# Optics Series Lecture, Lecture – XI.

**“Fresnel’s Bi-prism: measurement of wavelength of light by it.”** This lecture was delivered on 16th February in a lecture session of **1** and **1/2** hours. This lecture was delivered to Physics elective students and later to honors students. This web-version does not strictly pertain to 1 and 1/2 hours of regular lecturing session that we have mostly been employing.

That’s because it was created with another part which can be optionally appended to other related subject matter. In this web-version that’s what we will do. Our guiding principle is more in line with the honors course, where the subject matter is quite extensive and deep which brings more flexibility and choices into the lecture compositions.

Today we will discuss another interesting interference set-up, now that we have discussed the **Young’s double slit experiment**, in **lecture – IX**. A few words about the general mechanism behind interference. There are two kinds of interference basically that we will be discussing in our lectures. We discussed the Young’s DS interference pattern based on our understandings of intensity or irradiance patterns that we studied here: **lecture – VII**.

Interference is sustained and visible if the corresponding sources of light are coherent among themselves, that is, if the sources have phase differences that are not arbitrarily or abruptly changing, as a consequence we can safely assume the phase differences are constant and therefore predictable. Incoherent light makes this impossible.

Incoherent light is that light source whose production itself is arbitrary and abrupt and unpredictable, hence nothing can be definitively said on its phase, as a result the coherence is only short lived. If two light sources are so generated that their respective coherence time (or coherence length) are well within each others span, they are said to be coherent light.

Recall the idea of temporal and spatial coherence here that we discussed: **here**, when we discussed Young’s DS interference. We observe one basic thing about interference here. The two coherent sources **S _{1}** and

**S**that we considered give rise to two different wave-fronts that meet up after traversing their respective optical paths. When they meet they produce interference. For this reason such type of interference are called as wave-front splitting interference.

_{2}Young’s DS experiment is an example of wave-front splitting interference. The Fresnel bi-prism that we will discuss is also an example of wave-front splitting interference. But there is yet another type of interference mechanism. Its called amplitude-splitting interference, examples of which are colors of thin films and Newton’s ring phenomena which we will study soon enough in future lectures.

In an amplitude splitting interference what happens is there is only one wave (or its wave-fronts) which splits into different components such as reflected or transmitted (refracted) parts according to the respective coefficients for these processes. So the amplitude has a fraction which is reflected and another which is refracted.

Naturally the question of coherence does not deter the production of interference effects. There always is inherent coherence in the amplitude splitting processes. When these different components meet up later, they produce interference.

## Fresnel’s Bi-prism.

Fresnel’s bi-prism is a combination of two prisms with very small base angles, typically of ~**20′**, when monochromatic light from a slit falls on it. It refracts and produces two virtual images which act like **coherent sources**. An interference pattern is produced which can be seen with an eyepiece. Relevant parameters can be measured by a micrometer attached to the eyepiece. Let us make a diagram suitably representing our situation.

Let us briefly explain the set up. The refracted light rays from **S** and virtually from **S _{1}** and

**S**which act like coherent sources now, go through a convex lens placed in between the Bi-prism and the eyepiece. If the eyepiece is fixed in location there are two positions

_{2}**L**and

_{1}**L**at which images of

_{2}**S**and

_{1}**S**can be seen at the eyepiece.

_{2 }As should be clear by now to the attentive learner the arrangement of Fresnel’s bi-prism must produce the same interference pattern that we discussed for Young’s Double Slit arrangement. We are concerned about measuring the wavelength of light of the source we are using — eg the monochromatic Sodium light source that we use usually. There are two ways to measure the wavelength.

### Method-I:

If **n** represents the refractive index of the bi-prism material and **α** the base angle of the prism, then the angular deviation is given by: **δ = (n-1) α**. From geometrical considerations **S _{1}**

**S**≅

_{2}**2a (n-1) α**where

**a**is the distance of

**S**to the base of the bi-prism.

Typically **n = 1.5** — glass, **α = 20′ = 5.8 × 10 ^{-3} rad**,

**a ≅ 2 cm**which gives

**d = 0.012 cm**. We have seen in the Young’s DS arrangement the fringe spacing

**β**is related to the wave-length

**λ**as follows:

**λ = dβ/D**. We measure

**β**through the micrometer attached to the eye piece. Thus we can determine the wavelength:

**λ**.

### Method-II:

**d** and **D** can be measured by placing a convex lens between bi-prism and eye-piece. Let **d _{1}** be the distance between two images when lens is placed at

**L**, which is at a distance

_{1}**b**from eyepiece.

_{1}Similarly let **d _{1}** be the distance between two images when lens is at

**L**at a distance

_{2}**b**from eyepiece. Then d is the geometric mean of

_{2}**d**and

_{1}**d**, that is:

_{2}**d = square root (d**and D =

_{1}d_{2})**b**+

_{1}**b**. By using the formula

_{2}**λ = dβ/D**again we can have the wavelength of a monochromatic light source.

## One comment