The fringe width (\( \beta \)) in a double-slit experiment is given by: \[ \beta = \frac{\lambda D}{d}, \] where: - \( \lambda \) is the wavelength of the light, - \( D \) is the distance between the slits and the screen, - \( d \) is the separation between the slits.
Step 1: Relation between fringe widths. Since \( D \) and \( d \) are constant, the fringe width \( \beta \) is directly proportional to \( \lambda \): \[ \beta \propto \lambda. \]
Step 2: Calculate the new fringe width. Let the initial fringe width (\( \beta_1 \)) correspond to \( \lambda_1 = 400 \, \text{nm} \) and the new fringe width (\( \beta_2 \)) correspond to \( \lambda_2 = 600 \, \text{nm} \). Then: \[ \frac{\beta_2}{\beta_1} = \frac{\lambda_2}{\lambda_1}. \] Substituting \( \beta_1 = 2 \, \text{mm} \), \( \lambda_1 = 400 \, \text{nm} \), and \( \lambda_2 = 600 \, \text{nm} \): \[ \frac{\beta_2}{2} = \frac{600}{400} \implies \beta_2 = 2 \cdot 1.5 = 3 \, \text{mm}. \]
Final Answer: The fringe width for \( \lambda = 600 \, \text{nm} \) is: \[ \boxed{3 \, \text{mm}}. \]
A sub-atomic particle of mass \( 10^{-30} \) kg is moving with a velocity of \( 2.21 \times 10^6 \) m/s. Under the matter wave consideration, the particle will behave closely like (h = \( 6.63 \times 10^{-34} \) J.s)