © 2012 Pearson Education, Inc.

Continued Chemical Thermodynamics Second Law of Thermodynamics The second law of thermodynamics states that the entropy of the universe increases for spontaneous processes, and the entropy of the universe does not change for reversible processes. © 2012 Pearson Education, Inc. Chemical Thermodynamics Second Law of Thermodynamics In other/for the products and reactants and use Equation 19.14: We multiply the molar quantities by the coefficients in the balanced equation and subtract the total for the reactants/


Introduction to thermodynamics 1. Basics of chemical thermodynamics 2. Methods of thermodynamic value measurements.

. PV=nRT (gas law for ideal gas) equation of state of ideal gas; heat capacity at constant P and constant V are related as C P =C V +R ; C P /C V =  When the system undergoes change from one thermodynamic state to final state due change in properties like temperature, pressure, volume etc, the system is said to have undergone thermodynamic process. Second law of thermodynamics introduces entropy S/


Thermodynamics AP Physics Chapter 15.

proportional to temperature 13.4 Thermal Expansion Change in length is proportional to temperature So the equation is a is called the coefficient of linear expansion T0 T L0 DL 13.4 Imagine an infinitely thin ring 13.4 Thermal / .005 m3 and T = 300 K. The cycle is Totals 15.2 15.4 The Second Law of Thermodynamics-Intro 15.3 The Second Law of Thermodynamics-Intro The first law deals with conservation of energy. However there are situations that would conserve energy, but do not occur. Falling objects convert/


Entropy Balance Equation

basis by dividing both sides of the equation by the mass of the system, The Second Law of Thermodynamics Incorporating the net entropy transport into the system due to the mass flows gives the complete form of the Second Law of Thermodynamics! Notice that if the system is closed, The Laws of the Universe Conservation of Mass – The Continuity Equation Conservation of Energy – The First Law of Thermodynamics The Entropy Balance – The Second Law of Thermodynamics Special Application – Closed Systems Consider/


Weakly nonlocal continuum physics – the role of the Second Law Peter Ván HAS, RIPNP, Department of Theoretical Physics –Introduction Second Law Weak nonlocality.

physics – the role of the Second Law Peter Ván HAS, RIPNP, Department of Theoretical Physics –Introduction Second Law Weak nonlocality –Liu procedure –Classical irreversible thermodynamics –Ginzburg-Landau equation –Discussion general framework of any Thermodynamics (?) macroscopic continuum theories Thermodynamics science of macroscopic energy changes Thermodynamics science of temperature Nonequilibrium thermodynamics reversibility – special limit General framework: – Second Law – fundamental balances/


The Laws of Thermodynamics

and entropy decreases More About Entropy Note, the equation defines the change in entropy The entropy of the Universe increases in all natural processes This is another way of expressing the Second Law of Thermodynamics There are processes in which the entropy of a system decreases If the entropy of one system, A, decreases it will be accompanied by the increase of entropy of another system, B. The change in entropy/


–Introduction Second Law Weak nonlocality –Ginzburg-Landau equation –Schrödinger-Madelung equation –Digression: Stability and statistical physics –Discussion.

Second Law Weak nonlocality –Ginzburg-Landau equation –Schrödinger-Madelung equation –Digression: Stability and statistical physics –Discussion Weakly nonlocal nonequilibrium thermodynamics – fluids and beyond Peter Ván BCPL, University of Bergen, Bergen and RMKI, Department of Theoretical Physics, Budapest general framework of any Thermodynamics (?) macroscopiccontinuum theories Thermodynamics science of macroscopic energy changes Thermodynamics science of temperature Nonequilibrium thermodynamics/


Bond Graph Modeling and Simulation of Thermodynamic Systems For Plenary session, 2007 ICBGM Forbes T. Brown Lehigh University, emeritus, Bethlehem, PA.

true energy-based bond graph). The Second Law of Thermodynamics says that thermal energy is only partly convertible to free energy. A practical bond graph scheme for thermodynamics requires the efficient calculation of several thermodynamic properties. Preliminaries: This presentation is downloadable/, the output efforts are found from Chemical reactions, continued With more than one species present, the equations become Each μ i is a partial Gibbs free energy known as a chemical potential. This suggests the/


1 Second Law of Thermodynamics As the reaction goes to products our system becomes more disordered and the entropy of our system increases. One driving.

produces the very useful equation:This produces the very useful equation:                   1 2 11 1 2 TT R H K K n T T 28 THE EQUILIBRIUM CONSTANT Δ A plot of ln K vs. 1/T yields a straight line with a slope of - Δ H o /R. 29 20.5 THERMODYNAMICS AND TIME The first and second Laws of Thermodynamics cannot be proven, they are laws of experience and tell us/


JIF 314 Thermodynamics Sidang Video 2 22 OCT pm – pm

= (CV + nR) – V (dP/dT) At constant pressure, dP=0, the LHS becomes CP and, dP/dT = 0 Hence the equation reduce to (CP = CV + nR)/n  cP = cV + R = 3R/2 + R = 5R/2 Chapter 6 The second law of thermodynamics JIF 314 Thermodynamics Chapter 6 The second law of thermodynamics Chapter 7 The Carnot cycle and the thermodynamic temperature scale JIF 314 Thermodynamics Chapter 7 The Carnot cycle and the/


Weakly nonlocal non-equilibrium thermodynamics Peter Ván Budapest University of Technology and Economics, Department of Chemical Physics Non-equilibrium.

fluid reversible pressure (Fisher entropy) Schrödinger-Madelung fluid Potential form: Bernoulli equation Schrödinger equation Euler-Lagrange form Variational origin Why nonequilibrium thermodynamics? science of temperature Thermodynamics science of macroscopic energy changes general framework of any Thermodynamics (?) macroscopic (?) continuum (?) theories General framework: fundamental balances objectivity - frame indifference Second Law reversibility – special limit Conclusions Not everything is a balance/


Slide 1 www.kostic.niu.edu Reflections on Real (Thermodynamic) Entropy, Disorder and Statistical Information Entropy – (Lecture IV) Prof. M. Kostic Mechanical.

at first. Actually it is probably the most important equation in Thermodynamics and among the most important equations in natural sciences. T=T Any Slide 27 “Definition” of Temperature, Mass, etc… www.kostic.niu.edu The/ increased (The Second Law): 2009 January 10-12 © M. Kostic Slide 46 © M. Kostic “ The Second Law of Thermodynamics is considered one of the central laws of science, engineering and technology. “ The Second Law of Thermodynamics is considered one of the central laws of science, engineering /


Apes Practice Exam 2 Directions: Each group of lettered answer choices refers to the numbered statements of questions that immediately follow. For each.

distasteful. 60. In the general pattern of the oceans cur­rents, the direction of the currents nearest the equator move from (A) east to /of energy in the form of heat" is an example of the_____________, (A) first law of thermodynamics; first law of thermodynamics (B) second law of thermodynamics; first law of thermodynamics (C) first law of thermodynamics; second law of thermodynamics (D) first law of thermodynamics; third law of thermodynamics (E) third law of thermodynamics; first law of thermodynamics/


Heat flows from hot to cold Ch. 24 Thermodynamics.

K? The equation for ideal efficiency is as follows: Answer: Zero efficiency; (400 - 400)/400 = 0. This means no work output is possible for any heat engine unless a temperature difference exists between the reservoir and the sink. Heat Engines and the Second Law Natural systems tend to proceed toward a state of greater disorder. Order Tends to Disorder The first law of thermodynamics states that energy/


Chemical Thermodynamics Topics Overview: - Entropy – a measure of disorder or randomness - Second Law of Thermodynamics  The entropy of the universe increases.

slow to be truly reversible. Second Law of Thermodynamics The entropy of the universe does not change for a reversible (non-spontaneous) process. The entropy of the universe increases for irreversible (spontaneous) process. (In words) The truth is… “as a result of all spontaneous processes the entropy of the universe increases.” For reversible processes:  S univ =  S sys +  S surr = 0 (In mathematical equation) Second Law of Thermodynamics (continued)… In fact, we can/


Thermodynamics: Entropy, Free Energy Direction of Chemical Reactions Chapter 20 Entropy and Free Energy - Spontaneity of Reaction 1. The Second Law of.

the heat transferred plus the work performed, E = q + w. spontaneous ∆S universe > 0 (∆S universe ) The Second Law of Thermodynamics states that for a spontaneous process, ∆S universe = ∆S system + ∆S surroundings > 0 (∆S universe positive) Figure /equation: ∆S 0 =  mS 0 products -  nS 0 reactants Lecture 2 given condition, ∆S 0 rxn <0 In many spontaneous reaction, the system become more ordered at a given condition, ∆S 0 rxn <0. The Second Law of Thermodynamics indicated that the decrease in entropy of/


1 Thermodynamics Entropy, Energy and equilibrium Chapter 19.

Second Law of Thermodynamics 44 19.3 Second Law of Thermodynamics: System 10. Predict the sign of ΔS 0 for each of the following reactions: a) Ca +2 (aq) + 2OH - (aq) → Ca(OH) 2 (s) b) MgCO 3 (s) → MgO(s) + CO 2 (g) d) H 2 (g) + Br 2 (g) → 2HBr(g) 45 Second Law of Thermodynamics The second law of thermodynamics states that the entropy of/ + 2H 2 O(g) ΔH 0 = 114.4 kJ a) using Gibbs free Energy equation b) from standard free energies of formation. ( -76.0 kJ) 82 19.4 Gibbs free Energy: Example 18. For the /


111 Status of Core Courses: Biothermodynamics Christopher M. Saffron Department of Biosystems and Agricultural Engineering 07/14/14.

in Engineering Curriculum Course Description: …learn to apply the first and second laws of thermodynamics. Analysis of closed and open systems. Study of power cycles and refrigeration cycles. Study of gas-vapor mixtures and psychrometry. Analysis of reaction equilibria and phase equilibria. Prerequisites at MSU: BE 101. Introduction to Biosystems Engineering MTH 235. Differential Equations (first-order linear equations, exact equations, introduction to PDEs) BS 161. Cells and Molecules (energy metabolism/


Chemical Thermodynamics Lecture 3. ‘Theoretical basis of bioenergetics. Chemical kinetics and biological processes. Electrochemistry.’ ass. Falfushynska.

-4 M/s (0.08 M)(0.034 M) = 0.08/M s 13.2 rate = k [S 2 O 8 2- ][I - ] Chemical Thermodynamics Summary of the Kinetics of Zero-Order, First-Order and Second-Order Reactions OrderRate Law Concentration-Time Equation Half-Life 0 1 2 rate = k rate = k [A] rate = k [A] 2 ln[A] = ln[A] 0 - kt 1 [A] = 1/


Chemical Thermodynamics Chapter 17 Chemical Thermodynamics.

Chapter 17 Chemical Thermodynamics Chemical Thermodynamics Spontaneous Processes Entropy Second Law of Thermodynamics Third Law of Thermodynamics Gibbs Free Energy Predicting Spontaneity Standard Enthalpies of Formation Gibbs Free Energies of Formation Free Energy Changes Contents Chemical Thermodynamics Thermodynamics is the study of energy relationships that involve heat, mechanical work, and other aspects of energy and heat transfer. Chemical Thermodynamics First Law of Thermodynamics You will recall/


Thermodynamics AP Physics Chapter 15. Thermodynamics 13.3 Zeroth Law of Thermodynamics.

Temperature 14.2 Internal Energy Internal Energy equation First internal Energy (U) is equal to the number of particles (N) times average kinetic energy Since The equation changes to And since 14.2 Thermodynamics 14.3 Specific Heat and Calorimetry / monatomic gas that goes from 500 K to 372 K? Thermodynamics 15.4 The Second Law of Thermodynamics-Intro 15.3 The Second Law of Thermodynamics-Intro The first law deals with conservation of energy. However there are situations that would conserve energy, but/


Thermodynamics and Equilibrium. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–2 –We introduced the thermodynamic.

p, equals the enthalpy change,  H. –The second law for a spontaneous reaction at constant temperature and pressure becomes (Spontaneous reaction, constant T and P) Entropy, Enthalpy, and Spontaneity Now you can see how thermodynamics is applied to the question of reaction spontaneity. Copyright © Houghton Mifflin Company.All rights reserved. Presentation of Lecture Outlines, 19–12 –Rearranging this equation, we find –This inequality implies that for/


AE 630 Aero Engineering Thermodynamics. Unit - I.

/lb) – how much for water? Sensible heat vs Latent heat LHV/LHF Second Law of Thermodynamics: must expend energy to get process to work Refrigeration Cycle Refrigeration - Cooling of an object and maintenance of its temp below that of surroundings Working substance must alternate b/t colder and hotter regions Most common: vapor compression –Reverse of power cycle –Heat absorbed in low temp region and released in high/


Fundamental Concepts in Thermodynamics Doba Jackson, Ph.D. Associate Professor of Chemistry & Biochemistry Huntingdon College.

Law of Thermodynamics Equations of state and Ideal gas law Ideal Gas Law: PV= nRT PV/nT = constant (R) Ideal Gas Constant (R) *R is used in other thermodynamic equations * * Equations of State are equations that relate the major macroscopic variables of a physical state Volume is a decreasing function of pressure Boyle’s Law/ Usually the equation is trunicated after the second or third term. The Compression Factor Real gases show deviations from the ideal gas law mainly because of molecular interactions /


1 Chemistry Second Edition Julia Burdge Lecture PowerPoints Jason A. Kautz University of Nebraska-Lincoln Copyright (c) The McGraw-Hill Companies, Inc.

(rhombic)(s)° Chapter Summary: Key Points 5 Energy and Energy Changes Forms of Energy Energy Changes in Chemical Reactions Units of Energy Introduction to Thermodynamics States and State Functions The First Law of Thermodynamics Work and Heat Enthalpy Reactions Carried Out at Constant Volume or at Constant Pressure Enthalpy and Enthalpy Changes Thermochemical Equations Calorimetry Specific Heat and Heat Capacity Constant-Pressure Calorimetry Constant-Volume Calorimetry Hess/


Apes Practice Exam 2 Directions: Each group of lettered answer choices refers to the numbered statements of questions that immediately follow. For each.

distasteful. 60. In the general pattern of the oceans cur­rents, the direction of the currents nearest the equator move from (A) east to /of energy in the form of heat" is an example of the_____________, (A) first law of thermodynamics; first law of thermodynamics (B) second law of thermodynamics; first law of thermodynamics (C) first law of thermodynamics; second law of thermodynamics (D) first law of thermodynamics; third law of thermodynamics (E) third law of thermodynamics; first law of thermodynamics/


Chapter 2 T h e Laws of Thermodynamics. 1 The first law In physics,the principle of conservation of energy is of fundamental importance. Therefore,besides.

dT is only valid for reversible processes,while Equation (2.1)is always true. There exist many formulations for the first law of thermodynamics,which all have the same meaning, for example,there is no perpetuum mobile of the first kind. Example2.1: Internal energy/,in an isolated system the entropy is constant dS=0.Every experience confirms that this extremum is a maximum. R.Clausius Second law--For isolated systems in equilibrium it holds that dS=0 S=S max and for irreversible processes it holds that dS 〉/


© Copyright 2016Operator Generic Fundamentals Operator Generic Fundamentals 193004 - Thermodynamic Processes.

16 Figure: Basic Energy Balance of the First Law of Thermodynamics ELO 1.2 © Copyright 2016Operator Generic Fundamentals General Energy Equation 17 Figure: General Energy Equation for the First Law of Thermodynamics ELO 1.2 © Copyright 2016Operator Generic Fundamentals Thermodynamic Processes 18 Figure: Six Basic Processes of Steady Flow Systems ELO 1.2 © Copyright 2016Operator Generic Fundamentals Thermodynamic Processes Our four basic processes of our thermodynamic cycle are: –Steam Generator Process/


Chapter 4 Energy Analysis of Closed Systems Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition by Yunus.

is Now the conservation of energy principle, or the first law of thermodynamics for closed systems, is written as If the system does not move with a velocity and has no change in elevation, the conservation of energy equation reduces to We will / derive this last expression for h again once we have discussed the first law for the open system in Chapter 5 and the second law of thermodynamics in Chapter 7. The specific heats of selected liquids and solids are given in Table A-3. Example 4-8 Incompressible/


Chemical Thermodynamics 化學熱力學

Equations 熱化學方程式 Standard States and Standard Enthalpy Changes Standard Molar Enthalpies of Formation, Hfo Hess’s Law Bond Energies Changes in Internal Energy,  E Relationship of H and E Outline Spontaneity of Physical and Chemical Changes The Two Aspects of Spontaneity Dispersal of Energy and Matter Entropy熵, S, and Entropy Change, DS The Second Law of Thermodynamics Free Energy Change, DG, and Spontaneity The Temperature Dependence of Spontaneity The First Law of Thermodynamics 熱力學第一定律 Thermodynamics/


R. M. Kiehn University of Houston www.cartan.pair.com UNIA Lectures Baeza, Spain June 23-25, 2008 Environmental Turbulence From the new paradigm of Topological.

component). The number of holes (the second Betti number) is apparently 4. The second Betti number is a topological property ( an invariant of continuous deformation) of the sample box (~/ Evolution (with topological change) is the abstract and dynamical equivalent of the FIRST LAW OF THERMODYNAMICS L(J)A = i(J)dA + d{i(J)A} => Q /by Solutions to the equations of Continuous Topological Evolution Limit Cycle core Z = t Vortex and Spiral Arms Surprise Two Classes Of Solutions. 1.Those Solutions/


Chapter 4 Energy Analysis of Closed Systems Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 7th edition by Yunus.

of energy principle, or the first law of thermodynamics for closed systems, is written as Chapter 4 Closed System First Law for a Cycle If the system does not move with a velocity and has no change in elevation, the conservation of energy equation / derive this last expression for h again once we have discussed the first law for the open system in Chapter 5 and the second law of thermodynamics in Chapter 7. The specific heats of selected liquids and solids are given in Table A-3. Chapter 4 Example/


Ch15. Thermodynamics Thermodynamics is the branch of physics that is built upon the fundamental laws that heat and work obey. In thermodynamics the collection.

Specific Heat Capacities where the capital letter C refers to the molar specific heat capacity in units of J/(mol·K). The Second Law of Thermodynamics THE SECOND LAW OF THERMODYNAMICS: THE HEAT FLOW STATEMENT Heat flows spontaneously from a substance at a higher temperature to a substance/without reference to algebraic signs. Therefore, when these symbols appear in an equation, they do not have negative values assigned to them. Efficiencies are often quoted as percentages obtained by /


Anandh Subramaniam & Kantesh Balani

we usually we do not worry about the universe at large! The language of TD To understand the laws of thermodynamics and how they work, first we need to get the terminology right. Some of the terms may look familiar (as they are used in everyday language as / the above equations is called a perfect gas. Internal energy (a state function) is normally a function of T & V: U = U(T,V).  For a perfect gas: U = U(T) only. Humorous look at the three laws The first law says: “you cannot win”. The second law says: “/


Chapter 4 Energy Analysis of Closed Systems Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 5th edition by Yunus.

is Now the conservation of energy principle, or the first law of thermodynamics for closed systems, is written as If the system does not move with a velocity and has no change in elevation, the conservation of energy equation reduces to We will / derive this last expression for h again once we have discussed the first law for the open system in Chapter 5 and the second law of thermodynamics in Chapter 7. The specific heats of selected liquids and solids are given in Table A-3. Example 4-8 Incompressible/


A Research-Based Approach to the Learning and Teaching of Physics David E. Meltzer Department of Physics University of Washington.

’ thinking from introductory through advanced-level course Develop research-based curricular materials In collaboration with John Thompson, University of Maine Studies of university students in general physics courses have revealed substantial learning difficulties with fundamental concepts, including heat, work, and the first and second laws of thermodynamics: USA M. E. Loverude, C. H. Kautz, and P. R. L. Heron (2002); D. E. Meltzer (2004); M. Cochran/


Entropy: A Measure of Disorder. 2 Entropy and the Clausius Inequality The second law of thermodynamics leads to the definition of a new property called.

the isolated system The total entropy change for the isolated system is 18 This equation is the working definition of the second law of thermodynamics. The second law, known as the principle of increase of entropy, is stated as The total entropy change of an isolated system during a process always increases or, in the limiting case of a reversible process, remains constant. Now consider a general system exchanging mass as well/


Weakly nonlocal heat conduction – modeling memory and structure with nonequilibrium thermodynamics Peter Ván HAS, RIPNP, Department of Theoretical Physics.

–Hierarchy of heat equations - balances –Discussion general framework of any Thermodynamics (?) macroscopic (?) continuum (?) theories Thermodynamics science of macroscopic energy changes Thermodynamics science of temperature Why nonequilibrium thermodynamics? reversibility – special limit General framework: – Second Law – fundamental balances – objectivity - frame indifference Nonlocalities: Restrictions from the Second Law. change of the entropy current change of the entropy Change of the constitutive/


REFER TO THE FOLLOWING ENERGY EFFICIENCEIS, EXPRESSED AS PERCENTAGES: A) 100%B) 95%C) 30%D) 15% E) 1% 1.APPROXIMATE EFFICIENCY OF AN AVERAGE COAL-FIRED.

The Second Law of Thermodynamics is one of three Laws of Thermodynamics. The term "thermodynamics" comes from two root words: "thermo," meaning heat, and "dynamic," meaning power. Thus, the Laws of Thermodynamics are the Laws of "Heat Power." As far as we can tell, these Laws are absolute. All things in the observable universe are affected by and obey the Laws of Thermodynamics. WHAT IS THE 2 ND LAW OF THERMODYNAMICS (2 of 3) Second Law of Thermodynamics - Increased Entropy The Second Law of Thermodynamics/


Chapter Seventeen General Chemistry 4 th edition, Hill, Petrucci, McCreary, Perry Hall © 2005 Prentice Hall © 2005 1 Thermodynamics: Spontaneity, Entropy,

it possible for a spontaneous process to exhibit a decrease in entropy? Yes, if the surroundings ____________________. The Second Law of Thermodynamics Chapter Seventeen General Chemistry 4 th edition, Hill, Petrucci, McCreary, Perry Hall © 2005 Prentice Hall © 2005/ p  G f °(products) –  v r  G f °(reactants) Standard Free Energy Change, ∆G° The form of this equation should appear very familiar by now! Chapter Seventeen General Chemistry 4 th edition, Hill, Petrucci, McCreary, Perry Hall © 2005 Prentice/


Raymond A. Serway Chris Vuille Chapter Twelve The Laws of Thermodynamics.

Section 12.5 More About Entropy Note, the equation defines the change in entropy The entropy of the Universe increases in all natural processes – This is another way of expressing the Second Law of Thermodynamics There are processes in which the entropy of a system decreases – If the entropy of one system, A, decreases it will be accompanied by the increase of entropy of another system, B – The change in entropy/


PPT 107PHYSICAL CHEMISTRY Semester 2. CHAPTER 1 THERMODYNAMICS.

equilibrium with each other. It is so called because only after the first, second, and third laws of thermodynamics had been formulated was it realized that the zeroth law is needed for the development of thermodynamics. Moreover, a statement of the zeroth law logically precedes the other three. The zeroth law allows us to assert the existence of temperature as a state function. 1.4The Mole Relative Atomic Mass, Ar The/


Chapter 6 Thermochemistry. Copyright © Cengage Learning. All rights reserved 2 Capacity to do work or to produce heat. Law of conservation of energy –

s law of heat summation states that for a chemical equation that can be written as the sum of two or more steps, the enthalpy change for the overall equation is the sum of the enthalpy changes for the individual steps. Hess’s Law / spontaneous. Thermodynamics is used to help predict if a reaction will occur. Another factor is needed. Entropy The second law of thermodynamics - the universe spontaneously tends toward increasing disorder or randomness. Entropy (S o ) - a measure of the randomness of a chemical/


Solutions, Acids and Bases, Thermodynamics, Electrochemistry, Precipitation, Chemical Equilibrium, and Chemical Kinetics By: Karl Lewis, Mark Liv, Kevin.

from absolute zero, the entropy increases. Standard Entropy: S 0 = q rev (heat added)/T (temperature in Kelvin) Gibbs Free-Energy Gibbs Free-Energy Equation:  G 0 =  H 0 - T  S 0 –Equation is derived directly from the second law of thermodynamics. Electrochemistry Essential Definitions Electrolysis- a non-spontaneous chemical reaction is forced to occur when two electrodes are immersed in an electrically conductive sample, and/


1 PRINCIPLES OF REACTIVITY: ENTROPY AND FREE ENERGY.

.This entropy change is calculated by considering the two terms that make up this entropy. 36 Second Law of Thermodynamics ΔS o universe = ΔS o surroundings + ΔS o system, where ΔS o surroundings = q surroundings / T = - ΔH o system / T and Δ S o system = ΔS o (products) - ΔS o (reactants), Equation 20.1. Be sure to include the stoichiometric coefficient with each term. 37 2nd/


Chapter 18 Thermodynamics and Equilibrium 18 | 2 Contents and Concepts 1.First Law of Thermodynamics 2.Entropy and the Second Law of Thermodynamics 3.Standard.

,  H. 18 | 7 Spontaneous Processes and Entropy 2. Entropy and the Second Law of Thermodynamics a.Define spontaneous process. b.Define entropy. c.Relate entropy to disorder in a molecular system (energy dispersal). d.State the second law of thermodynamics in terms of system plus surroundings. 18 | 8 2. Entropy and the Second Law of Thermodynamics (cont) e.State the second law of thermodynamics in terms of the system only. f.Calculate the entropy change for a phase/


What is thermodynamics and what is it for? II. Continuum physics – constitutive theory Peter Ván HAS, RIPNP, Department of Theoretical Physics –Introduction.

e.g. Nonlocalities: Restrictions from the Second Law. change of the entropy current change of the entropy Change of the constitutive space Second Law: basic balances – basic state: – constitutive state: – constitutive functions: weakly nonlocal Second law: Constitutive theory Method: Liu procedure (universality) (and more) Irreversible thermodynamics: – basic state: – constitutive state: – constitutive functions: primary!! Liu procedure (Farkas lemma): A) Liu equations: Heat conduction: a=e B) Dissipation/


2. Thermodynamics of systems. 2 2.1 The Helmholtz free energy  S system +  S surroundings  0 We define two further thermodynamic functions which are.

the enthalpy of the stable modification of an element is taken zero, that of a compound is taken equal to the enthalpy of formation. Remember: The zero level of entropy is fixed by the third law of thermodynamics: the entropy of pure /equation of state second third fourth virial coefficient This virial equation of state it is basically a power series of the concentration (1/V m ) Substituting V/n for V m : (2.64) (2.65) 74 2.13 The principle of corresponding states The deviation from the ideal gas law/


Chemical Thermodynamics Chemical Thermodynamics Thermo Part 2 1.

11 Chemical Thermodynamics Second Law of Thermodynamics The second law of thermodynamics states that the entropy of the universe increases for spontaneous processes, and the entropy of the universe does not change for reversible processes. 12 Chemical Thermodynamics Second Law of Thermodynamics In / m are the coefficients in the balanced chemical equation. 30 Chemical Thermodynamics SAMPLE EXERCISE 19.5 Calculating  S from Tabulated Entropies Calculate  S° for the synthesis of ammonia from N 2 (g) and H/


Ads by Google