Thermodynamics Homework: Entropy Change, Phase Equilibrium & More

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SUMMARY

The discussion focuses on thermodynamics homework involving entropy change and phase equilibrium, specifically regarding the heating and vaporization of 250 g of water at different pressures. For part (1a), the total change in entropy can be calculated using the equation S2-S1 = mC ∫(dT/T) + Latent heat of transformation/373.15K, where the latent heat must be referenced from steam tables. In part (1b), the change in entropy at 8 atm can be derived using a modified version of the equation from part (1a). Part (1c) discusses the equilibrium condition between two phases, emphasizing the importance of the term +μdN in the fundamental thermodynamic relation.

PREREQUISITES
  • Understanding of thermodynamic principles, particularly entropy and phase changes.
  • Familiarity with the concept of latent heat and its role in phase transitions.
  • Knowledge of steam tables for specific enthalpy and entropy values.
  • Ability to apply calculus in thermodynamic equations, specifically integrals.
NEXT STEPS
  • Research the enthalpy of vaporization for water at various pressures.
  • Learn how to use steam tables to find specific enthalpy and entropy values.
  • Study the derivation of the fundamental thermodynamic relation and its applications.
  • Explore the implications of phase equilibrium and the role of chemical potential in thermodynamics.
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Students of thermodynamics, particularly those tackling advanced topics in phase equilibrium and entropy changes, as well as educators seeking to enhance their teaching materials on these subjects.

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Homework Statement



(1a) What are the total change in energy and entropy if 250 g of water at 20◦C is heated
and vaporised to yield 250 g of steam, all at atmospheric pressure?

(1b) Find the change in the entropy of 250 g of liquid water at its boiling point when it is
vaporised at a pressure of 8 atm. Give a brief physical explanation for how this entropy
change compares with the entropy change for vaporisation at 1 atm pressure.

(1c) We can allow for a possible transition between two phases of a substance by adding
the term +μdN in the fundamental thermodynamic relation for dE. Derive the condition
for equilibrium between two phases at a fixed temperature and pressure.

Homework Equations





The Attempt at a Solution



1(a) S2-S1 = mC Integral form T1 to T2 of (dT/T) + Latent heat of transformation/373.15K

The latent heat wasn't given in the question so I'm wondering how to get around using it

1(b)

i was thinking of using S2-S1 = (1/T) integral from 1 to 2 of PdV but i can't figure how to eliminate the volume

1(c)
i don't have anything for this
 
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senan said:

Homework Statement



(1a) What are the total change in energy and entropy if 250 g of water at 20◦C is heated
and vaporised to yield 250 g of steam, all at atmospheric pressure?

(1b) Find the change in the entropy of 250 g of liquid water at its boiling point when it is
vaporised at a pressure of 8 atm. Give a brief physical explanation for how this entropy
change compares with the entropy change for vaporisation at 1 atm pressure.

(1c) We can allow for a possible transition between two phases of a substance by adding
the term +μdN in the fundamental thermodynamic relation for dE. Derive the condition
for equilibrium between two phases at a fixed temperature and pressure.

Homework Equations





The Attempt at a Solution



1(a) S2-S1 = mC Integral form T1 to T2 of (dT/T) + Latent heat of transformation/373.15K

The latent heat wasn't given in the question so I'm wondering how to get around using it

1(b)

i was thinking of using S2-S1 = (1/T) integral from 1 to 2 of PdV but i can't figure how to eliminate the volume

1(c)
i don't have anything for this
Is one familiar with steam tables in which properties such as specific enthalpy and specfic entropy are given as functions of pressure and temperature?

For water properties at 1 atm (1 bar) please see -
http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/phase.html#c1


In part a, the liquid is subcooled with respect to saturation conditions. The liquid must be increased from 20°C to 100°C, and then the liquid changes phase to vapor at constant pressure.
 
Welcome to PF, senan!

1(a). You're going to have to look up the enthalpy of vaporization (along with the heat capacity).

1(b). How about using the same equation as in 1(a), adjusted to the new conditions?

1(c). The fundamental statement of equilibrium is dS=0. Try to get there. Note that you'll have a \mu\,dN term for each phase, with dN_1=-dN_2 (because any matter that leaves one phase joins the other).
 

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