To solve this problem, we need to use the relationship for adiabatic processes in ideal gases, given by the equation:
\(P_1 V_1^\gamma = P_2 V_2^\gamma\)
where:
We can rearrange this equation to find the ratio of initial pressure to final pressure:
\(\frac{P_1}{P_2} = \left(\frac{V_2}{V_1}\right)^\gamma\)
Substituting the given values \(V_1 = 5\, \text{litres}\) and \(V_2 = 4\, \text{litres}\):
\(\frac{P_1}{P_2} = \left(\frac{4}{5}\right)^{1.5}\)
Calculating \(\left(\frac{4}{5}\right)^{1.5}\):
\(\left(\frac{4}{5}\right)^{1.5} = \left(\frac{4}{5}\right) \times \sqrt{\left(\frac{4}{5}\right)} = \frac{4}{5} \times \frac{2}{\sqrt{5}} = \frac{8}{5\sqrt{5}}\)
Thus, the ratio of initial pressure to final pressure is:
\(\frac{8}{5\sqrt{5}}\)
Hence, the correct answer is \(\frac{8}{5\sqrt{5}}\).
For an adiabatic process, the relation between pressure and volume is:
\[ P_iV_i^\gamma = P_fV_f^\gamma, \] where \(\gamma = 1.5\).
Substitute the given volumes (\(V_i = 5 \, \text{litres}, V_f = 4 \, \text{litres}\)):
\[ P_i (5)^{1.5} = P_f (4)^{1.5}. \]
Rearranging for \(\frac{P_i}{P_f}\):
\[ \frac{P_i}{P_f} = \frac{(4)^{1.5}}{(5)^{1.5}}. \]
Simplify:
\[ \frac{P_i}{P_f} = \left(\frac{4}{5}\right)^{1.5}. \]
Write \(1.5\) as \(\frac{3}{2}\):
\[ \frac{P_i}{P_f} = \left(\frac{4}{5}\right)^{\frac{3}{2}} = \left(\frac{4}{5}\right)^1 \times \left(\frac{4}{5}\right)^{\frac{1}{2}}. \]
Simplify each term:
\[ \frac{P_i}{P_f} = \frac{4}{5} \times \sqrt{\frac{4}{5}} = \frac{4}{5} \times \frac{2}{\sqrt{5}} = \frac{8}{5\sqrt{5}}. \]
Final Answer: \(\frac{8}{5\sqrt{5}}\).
The equivalent resistance between the points \(A\) and \(B\) in the given circuit is \[ \frac{x}{5}\,\Omega. \] Find the value of \(x\). 
Method used for separation of mixture of products (B and C) obtained in the following reaction is: 
In the following \(p\text{–}V\) diagram, the equation of state along the curved path is given by \[ (V-2)^2 = 4ap, \] where \(a\) is a constant. The total work done in the closed path is: 