How Is Entropy Change Calculated in a Heat Transfer Problem?

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SUMMARY

The entropy change in a heat transfer problem involving a solid metallic cube with heat capacity S at 300K brought into contact with a reservoir at 600K is calculated to be 0.19S. The relevant equations include Q = SΔT and the change in entropy dS = dqrev/T. The solution requires integrating the entropy change over the temperature range for the block and applying the principle of energy conservation to find the heat exchanged with the reservoir. The final entropy change of the universe is the sum of the entropy changes of both the block and the reservoir.

PREREQUISITES
  • Understanding of thermodynamic principles, specifically heat transfer and entropy.
  • Familiarity with the equations Q = SΔT and dS = dqrev/T.
  • Knowledge of thermal equilibrium concepts.
  • Ability to perform integration in the context of thermodynamic processes.
NEXT STEPS
  • Study the integration of entropy change in thermodynamic systems.
  • Learn about the concept of heat capacity and its implications in heat transfer problems.
  • Explore energy conservation principles in thermodynamic processes.
  • Investigate the role of thermal reservoirs in heat transfer scenarios.
USEFUL FOR

Students studying thermodynamics, particularly those tackling heat transfer problems and entropy calculations, as well as educators preparing coursework in this area.

astrophysics12
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Homework Statement


A solid metallic cube of heat capacity S is at temperature 300K. It is brought in contact with a reservoir at 600K. If the heat transfer takes place only between the reservoir and the cube, the entropy change of the universe after reaching the thermal equillibrium is

A. 0.69S
B. 0.54S
C. 0.27S
D. 0.19S

[Answer : 0.19S]

Homework Equations


(heat supplied)=SΔT

Q = SΔT

Change in entropy = (change in heat Q)/T

ΔE = Q/T

[I have taken entropy as E rather than usual S since S is already taken for heat capacity]

The Attempt at a Solution


[/B]
Should I take reservoir as an infinite pool of temperature? Then, I get

Q = SΔT
Q=S*(600-300) since, at thermal equillibrium the temperatures are same
Q=300S
ΔE=(300/600)=0.5 which is not the answer

If I take reservoir which loses temperature, I am unable to continue with the problem since I do not know the heat capacity of it.

Is there a different approach to this problem?
 
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astrophysics12 said:

Homework Statement


A solid metallic cube of heat capacity S is at temperature 300K. It is brought in contact with a reservoir at 600K. If the heat transfer takes place only between the reservoir and the cube, the entropy change of the universe after reaching the thermal equillibrium is

A. 0.69S
B. 0.54S
C. 0.27S
D. 0.19S

[Answer : 0.19S]

Homework Equations


(heat supplied)=SΔT

Q = SΔT

Change in entropy = (change in heat Q)/T

ΔE = Q/T

[I have taken entropy as E rather than usual S since S is already taken for heat capacity]

The Attempt at a Solution


[/B]
Should I take reservoir as an infinite pool of temperature? Then, I get

Q = SΔT
Q=S*(600-300) since, at thermal equillibrium the temperatures are same
Q=300S
ΔE=(300/600)=0.5 which is not the answer

If I take reservoir which loses temperature, I am unable to continue with the problem since I do not know the heat capacity of it.

Is there a different approach to this problem?

Bits are right, but a lot of what you have is incorrect.

BTW this is a HORRIBLE problem -- it seems like the person who wrote the problem is trying to confuse you with the heat capacity = "S' garbage.

dS = dqrev/T

For the block, to calculate Delta S, you will need to integrate the above over the temperature range.

For the bath, assuming that the bath has a huge heat capacity, and does not change temperature (T is constant), then Delta S bath = Qbath/T

To find Qbath, you need to find Qblock (Qbath = - Qblock -- energy is conserved). Qblock can be found from "S" Delta T, as you have noted.

Delta S Universe = Delta S block + Delta S bath
 
Thanks a lot. I got it.

This is actually from a question paper that I was practicing.
 

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