Irreversibility and Entropy of an Isolated System
5. Irreversibility and Entropy of an Isolated System
Since δQ = 0 for isolated systems, and δσ > 0 for irreversible processes, Eq. (28) yields that dS > 0. When warm water is exposed to ambient air, as illustrated in Example 9, the
system “drifts” in the absence of internal constraints towards an equilibrium state. We saw from Example 9 that for a composite system consisting of (1) warm water directly losing heat to air (cf. Figure 16a ) and (2) that water being supplied with heat equal to the lost value through a Carnot heat pump, a net work loss occurred. This loss is called the irreversibility I of the composite system. In the case discussed in Example 9,
I=T 0 σ.
A rigorous proof of this equality is contained in Chapter 4. j. Example 10
An uninsulated coffee pot is maintained at a temperature of 350 K in a 300 K ambient –2 by supplying 1050 W of electrical work. The heat transfer coefficient is 0.2 kW m –1 2
K , and heat transfer occurs over a pot surface area of 0.5 m . Determine the entropy generated:
In the system contained within the boundary cs 1 , as illustrated in Figure 20a (i.e., for only the coffee within the pot), assuming the pot boundary temperature to be 350 K.
The matter contained within cs 2 , as illustrated in Figure 20b (i.e., for the system in- cluding both the coffee and pot) For the system containing the coffee, pot, and the ambient (i.e., bounded by the sur-
face cs 3 illustrated in Figure 20c ) for which T b =T 0 which is the ambient temperature. Solution
Selecting the control surface internally, and applying the First law, ˙ Q – W ˙ elec = dE/dt. At steady state, dE/dt = 0 so that ˙ Q = W ˙ elec = –1050 W. Applying the entropy balance equation in rate form dS/dt –
Q /T ˙ b = σ ˙ , we obtain
0 – (–1050/T b )= σ ˙ . Since T b = 350 K,
= 1050÷350 = 3 W K –1 . Selecting the control surface
cs 2 to be flush with the pot walls, the boundary tempera- ture T b must be determined. Applying the convection heat transfer relation
h A (T b –T 0 )= ˙ Q = 1050
W, the boundary temperature is determined as,
T b = 1.05 ÷ (0.2 × 0.5) + Figure 20: Entropy generation within a coffee pot.
300 = 310.5 K, and σ ˙ =
–(–1050 ÷ 310.5) = 3.382 W K –1 . Upon comparison with the previous solution, we find that irreversible heat transfer
between the coffee and pot walls causes an entropy generation of 3.382 – 3 = 0.382 W K –1 .
Selecting the control surface cs 3 such that the boundary exists outside the pot, T b =T 0 ,
0 – (–1050 ÷ 300) = -1 σ, i.e., σ ˙ = + 3.5 W K . No irreversibilities exist outside the boundary of the control surface cs 3 . The entropy
change in this composite system (using T b =T 0 ) equals the entropy change in an iso- lated system, since there is no entropy production within the ambient. Remarks For the matter contained within the surfaces cs 2 and cs 3 which include the pot wall, σ ˙ = 0 – (1050 ÷ 310.5) – (–1050 ÷ 300) = 0.118 W K –1 due to the heat transfer between the ambient and pot walls. By a suitable choice of the boundary, we are able to determine contributions to over- all σ. The major contribution is due to destruction of electrical work into heat called
electrical frictional work. The change in entropy due to:
destruction of electrical work within the coffee pot = 3 W K –1 . irreversible heat transfer between coffee and pot walls = 0.38 W K –1 . irreversible heat transfer between pot walls and ambient = 0.12 W K –1
. The change in entropy of the isolated system = 3.5 W K .
k. Example 11 An uninsulated coffee pot is maintained at a temperature of 350 K in a 300 K ambi- ent. Instead of supplying electrical work, we can compensate for the heat loss by
placing a heat pump between the coffee pot and ambient, as shown in Figure 21 . What is the electrical work required to operate the heat pump?
Solution: COP = 350 ÷ (350–300) = 7, i.e., W ˙ elec = 1050 ÷ 7 = 150 W. The pot can be maintained at 350 K by providing 150 W of electrical power to a heat
engine, rather than directly supplying 1050 W as in the previous example.
Parts
» COMPUTATIONAL MECHANICS and APPLIED ANALYSIS
» Explicit and Implicit Functions and Total Differentiation
» Exact (Perfect) and Inexact (Imperfect) Differentials
» Intermolecular Forces and Potential Energy
» Internal Energy, Temperature, Collision Number and Mean Free Path
» Vector or Cross Product r The area A due to a vector product
» First Law for a Closed System
» First Law For an Open System
» STATEMENTS OF THE SECOND LAW
» Cyclical Integral for a Reversible Heat Engine
» Irreversibility and Entropy of an Isolated System
» Degradation and Quality of Energy
» SINGLE–COMPONENT INCOMPRESSIBLE FLUIDS
» Evaluation of Entropy for a Control Volume
» Internally Reversible Work for an Open System
» MAXIMUM ENTROPY AND MINIMUM ENERGY
» Generalized Derivation for a Single Phase
» LaGrange Multiplier Method for Equilibrium
» Absolute and Relative Availability Under Interactions with Ambient
» Irreversibility or Lost Work
» Applications of the Availability Balance Equation
» Closed System (Non–Flow Systems)
» Heat Pumps and Refrigerators
» Work Producing and Consumption Devices
» Graphical Illustration of Lost, Isentropic, and Optimum Work
» Flow Processes or Heat Exchangers
» CLASSICAL RATIONALE FOR POSTULATORY APPROACH
» Generalized Legendre Transform
» Van der Waals (VW) Equation of State
» Other Two–Parameter Equations of State
» Compressibility Charts (Principle of Corresponding States)
» Boyle Temperature and Boyle Curves
» Three Parameter Equations of State
» Empirical Equations Of State
» State Equations for Liquids/Solids
» Internal Energy (du) Relation
» EXPERIMENTS TO MEASURE (u O – u)
» Vapor Pressure and the Clapeyron Equation
» Saturation Relations with Surface Tension Effects
» Temperature Change During Throttling
» Throttling in Closed Systems
» Procedure for Determining Thermodynamic Properties
» Euler and Gibbs–Duhem Equations
» Relationship Between Molal and Pure Properties
» Relations between Partial Molal and Pure Properties
» Mixing Rules for Equations of State
» Partial Molal Properties Using Mixture State Equations
» Ideal Solution and Raoult’s Law
» Completely Miscible Mixtures
» DEVIATIONS FROM RAOULT’S LAW
» Mathematical Criterion for Stability
» APPLICATION TO BOILING AND CONDENSATION
» Physical Processes and Stability
» Constant Temperature and Volume
» Equivalence Ratio, Stoichiometric Ratio
» Entropy, Gibbs Function, and Gibbs Function of Formation
» Entropy Generated During an Adiabatic Chemical Reaction
» MASS CONSERVATION AND MOLE BALANCE EQUATIONS
» Evaluation of Properties During an Irreversible Chemical Reaction
» Criteria in Terms of Chemical Force Potential
» Generalized Relation for the Chemical Potential
» Nonideal Mixtures and Solutions
» Gas, Liquid and Solid Mixtures
» Availability Balance Equation
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