4:5
3:2
In Young's double-slit experiment, two different light beams of wavelengths \(\lambda_1\) and \(\lambda_2\) produce interference patterns with band widths \(\beta_1\) and \(\beta_2\) respectively. We are given that the ratio between \(\beta_1\) and \(\beta_2\) is 3:2, and we need to find the ratio between \(\lambda_1\) and \(\lambda_2\).
The bandwidth (fringe width) \(\beta\) in Young's double-slit experiment is given by:
\(\beta = \frac{\lambda D}{d}\)
Where:
We are given that \(\frac{\beta_1}{\beta_2} = \frac{3}{2}\). We can write this as:
\(\frac{\beta_1}{\beta_2} = \frac{\frac{\lambda_1 D}{d}}{\frac{\lambda_2 D}{d}}\)
The terms \(D\) and \(d\) are the same for both wavelengths (since it's the same experimental setup), so they cancel out:
\(\frac{\beta_1}{\beta_2} = \frac{\lambda_1}{\lambda_2}\)
Since \(\frac{\beta_1}{\beta_2} = \frac{3}{2}\), we have:
\(\frac{\lambda_1}{\lambda_2} = \frac{3}{2}\)
The ratio between \(\lambda_1\) and \(\lambda_2\) is 3:2.
In Young's Double-Slit Experiment, the fringe width \( \beta \) of the interference pattern is given by the formula: \[ \beta = \frac{\lambda D}{d} \] where: - \( \lambda \) is the wavelength of the light used, - \( D \) is the distance between the slits and the screen, - \( d \) is the distance between the two slits.
Suppose two light sources with different wavelengths \( \lambda_1 \) and \( \lambda_2 \) produce fringe widths \( \beta_1 \) and \( \beta_2 \) respectively. Then, \[ \beta_1 = \frac{\lambda_1 D}{d}, \quad \beta_2 = \frac{\lambda_2 D}{d} \]
Now taking the ratio of the two fringe widths: \[ \frac{\beta_1}{\beta_2} = \frac{\lambda_1 D / d}{\lambda_2 D / d} = \frac{\lambda_1}{\lambda_2} \] This implies: \[ \frac{\beta_1}{\beta_2} = \frac{\lambda_1}{\lambda_2} \]
Given: \[ \frac{\beta_1}{\beta_2} = \frac{3}{2} \Rightarrow \frac{\lambda_1}{\lambda_2} = \frac{3}{2} \]
Final Answer: \( \boxed{3:2} \)
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