In the previous section, we leant how the angle *θ* at which the fringes are formed is related to the wavelength of the light (and the slit separation). In practice, however, we almost never measure the angle *θ* for the double-slit pattern. Instead we work with the fringe separation *∆y*. Between which two fringes? You might ask. Well, any two. Because the double-slit pattern (usually) has a constant fringe spacing. A little mathematics tells us why.

Let’s use *θ _{n}* to denote the angle at which the

*n*th order bright fringe is formed. Let’s also use

*y*to denote the distance between

_{n}*n*th order and 0th order bright fringe.

Let’s start from the fact that

,

Rearranging the equation, we get

,

For double-slits, *d* is of the order of 0.1 mm, and *l *is between 400 nm and 750 nm, making very small. This means that the low order fringes (let’s say ) are all formed at very small *θ*.

For small values of *θ*, we can replace with . This is because if *θ* is small, . So

,

In other words, the bright fringes are formed at

,

The fringe separation is thus

Let’s remind ourselves that the fringe separation is constant only for the fringes which are formed at small *θ*. However, the higher order fringes of a double-slit pattern are usually too dim to be seen anyway (due to the diffraction envelope effect, which will be discussed later). All we get to see are the lower order fringes, which are formed at small values of *θ*, which thus display a constant fringe separation.

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**Applet**

Interference of Light at a Double-Slit (Walter-Fendt)

**Concept Test**