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Question: A body takes 10 minutes to cool from 60°C to 50°C. The temperature of the surroundings is constant a...

A body takes 10 minutes to cool from 60°C to 50°C. The temperature of the surroundings is constant at 25°C. Then, the temperature of the body after the next 10 minutes will be approximately
A. 43C43^\circ C
B. 47C47^\circ C
C. 41C41^\circ C
D. 45C45^\circ C

Explanation

Solution

Solution to this question will be determined by using Newton’s Law of Cooling. From the given values, we will determine the heat transfer coefficient. The next and final step will be to use the coefficient and the penultimate temperature change to find out the ultimate temperature of the given body.

Formula Used:
Newton’s Law of Cooling: dθdt=k(ΔT)=k(θ2θ0)\dfrac{{d\theta }}{{dt}} = k(\Delta T) = k(\dfrac{{\sum \theta }}{2} - {\theta _0})
Where θ\theta is the temperature of the body during instances of change and is expressed in Celsius (C)(^\circ C). It will be determined as θ1,θ2,θ3,θ0{\theta _1},{\theta _2},{\theta _3},{\theta _0} for the first, second, third and surrounding temperatures respectively. tt is the time period for the above temperature changes and t1,t2{t_1},{t_2} are the time periods for the first and second temperature changes. dtdt is the temperature change of the body and is expressed in Celsius (C)(^\circ C), dtdt is the time taken for those changes to occur and is expressed in minutes (min)(\min ) and kk is heat transfer coefficient.

Complete step by step answer:
We have the following given data:
θ1=60C{\theta _1} = 60^\circ C
θ2=50C{\theta _2} = 50^\circ C
θ0=25C{\theta _0} = 25^\circ C
t1=10min{t_1} = 10\min
t2=10min{t_2} = 10\min
As we can see, we need the value of kk to determine the final temperature change. Therefore using the given data in Newton’s Law of Cooling we get,
dθdt=k(ΔT)=k(θ2θ0) dθdt=k(θ2θ0)=k(60+50226) 605010=k(60+50226) k=129  \dfrac{{d\theta }}{{dt}} = k(\Delta T) = k(\dfrac{{\sum \theta }}{2} - {\theta _0}) \\\ \Rightarrow \dfrac{{d\theta }}{{dt}} = k(\dfrac{{\sum \theta }}{2} - {\theta _0}) = k(\dfrac{{60 + 50}}{2} - 26) \\\ \Rightarrow \dfrac{{60 - 50}}{{10}} = k(\dfrac{{60 + 50}}{2} - 26) \\\ \Rightarrow k = \dfrac{1}{{29}} \\\
Now that we have the value of kk, we can easily determine θ3{\theta _3}.
Again using Newton’s Law of Cooling and substituting the available data we get,
dθdt=k(ΔT)=k(θ2θ0) 50θ310=129(50+θ3226)=44.4117C θ345C  \dfrac{{d\theta }}{{dt}} = k(\Delta T) = k(\dfrac{{\sum \theta }}{2} - {\theta _0}) \\\ \Rightarrow \dfrac{{50 - {\theta _3}}}{{10}} = \dfrac{1}{{29}}(\dfrac{{50 + {\theta _3}}}{2} - 26) = 44.4117^\circ C \\\ \Rightarrow {\theta _3} \approx 45^\circ C \\\

In conclusion, the correct option is D.

Note: the temperature should not be approximated by stepping down. If its 44.4117C44.4117^\circ C, it is to be either stepped up or rounded off to 44C44^\circ C. Never should it be considered by stepping down to 43C43^\circ C.