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Question: Hot coffee in a mug cools from \(90^{\circ}\)C to \(70^{\circ}\)C in 4.8 minutes. The room temperatu...

Hot coffee in a mug cools from 9090^{\circ}C to 7070^{\circ}C in 4.8 minutes. The room temperature is 2020^{\circ}C. Applying newton’s law of cooling the time needed to cool it further by 1010^{\circ}C should be nearly:
A. 4.2 min
B. 3.8 min
C. 3.2 min
D. 2.4 min

Explanation

Solution

Newton was the first successful person to compute the relation between temperature variation and time. However his thesis were limited only for some special type of system in which certain assumptions were made. The assumptions made so that the law is valid are that the temperature difference of the body must not be very large and the time of consideration of the variation also must be small. This law is called Newton’s law of cooling.
Formula used:
TfTit=α(TsTavg)\dfrac{T_f-T_i}t = \alpha\left( T_s - T_{avg} \right)

Complete answer:
Since we are given here that the law is applicable, hence we can use Newton's law of cooling. Hence using: TfTit=α(TsTavg)\dfrac{T_f-T_i}t = \alpha\left( T_s - T_{avg} \right) where Tf,Ti and TsT_f, T_i \ and \ T_sare the final, initial and surrounding temperature with respect to the body. Also, Tavg=(Tf+Ti)2 and αT_{avg} = \dfrac{(T_f+T_i)}2 \ and \ \alphais a constant.
Given (Case I): Tf=70, Ti=90, t=4.8 min and Ts=20T_f = 70^{\circ},\ T_i = 90^{\circ},\ t = 4.8 \ min \ and \ T_s = 20^{\circ}
Thus;
70904.8=α(2090+702)\dfrac{70-90}{4.8} = \alpha\left( 20 - \dfrac{90+70}{2} \right)
    α=204.8×60=114.4\implies \alpha = \dfrac{20}{4.8\times 60} = \dfrac{1}{14.4}
Now, for the second case:
TfTit=α(TsTavg)\dfrac{T_f-T_i}t = \alpha\left( T_s - T_{avg} \right)
6070t=114.4(2070+602)\dfrac{60-70}{t} = \dfrac{1}{14.4}\left( 20 - \dfrac{70+60}{2}\right)
    t=14445=3.2 min\implies t = \dfrac{-144}{-45} = 3.2\ min

So, the correct answer is “Option C”.

Note:
It should be noted that this form of Newton’s law of cooling is the most approximate form of the law. Important point to be remembered using it is that the time and temperature difference must not vary by a certain amount i.e. should be small. If we want to calculate the temperature over a longer period of time and to any value of temperature, one can use Stephen-Boltzmann’s law.

Also α\alpha is a constant in this equation. But actually it depends upon certain factors. In fact α=4σeAT3ms\alpha =\dfrac{ 4\sigma eAT_{\circ}^3}{ms} [where symbols have its usual meaning ]depends upon the surrounding temperature also. So alpha is constant only till the medium is not changed.