Step 1: In single-slit diffraction, the condition for the \( m \)-th diffraction minimum is given by:
\[ a \sin \theta_m = m\lambda, \]
where \( a \) is the width of the slit, \( \lambda \) is the wavelength of light, and \( m \) is the diffraction order.
Step 2: For the 2nd order minimum of \( \lambda_1 \) and the 3rd order minimum of \( \lambda_2 \), we can set the angle for both minima equal since they coincide:
\[ 2\lambda_1 = 3\lambda_2 \]
Thus:
\[ \frac{\lambda_1}{\lambda_2} = \frac{3}{2}. \]

A quantity \( X \) is given by: \[ X = \frac{\epsilon_0 L \Delta V}{\Delta t} \] where:
- \( \epsilon_0 \) is the permittivity of free space,
- \( L \) is the length,
- \( \Delta V \) is the potential difference,
- \( \Delta t \) is the time interval.
The dimension of \( X \) is the same as that of: