The acceleration of the system is given by:
\[ a = \frac{m_2 - m_1}{m_1 + m_2} g \]
Given \(a = \frac{g}{\sqrt{2}}\), substitute in the equation:
\[ \frac{g}{\sqrt{2}} = \frac{m_2 - m_1}{m_1 + m_2} g \]
Simplifying:
\[ \frac{1}{\sqrt{2}} = \frac{m_2 - m_1}{m_1 + m_2} \]
Cross-multiplying:
\[ \sqrt{2}(m_2 - m_1) = m_1 + m_2 \]
Rearranging:
\[ m_1(\sqrt{2} + 1) = m_2(\sqrt{2} - 1) \]
The ratio of masses is:
\[ \frac{m_1}{m_2} = \frac{\sqrt{2} - 1}{\sqrt{2} + 1} \]
To solve this problem, we will analyze the motion of the two blocks connected by a string passing over a pulley. The masses of the blocks are \( m_1 \) and \( m_2 \) (where \( m_2 > m_1 \)), and the acceleration of the system is given as \( \frac{g}{\sqrt{2}} \).
Let's begin by applying Newton's second law to both masses:
Here, \( T \) is the tension in the string, and \( a = \frac{g}{\sqrt{2}} \) is the acceleration of the system.
From the two equations, we have:
Equating the two expressions for tension \( T \), we get:
\(m_1g + m_1a = m_2g - m_2a\)
Plug in the value of \( a = \frac{g}{\sqrt{2}} \) into the equation:
\(m_1g + m_1\left(\frac{g}{\sqrt{2}}\right) = m_2g - m_2\left(\frac{g}{\sqrt{2}}\right)\)
Simplify the equation:
\(g(m_1 + \frac{m_1}{\sqrt{2}}) = g(m_2 - \frac{m_2}{\sqrt{2}})\)
Cancel out the common factor \( g \):
\(m_1(1 + \frac{1}{\sqrt{2}}) = m_2(1 - \frac{1}{\sqrt{2}})\)
Rearrange to express the ratio of the masses:
\(\frac{m_1}{m_2} = \frac{1 - \frac{1}{\sqrt{2}}}{1 + \frac{1}{\sqrt{2}}}\)
Simplify the expression using the conjugate:
\(\frac{1 - \frac{1}{\sqrt{2}}}{1 + \frac{1}{\sqrt{2}}} \times \frac{\sqrt{2} - 1}{\sqrt{2} - 1} = \frac{(\sqrt{2} - 1)(1 - \frac{1}{\sqrt{2}})}{(\sqrt{2}^2 - 1^2)}\)
This simplifies to:
\(\frac{\sqrt{2} - 1}{\sqrt{2} + 1}\)
Thus, the correct option for the ratio \(\frac{m_1}{m_2}\) is:
\(\frac{\sqrt{2} - 1}{\sqrt{2} + 1}\)

Let the lines $L_1 : \vec r = \hat i + 2\hat j + 3\hat k + \lambda(2\hat i + 3\hat j + 4\hat k)$, $\lambda \in \mathbb{R}$ and $L_2 : \vec r = (4\hat i + \hat j) + \mu(5\hat i + + 2\hat j + \hat k)$, $\mu \in \mathbb{R}$ intersect at the point $R$. Let $P$ and $Q$ be the points lying on lines $L_1$ and $L_2$, respectively, such that $|PR|=\sqrt{29}$ and $|PQ|=\sqrt{\frac{47}{3}}$. If the point $P$ lies in the first octant, then $27(QR)^2$ is equal to}