Using the condition for the first minimum a sin(30°) = λ, we find the ratio a/λ = 1/√3.

The intensity of the central maximum is theoretically infinite compared to the first minimum, which has zero intensity.

The intensity of the central maximum in a diffraction pattern is at its maximum compared to other maxima.

The intensity of the central maximum in a diffraction pattern depends on both the wavelength of light and the slit width.

Fringe separation refers to the distance between two consecutive maxima in a diffraction pattern.

The order of diffraction refers to the number of maxima observed in the diffraction pattern, with the central maximum being the zeroth order.

Increasing the slit width results in a wider central maximum due to the decrease in diffraction effects.

The intensity of the central maximum is typically much greater than that of the first minimum, often approximated as 1:4.

Bit rate refers to the number of bits transmitted per second in a digital communication system.

The depletion region in a diode is the area where no charge carriers are present.

The depletion region is the area in a diode where no current flows under reverse bias.

Using the lens maker's formula, f = (R1 * R2) / (n - 1) * (1/R1 - 1/R2), we find f = 12 cm.

Fringe separation is directly proportional to the distance from the slits to the screen; increasing this distance increases fringe separation.

Fringe width β = λD/d = (600 x 10^-9 m)(1 m)/(0.2 x 10^-3 m) = 0.003 m = 0.6 mm.

Distance between fringes = β = λD/d. For first and second bright fringes, the distance is 2β.

Using the formula for fringe separation, y = (λD)/d, we find y = (500 x 10^-9 m * 2 m) / (0.5 x 10^-3 m) = 2 cm.

Fringe width (β) is given by β = λD/d, where d is the distance between the slits. If d is doubled, β is halved.

Fringe width (β) is inversely proportional to the distance between the slits (d). If d is doubled, β is halved.

The fringe separation is inversely proportional to the distance between the slits; thus, if the distance is doubled, the fringe separation halves.

Fringe width (β) is given by β = λD/d, where d is the distance between the slits. If d is doubled, β becomes β/2, hence the fringe width halves.

The fringe separation is inversely proportional to the distance between the slits; halving the distance doubles the fringe separation.

Increasing the distance between the slits (d) causes the fringe width (β) to decrease, making the fringes narrower.

Increasing the distance between the slits decreases the fringe width, which can lead to more visible fringes within a given distance on the screen.

Fringe separation is directly proportional to the distance from the slits to the screen (D), so increasing D increases the fringe separation.

Increasing the distance to the screen increases the fringe width, as fringe width is proportional to the distance from the slits.

Increasing the distance to the screen increases the fringe width, as fringe width is proportional to the distance from the slits.

At the first minimum, the intensity is 0 due to destructive interference.

Fringe separation is directly proportional to the distance from the slits to the screen (D), hence it increases.

Moving the screen further away increases the distance (D) in the fringe width formula, causing the fringes to become wider.

Moving the screen further away increases the fringe spacing, as fringe width is directly proportional to the distance from the slits.