To solve this problem, we start by considering the mixture of two ideal monoatomic gases at equilibrium. Given gases 1 and 2 have equal proportions, their number of moles are the same, i.e., \(n_1 = n_2\).
The problem states that the atomic masses are \(m\) and \(2m\) respectively. The root mean square (\(rms\)) speed \(v_{\text{rms}}\) of gas molecules is determined using the equation:
\[v_{\text{rms}} = \sqrt{\frac{3k_BT}{m_i}}\]
where \(k_B\) is the Boltzmann constant, \(T\) is the temperature, and \(m_i\) is the mass of the gas particle. For gas 1, the \(rms\) speed is:
\[v_{1,\text{rms}} = \sqrt{\frac{3k_BT}{m}}\]
And for gas 2, it is:
\[v_{2,\text{rms}} = \sqrt{\frac{3k_BT}{2m}}\]
Given both gases are in equal proportion, the average \(rms\) speed \(V_{\text{rms}}\) for a randomly selected molecule is:
\[V_{\text{rms}} = \sqrt{\frac{v_{1,\text{rms}}^2 + v_{2,\text{rms}}^2}{2}}\]
Substituting the values:
\[V_{\text{rms}} = \sqrt{\frac{\left(\frac{3k_BT}{m}\right) + \left(\frac{3k_BT}{2m}\right)}{2}}\]
\[= \sqrt{\frac{3k_BT(1 + \frac{1}{2})}{2m}}\]
\[= \sqrt{\frac{3k_BT \cdot 1.5}{2m}}\]
\[= \sqrt{\frac{4.5k_BT}{2m}} = \sqrt{\frac{2.25k_BT}{m}}\]
Thus the expression for \(V_{\text{rms}}\) simplifies to:
\[V_{\text{rms}} = \sqrt{\frac{9}{4} \cdot \frac{k_BT}{m}} = \frac{3}{2}\sqrt{\frac{k_BT}{m}}\]
Therefore, \(x = \frac{3}{2} = 1.5\). This calculated value falls within the specified range of 1.57.