The color seen depends on the thickness of the film and the wavelength of light. Typically, red is seen due to constructive interference for certain thicknesses.

At the center of the film with thickness λ/2, destructive interference occurs for all wavelengths, leading to no color.

The color that is most prominently visible depends on the thickness of the film and the wavelength of light. Typically, shorter wavelengths like blue are enhanced due to constructive interference.

Decreasing the slit width increases the diffraction angle, causing the diffraction pattern to become wider.

Fringe width (β) is inversely proportional to the distance to the screen (D). If D is halved, the fringe width decreases.

Increasing the slit width reduces the coherence of the light waves, leading to decreased fringe visibility.

Fringe separation is directly proportional to the wavelength; increasing the wavelength increases the fringe separation.

Fringe separation β = λD/d. Increasing λ increases β, hence fringe separation increases.

Fringe width β = λD/d = (500 x 10^-9 m)(1 m)/(0.2 x 10^-3 m) = 2.5 mm.

For the first order bright fringe, thickness t = λ/2 = 550 nm / 2 = 275 nm.

For constructive interference in a soap bubble, the minimum thickness t = λ/2 = 600 nm / 2 = 300 nm.

For constructive interference, the minimum thickness t = λ/2 = 550 nm / 2 = 275 nm.

A soap bubble appears black when the thickness is λ/4 due to destructive interference of light reflected from the top and bottom surfaces.

For destructive interference in reflected light, the minimum thickness t = λ/2n, where n is the refractive index (approximately 1.5 for soap). Thus, t = 600 nm / (2 * 1.5) = 200 nm.

For destructive interference in reflected light, the minimum thickness of the film must be λ/2.

In single-slit diffraction, the central maximum corresponds to m = 0, which is the first bright fringe.

Path difference = d sin θ = 1 m * sin(45°) = 1 m * √2/2 = 0.707 m.

Path difference = d sin θ = d sin(45°) = d(√2/2). For d = λ, path difference = √2λ.

The path difference for the first minimum is λ/2, which leads to destructive interference.

A phase difference of 180° corresponds to the waves being out of phase, leading to destructive interference.

Constructive interference occurs when the phase difference is an integer multiple of 2π, which corresponds to a phase difference of 0.

Destructive interference occurs when the phase difference is π radians (or an odd multiple of π).

The bending of light waves around the edges of an obstacle is known as diffraction.

The angle of diffraction is inversely proportional to the wavelength; as the wavelength increases, the angle of diffraction increases.

The angle of incidence and angle of diffraction are related by the grating equation d sin(θ) = mλ.

The width of the central maximum is inversely proportional to the slit width and directly proportional to the wavelength.

When light passes through a polarizer and then an analyzer at 90 degrees, no light passes through due to the orthogonal orientation.

A phase change of π (or half a wavelength) occurs upon reflection from a medium of higher refractive index, affecting the interference pattern.

Using d sin θ = mλ, λ = d sin θ/m. For m=1, d=0.1 mm, θ=30°, λ = 0.1 mm * sin(30°) = 0.1 mm * 0.5 = 0.05 mm = 500 nm.

Using d sin θ = mλ, λ = d sin θ/m. For m=1, d=0.1 mm, θ=30°, λ = 0.1 mm * sin(30°) = 0.1 mm * 0.5 = 0.05 mm = 0.2 mm.