Huygens–Fresnel principle

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The Huygens–Fresnel principle [1] (named for Dutch physicist Christiaan Huygens and French physicist Augustin-Jean Fresnel) is a method of analysis applied to problems of wave propagation (both in the far field limit and in near field diffraction). It recognizes that each point of an advancing wave front is in fact the center of a fresh disturbance and the source of a new train of waves; additionally, the advancing wave as a whole may be regarded as the sum of all the secondary waves arising from points in the medium already traversed. This view of wave propagation helps better understand a variety of wave phenomena, such as diffraction.

For example, if two rooms are connected by an open doorway and a sound is produced in a remote corner of one of them, a person in the other room will hear the sound as if it originated at the doorway. As far as the second room is concerned, the vibrating air in the doorway is the source of the sound. The same is true of the light passing the edge of an obstacle, but this is not as easily observed because of the short wavelength of visible light.

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Single slit diffraction

A common application of Huygens' principle is for the case of a sine wave (usually light, radio waves, x-rays or electrons) incident on an aperture of arbitrary shape. Huygens' principle states that each point in the hole acts as a point source. A point source generates waves that travel spherically in all directions (similar to circular waves caused by dropping small stone in a pond). The sum of the waves from all the point sources at any point beyond the aperture can be calculated by integration or numerical modelling.

Consider the case of single slit diffraction where we have one slit through which we shine light onto a distant screen. Suppose, we want to calculate at which point on the screen interference minima (dark stripes) occur. We then replace this relatively wide slit by an increasing number of narrow ones (subslits), and add waves produced by each. Two small slits interfere destructively when their path lengths differ by λ / 2 (a 180 degrees phase difference). We can calculate (using phasors or a similar wave-addition math) that for three waves from three slits to cancel each other the phases of slits must differ 120 degrees, thus path difference from the screen point to slits must be λ / 3, and so forth. In the limit of approximating the single wide slit with an infinite number of subslits the path length difference between edges of slit must be exactly λ to get complete destructive interference (and so a dark stripe on the screen).

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