For an isothermal and reversible expansion, the work done is given by:
\[ W = nRT \ln \left( \frac{V_f}{V_i} \right) \]where:
Rewriting the equation:
\[ T = \frac{W}{nR \ln \left( \frac{V_f}{V_i} \right)} \] Step 3: Substituting the values. \[ T = \frac{1728.85}{1 \cdot 8.314 \cdot 0.693} \] \[ T = \frac{1728.85}{5.755522} \] \[ T \approx 300.48 \, \text{K} \] Step 4: Conclusion.The temperature of the system is approximately \( 300.48 \, \text{K} \), which lies between \( 299.90 \, \text{K} \) and \( 301.90 \, \text{K} \).
[A] | [B] | [C] | Rate (M/sec.) |
---|---|---|---|
0.2 | 0.1 | 0.02 | 8.08 × 10-3 |
0.1 | 0.2 | 0.02 | 2.01 × 10-3 |
0.1 | 1.8 | 0.18 | 6.03 × 10-3 |
0.2 | 0.1 | 0.08 | 6.464 × 10-2 |