Change in entropy when mixing cold and hot water

Click For Summary

Homework Help Overview

The discussion revolves around calculating the change in entropy when mixing hot and cold water, focusing on the thermodynamic principles involved in entropy changes during heat transfer. The subject area includes concepts from thermodynamics and statistical mechanics.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the expression for total entropy change and question the correctness of specific calculations. There is an attempt to integrate the expression for entropy change and express heat transfer in terms of temperature changes. Some participants raise questions about the integration process and the treatment of specific heat as a constant.

Discussion Status

Participants are actively engaging with the problem, discussing various approaches to calculating entropy change. Some have identified potential errors in previous calculations and are working through the integration process. There is no explicit consensus yet, but productive dialogue is occurring regarding the correct formulation of the equations involved.

Contextual Notes

Participants note issues with missing coefficients and the need for careful attention to signs in the equations. The discussion also highlights the complexity of integrating temperature-dependent variables in the context of entropy changes.

tuki
Messages
19
Reaction score
1
Homework Statement
1.00 kg of hot water (T = 100 celcius) and 1.00 kg of cold water (T = 0 celcius) are mixed in bowl. It results in 2.00kg of water which temperature is 50 Celcius. Calculate the whole systems change in entropy.
Relevant Equations
Change in entropy:
$$ dS = \frac{dQ}{T} $$
Heat capacity:
$$ Q = Cm\Delta T $$
I tried following:

$$ dS_{\text{total}} = |\frac{dQ}{T_c}| |\frac{dQ}{T_H}| $$

where ## T_h ## is temperature of hot water and ## T_c ## is temperature of cold water. Coefficient for water wasn't provided in the assignment so i used following value c = 4190 J/kgK.

$$ dS_{\text{total}} = |\frac{cm\Delta T}{T_c}| - |\frac{cm\Delta T}{T_h}| $$

where ## dQ = cm\Delta T = 4190 \text{ J/kgK} \cdot 1 \text{ kg} \cdot 50 \text{ K} ##

my result for change in entropy is:

$$ dS \approx 205 \text{ J/K} $$

However the correct answer should be:

$$ dS \approx 102 \text{ J/K} $$
 
Physics news on Phys.org
tuki said:
$$ dS_{\text{total}} = |\frac{cm\Delta T}{T_c}| - |\frac{cm\Delta T}{T_h}| $$
The expression ## |\frac{cm\Delta T}{T_c}|## is not the correct way to calculate the entropy change of the cold water. Can you see how to do this correctly by integrating the expression ##dS = \frac{dQ}{T}##?
 
TSny said:
The expression ## |\frac{cm\Delta T}{T_c}|## is not the correct way to calculate the entropy change of the cold water. Can you see how to do this correctly by integrating the expression ##dS = \frac{dQ}{T}##?

$$ S = \int \frac{1}{T}dQ $$

but what from now?

this equation has ## \Delta T ## but not T
$$ Q = cm \Delta T $$

I think I want ## T(Q) ## so I can integrate this properly?
 
tuki said:
$$ S = \int \frac{1}{T}dQ $$
Can you express ##dQ## in terms of ##dT##?
 
Well

$$ T = \frac{dQ}{dS} \implies dT = d(\frac{dQ}{dS}) $$

Not quite sure how I would do this? (this one probably not even in right direction)
 
Express ##\Delta Q = mc \Delta T## in infinitesimal form.
##dQ = ?##
 
## dQ = mcdT ## ?
 
Right. So, ##\int \frac{dQ}{T} = ?##
 
## \int \frac{dQ}{T} = \int \frac{mc}{T}dT ## ?
 
  • #10
tuki said:
## \int \frac{dQ}{T} = \int \frac{mc}{T}dT ## ?
Yes. When you put appropriate limits on the integral, it will represent the change in entropy ##\Delta S## for the cold water. Deal with the hot water in a similar way.

In doing the integrals, you can treat the specific heat ##c## as a constant (independent of temperature) to a good approximation.
 
  • #11
So then i have:

$$ \Delta S = \int_{T_0}^{T_1} \frac{cm}{T}dT = cm(ln(T_1)-ln(T_0)) $$

now when i compute ##\Delta S## for cold and hot

$$ \Delta S_{\text{total}} = cm(ln(T_n)-ln(T_H)+ln(T_c)-ln(T_n)) = cm(ln(T_c)-ln(T_h)) $$

Where ## T_n ## is temperature at balanced state. Now ##\Delta S_{\text{total}} ## gives wrong result

$$ \Delta S_{\text{total}} \approx -1307 \text{ J/kg} $$

Units seems to be off too.
 
  • #12
tuki said:
So then i have:

$$ \Delta S = \int_{T_0}^{T_1} \frac{cm}{T}dT = cm(ln(T_1)-ln(T_0)) $$

now when i compute ##\Delta S## for cold and hot

$$ \Delta S_{\text{total}} = cm(ln(T_n)-ln(T_H)+ln(T_c)-ln(T_n)) = cm(ln(T_c)-ln(T_h)) $$

Where ## T_n ## is temperature at balanced state. Now ##\Delta S_{\text{total}} ## gives wrong result

$$ \Delta S_{\text{total}} \approx -1307 \text{ J/kg} $$

Units seems to be off too.
The equation should read:
$$ \Delta S_{\text{total}} = cm(ln(T_n)-ln(T_H)-ln(T_c)+ln(T_n))$$
(check the signs)

For a straightforward step-by-step cookbook recipe on how to determine the change in entropy of a system that experiences and irreversible process, see the following Physics Forums Insights article: https://www.physicsforums.com/insights/grandpa-chets-entropy-recipe/
 
  • #13
tuki said:
So then i have:

$$ \Delta S = \int_{T_0}^{T_1} \frac{cm}{T}dT = cm(ln(T_1)-ln(T_0)) $$
OK. ##T_0## is intial temperature and ##T_1## is final temperature.

now when i compute ##\Delta S## for cold and hot

$$ \Delta S_{\text{total}} = cm(ln(T_n)-ln(T_H)+ln(T_c)-ln(T_n)) = cm(ln(T_c)-ln(T_h)) $$
You have two sign errors in the middle expression (as pointed out by @Chestermiller).
 

Similar threads

  • · Replies 5 ·
Replies
5
Views
2K
Replies
12
Views
1K
  • · Replies 7 ·
Replies
7
Views
1K
  • · Replies 6 ·
Replies
6
Views
1K
  • · Replies 10 ·
Replies
10
Views
3K
Replies
18
Views
3K
Replies
14
Views
1K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 4 ·
Replies
4
Views
4K
  • · Replies 4 ·
Replies
4
Views
2K