In Young's double slit experiment, the \(10^{th}\) maximum of wavelength \(\lambda_1\) is at a distance \(y_1\) from the central maximum. When the wavelength of the source is changed to \(\lambda_2\), the \(5^{th}\) maximum is at a distance of \(y_2\) from the central maximum. The ratio \(\left(\dfrac{y_1}{y_2}\right)\) is