To solve this problem, we need to make use of the adiabatic process relation for an ideal monoatomic gas. In an adiabatic process, the relationship between pressure and volume is given by:
\(P_1 V_1^\gamma = P_2 V_2^\gamma\)
Where:
From the problem, the gas is compressed to \(\left(\frac{1}{8}\right)^{\text{th}}\) of its initial volume. Thus, we have:
Substituting the values into the adiabatic equation, we get:
\(P_1 V_1^{\frac{5}{3}} = P_2 \left(\frac{V_1}{8}\right)^{\frac{5}{3}}\)
We can simplify this equation as follows:
\(P_1 V_1^{\frac{5}{3}} = P_2 \cdot \frac{V_1^{\frac{5}{3}}}{8^{\frac{5}{3}}}\)
\(P_1 = P_2 \cdot \frac{1}{8^{\frac{5}{3}}}\)
Rearranging for \(\frac{P_2}{P_1}\), we get:
\(\frac{P_2}{P_1} = 8^{\frac{5}{3}}\)
Calculating the value of \(8^{\frac{5}{3}}\):
\(8 = 2^3\), so \(8^{\frac{5}{3}} = (2^3)^{\frac{5}{3}} = 2^5 = 32\)
Therefore, the ratio of final pressure to initial pressure is 32.
Hence, the correct answer is 32.
A Wheatstone bridge is initially at room temperature and all arms of the bridge have same value of resistances \[ (R_1=R_2=R_3=R_4). \] When \(R_3\) resistance is heated, its resistance value increases by \(10%\). The potential difference \((V_a-V_b)\) after \(R_3\) is heated is _______ V. 