Water of mass $m$ gram is slowly heated to increase the temperature from $T_1$ to $T_2$ The change in…
- $\mathrm{m} \ln \left(\frac{\mathrm{T}_2}{\mathrm{~T}_1}\right)$
- zero
- $\mathrm{m} \ln \left(\frac{\mathrm{T}_1}{\mathrm{~T}_2}\right)$
- $\mathrm{m}\left(\mathrm{T}_2-\mathrm{T}_1\right)$
Solution
\(\Delta S=\int_{T_1}^{T_2} \frac{d Q}{T}\)
Since the water is being heated slowly, the process is reversible, and the heat added is given by:
\(d Q=m c d T\)
where:
- \(m\) is the mass of the water,
- \(c\) is the specific heat capacity (given as \(1 \mathrm{~J} \mathrm{~kg}^{-1} \mathrm{~K}^{-1}\)).
Substitute \(d Q\) into the integral:
\(\Delta S=\int_{T_1}^{T_2} \frac{m c d T}{T}=m c \int_{T_1}^{T_2} \frac{d T}{T}\)
Since \(c=1\), the equation simplifies to:
\(\Delta S=m \int_{T_1}^{T_2} \frac{d T}{T}\)
Evaluating the integral, we have:
\(\int_{T_1}^{T_2} \frac{d T}{T}=\left.\ln T\right|_{T_1} ^{T_2}=\ln \left(\frac{T_2}{T_1}\right)\)
Thus, the change in entropy is:
\(\Delta S=m \ln \left(\frac{T_2}{T_1}\right)\)
Comparing with the options provided, the correct answer is:
Option 1: \(m \ln \left(\frac{T_2}{T_1}\right)\).
Asked in: JEE Main 2025 (23 Jan Shift 2)