For an adiabatic process, the work done \( W \) is given by:
\[ W = \frac{nR\Delta T}{1-\gamma}. \]
1. **Using the Adiabatic Condition:**
Since the process is adiabatic, \( TV^{\gamma-1} = \text{constant} \). Let the initial temperature be \( T \) and the final temperature be \( T_f \) when the volume is doubled. Thus,
\[ TV^{\gamma-1} = T_f(2V)^{\gamma-1}. \]
2. **Calculate \( T_f \):**
Simplifying, we get:
\[ T_f = T \left(\frac{1}{2}\right)^{\frac{\gamma-1}{\gamma}} = T \left(\frac{1}{2}\right)^{\frac{1}{2}} = \frac{T}{\sqrt{2}}. \]
3. **Calculate the Work Done:**
Substitute into the work formula:
\[ W = \frac{R(T - T_f)}{1 - \frac{3}{2}} = \frac{R \left( T - \frac{T}{\sqrt{2}} \right)}{-\frac{1}{2}}. \] Simplifying further:
\[ W = 2RT\frac{\left(\sqrt{2} - 1\right)}{\sqrt{2}} = RT(2 - \sqrt{2}). \] **Answer:** \( RT(2 - \sqrt{2}) \)
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is: