Solving a 0.5kg Copper Heat Transfer Problem

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SUMMARY

The discussion focuses on solving a heat transfer problem involving a 0.5kg mass of copper at 600K and a litre of water at 20°C. The equilibrium temperature, T2, is calculated to be 336K (63°C) using the heat transfer equation where the heat lost by copper equals the heat gained by water. The change in entropy for the water is determined to be 575 J K-1 using the formula ∆S=C ln(T2/T1). The confusion arises regarding the calculation of entropy changes in different heating scenarios, particularly the distinction between isothermal and non-isothermal processes.

PREREQUISITES
  • Understanding of heat transfer principles, specifically the concept of heat exchange between substances.
  • Familiarity with specific heat capacity, particularly for copper (385 J kg-1K-1) and water (4200 J kg-1K-1).
  • Knowledge of entropy and its calculation using the formula ∆S=C ln(T2/T1).
  • Basic thermodynamics, including the distinction between isothermal and non-isothermal processes.
NEXT STEPS
  • Study the principles of heat transfer and the equations governing thermal equilibrium.
  • Learn about the calculation of entropy changes in both isothermal and non-isothermal processes.
  • Explore the implications of phase changes on entropy, particularly in the context of boiling and condensation.
  • Investigate the specific heat capacities of various materials to compare thermal properties.
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Students in thermodynamics, physics enthusiasts, and anyone studying heat transfer and entropy calculations in thermal systems.

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Homework Statement



(a) A 0.5kg mass of copper (specific heat 385 J kg-1K-1) at 600K is plunged into a litre of water at 20C. What is the equilibrium temperature, T2, of the system? What is the change in entropy of the water?
(b) A litre of water is heated slowly at a constant rate from 20C to T2. What is the change in entropy?
How do you account for the difference between (a) and (b)?


Homework Equations


not totally sure


The Attempt at a Solution



(a) ∆T_water=T_2-T_1=T_2-293 so ∆Q_water=C ∆T=〖4200 (T〗_2-293)

∆T_copper=T_2-T_1=T_2-600 so ∆Q_copper=C ∆T=〖385/2 (T〗_2-600)

Heat lost by copper is heat gained by water so ∆Q_water= ∆Q_copper so

〖4200 (T〗_2-293)=〖385/2 (T〗_2-600) => T_2=336K=63 degrees Centigrade

This is not an isothermal process so cannot use S=Q/T to calculate entropy before and after to calculate entropy difference.
Instead, use ∆S=C ln⁡〖T_2/T_1 〗 so ∆S=4200 ln⁡〖336/293=575 J K^(-1) 〗
However, if I treat it like an isothermal process, where
∆Q=4200 (336-293)=4200×43=180600 Joules
Then ∆S=∆Q/T=180600/293=616 J K^(-1)
The extra entropy gained could be because some of the water has turned to steam.

Please could somebody tell me what I am doing right, how I should calculate the entropy differently for part a and part b, and why, as I am very confused!

Many thanks :)
 
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Entropy is a state variable, dependent only pressure, temperature, and amount of material. I'm having a hard time seeing why the entropy change of water between 20°C and some arbitrary temperature T_2 could be path dependent, even if some quantity has boiled and recondensed.
 
Many thanks - yuor logic makes sense to me so I don't know what the question is trying to get at.
 

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