To solve this, we need to calculate the entropy changes for both the free expansion and the isothermal expansion.
Step 1: Entropy Change for Free Expansion (\( \Delta S_1 \))
For free expansion, the process is irreversible, and since the gas expands into a vacuum, there is no heat exchange with the surroundings. Therefore, the entropy change \( \Delta S_1 \) for the gas during free expansion is given by: \[ \Delta S_1 = nR \ln \left( \frac{V_f}{V_i} \right), \] where \( V_f \) and \( V_i \) are the final and initial volumes of the gas, respectively, and \( n \) is the number of moles. Since the volume doubles, \( \frac{V_f}{V_i} = 2 \), and we get: \[ \Delta S_1 = nR \ln(2). \] Step 2: Entropy Change for Isothermal Expansion (\( \Delta S_2 \))
For the isothermal expansion, the process is reversible, and the gas is at a constant temperature. The entropy change \( \Delta S_2 \) for the gas during an isothermal expansion is given by: \[ \Delta S_2 = nR \ln \left( \frac{V_f}{V_i} \right), \] where \( V_f \) and \( V_i \) are the final and initial volumes of the gas, respectively. Since the volume also doubles in this case, \( \frac{V_f}{V_i} = 2 \), and we get: \[ \Delta S_2 = nR \ln(2). \] Step 3: Comparing the Two Entropy Changes.
We are asked to find the ratio \( \frac{\Delta S_1}{\Delta S_2} \). Since both entropy changes are equal: \[ \frac{\Delta S_1}{\Delta S_2} = \frac{nR \ln(2)}{nR \ln(2)} = 1. \] Thus, the value of \( \frac{\Delta S_1}{\Delta S_2} \) is \( 1 \).
Which of the following best represents the temperature versus heat supplied graph for water, in the range of \(-20^\circ\text{C}\) to \(120^\circ\text{C}\)? 