# Water Waves Passing Through A Narrow Gap

**Introduction**

- Water Waves Passing Through A Narrow Gap Va
- Diffraction – Wave Spreading Around An Edge Physics And ...

Water will accelerate whenever it passes through a narrower gap – like when you put your thumb over a tap or the end of a hose – and so a fast current that flows out towards the sea is formed. They can flow at two metres per second, faster than any swimmer.”.

When waves pass through a narrow gap, they spread out. This spreading out is called diffraction. Diffraction is defined as the spreading of a wave into regions where it would not be seen if it moved only in straight lines after passing through a narrow slit or past an edge. Diffraction of a light wave is illustrated in *Figure 1*.

**Figure 1: Diffraction**

- The same thing happens to waves as they travel through small holes, or push past obstacles. As the water waves go through the gap they spread out, this is called diffraction. The longer the wavelength of the wave the larger the amount of diffraction. The greatest diffraction happens when the gap size is about the same size as the wavelength.
- A water wave in a shallow tank passes through a gap in a barrier. What happens to the speed and what happens to the wavelength of the wave as it passes through the gap?
- Diffraction: when a wave passes through a narrow gap, it spreads out Diffraction is usually represented by a wavefront as shown by the vertical lines in the diagram above The only property of a wave that changes when its diffracted is its amplitude This is because some energy is dissipated when a wave is diffracted through a gap.

Diffraction may also occur at an edge. When light travels through an aperture or passes the edge of an obstacle, it deviates from the straight-line direction and appears to spread out. Water also exhibits diffraction. The fact that light exhibits diffraction is a proof that light has wave properties. In *Figure 2*, diffraction is illustrated with two different sizes of aperture. It can be noted that the extent of the diffraction depends on the width of the gap compared with the wavelength. The greatest effect occurs when the wavelength is about the same size as the aperture.

**Figure 2: Diffraction at Different Size of Aperture**

**A. Huygens’ Explanation of Diffraction**

When a single drop of water falls into a ripple tank, a circular wavefront will spread outwards from the disturbance. This behaviour is explained by Huygens using the wave theory of light. He suggested that, at any instant, all points on a wavefront could be regarded as a secondary disturbance, giving rise to their own outward-spreading circular wavelets. The tangent curve of the wavefronts produced by the secondary sources gives the new position of the original wavefront. The construction of a circular wavefront is shown in *Figure 3*.

**Figure 3: Construction of a Circular Wavefront**

In the case of a plane wavefront, if it is restricted by passing through an aperture, some of the wavelets forming the wavefront are removed, and hence the edges of the wavefront are curved. In this case, the size of the aperture is larger than the wavelength of the wavefront, the effect of diffraction is relatively small and the wavefront is curved only at the edges. But, if the size of the aperture is approximately equal to the wavelength, the wavefront becomes circular, with the centre on the slit. It can be noted that the wavelength of the wavefront remains the same during diffraction.

**B. Diffraction at Single Slit**

*Figure 4* shows a plane wavefront diffracted at a single slit of width *a*. Each point on the wavefront passing through the slit can be considered to be a source of secondary wavelets. *A* is a source at the top edge of the slit and another one is *B*, at the centre of the slit. *B* is at a distance *a*/2 along the wavefront from *A*. The two sources produce wavelets that spread out and the overlapping points create an interference pattern. **Constructive interference** creates a bright fringe in the centre of the pattern. The condition for constructive interference is that the path difference should be a whole number of the wavelengths. To either side of the central fringe, there are directions where the path difference between the waves from *A* and *B* are an odd number of half-wavelengths. This is called **destructive interference** and results in dark fringes.

**Figure 4: Wavefront Diffracted at a Single Slit**

The above explanation can be extended to the whole of the slit. Every wavelet spreading from the top half of the slit can be paired with the one coming from a point *a*/2 below, in the lower half of the slit. Intensity graphs of the diffraction pattern as a function of the angle θ, at which the light is viewed, is shown in *Figure 5* below. It can be noted that the intensity is concentrated in the central region. A pattern of dark and bright fringes is also formed along the central region.

**Figure 5: Diffraction Pattern**

For destructive interference,

This is the condition for the first dark fringe at angle θ. This can be generalised as,

Where n is a whole number and is the order of the dark fringe counting outwards from the centre.

For light waves, the width of the aperture is very small and hence the diffraction angle, θ is also very small. When θ is very small (less than 5°),

This approximation does not apply for sound or water waves, where the diffraction angles are larger and the wavelength may be closer in magnitude to the width of the slit.

**C. Diffraction grating**

A diffraction grating is a plate on which there is a very large number of parallel, identical, very closely spaced slits. If light is incident on this plate, a pattern of narrow bright fringes is produced, as shown in *Figure 6*.

**Figure 6: Diffraction Grating**

*Figure 6 *shows a parallel beam of monochromatic light incident normally on a diffraction grating, in which the spacing between adjacent slits is d. Let us consider the first rays a and b, incident on adjacent slits as shown in *Figure 7*.

**Figure 7: Diffraction Grating**

path difference=dsin

Where, θ is the angle at which they emerge.

For constructive interference, the path difference should be an integral number of wavelength,

Where λ is the wavelength of the monochromatic light used and n is the integer.

### Water Waves Passing Through A Narrow Gap Va

When n=0, sin =0 and hence θ=0, and this is called the zero-order maximum.

When n=1, its called the first-order diffraction maximum, and so on.

**D. Summary**

- When waves pass through a narrow gap, they spread out. This spreading out is called
**diffraction**. **Huygens’ explanation of diffraction:**At any instant, all points on a wavefront could be regarded as secondary disturbance, giving rise to their own outward-spreading circular wavelets. The tangent curve of the wavefronts produced by the secondary sources gives the new position of the original wavefront.- In diffraction at a
**single slit**, two sources produce wavelets that spread out and the overlapping points create an interference pattern. - A
**diffraction grating**is a plate on which there is a very large number of parallel, identical, very closely spaced slits. - For constructive interference, the path difference should be an integral number of wavelength, d sinӨ=nλ, where n is the
**order of diffraction**.

**The wavelength** of water waves may beseveralmetres. If thewavelengthis of asimilar sizeto agapin aharbour wall,then thewavewill diffract or spread out into circular ripples. This is quite a good aerial image which shows the effect clearly.If thewavelength is much smaller than thesizeof thegap,then only alittle bit of diffraction will occur at the edge of the wave where the wave falls over on itself to form circular ripples and most of the wave passes straight through without significant direction change. We can see clearly that the depth of the water is pretty constant, if it weren’t the wavelength of the waves would change, and notice there’s **no change in wavelength, frequency or speed.**

Here are two images, one showing a narrow gap with circular diffraction, the other a wide gap with only small circular bits at each side.

**These diagrams are important, so learn them.**

Here’s a slightly more complicated diffraction image, showing multiple diffractions around different edges in sea waves.

It’s worth noticing that the waves actually pass through each other, their amplitudes adding up in space and time.

I just got back from the mountains where TV signals sometimes are a bit wobbly, because the waves can’t diffract well enough over the mountains to be received clearly in the valley. Work out the wavelength for yourself. The TV signal is a radio wave travelling at 300 million m/s and might have a frequency of 600MHz. Got it? Wavelength = speed/frequency = half a metre. Mountains are a lot bigger than this so there isn’t much diffraction around them. We have to use much lower frequencies or bounce the wave off a satellite.

The idea of diffraction is important in loudspeaker design. Speakers that produce low frequency bass notes are called “woofers”. They need to move a lot of air, so need to be quite large. Diameters of 30 cm or more are common.

However, a typical high treble note has a frequency of 5000 Hz or so, which corresponds to a wavelength of almost 7cm – sound travelling at 330 m/s in air. This is much less than the diameter we need for a woofer, so if we try to use the woofer to generate a high frequency note, the sound wave will beam straight ahead without significant diffraction, just like water waves passing through a wide gap. So, you won’t hear those notes unless you are right in front of the speaker.

It’s clear, then that the speakers which produce high frequency notes, called “tweeters”, must have a much smaller diameter than required for the woofer.

### Diffraction – Wave Spreading Around An Edge Physics And ...

In the picture, the woofer is above and the tweeter is below. A simple electric circuit inside the enclosure directs low frequencies to the woofer and high frequencies to the tweeter.