Change in entropy when mixing cold and hot water

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tuki
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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:

$$ dS \approx 102 \text{ J/K} $$
 
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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?
 
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)
 
## \int \frac{dQ}{T} = \int \frac{mc}{T}dT ## ?
 
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.
 
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.
 
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/
 
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).