THE BRAINS BEHIND DISCOVERING DIFFRACTION
*Italian scientist Francesco Maria Grimaldi originated the word "diffraction".He was the first to record accurate observations of the phenomenon(diffraction) in the year 1665. *
DEFINITON
Diffraction occurs when light(beam/ray of light) or other system of waves such as (water waves, sound, electromagnetic waves ( electromagnetic radiation), and small moving particles such as atoms, neutrons, and electrons, which show wavelike properties) passes sharp edges or goes through narrow slits(aperture), the rays are deflected(spread out) and produce fringes of light and dark bands.
Diffraction of light
Diffraction effects are classified into either Fresnel or Fraunhofer types.
Fresnel diffraction is concerned mainly with what happens to light in the immediate neighborhood of a diffracting object or aperture, so is only of interest when the illumination source is close by.
Fraunhofer diffraction is the light-spreading effect of an aperture when the aperture (or object) is lit by plane waves, i.e., waves that effectively come from a source that is infinitely far away.
TERMS USED AND THEIR DEFINITIONS
- Aperture : Aperture is an optical terminology,it layman's term it is called different names such as an opening, hole, or gap.It often refers to an opening in which light is allowed to pass in optical systems such as cameras and lasers.
- Waves
- Fringes
PRINCIPLES AND LAWS OF DIFFRACTION
HUYGENS PRINCIPLE
A Dutch physicist Christiaan Huygens earlier proposed in 1678, that "every point in which a luminous disturbance reaches act as a source of a wave spherical in nature", the summation of this secondary waves determines the form of the wave at any point in time".
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HUYGEN-FRESNEL PRINCIPLE
However, in 1816, French physicist Augustin-Jean Fresnel would argue that Huygens principle along with his own (principle of interference) can successfully explain not only the rectilinear propagation of light but also the effects of diffraction. To justify his claims he inculcated more arbitrary assumptions of secondary wave's phase and amplitude with and obliquity factor. His predictions were to some extend arrived at some agreement including the Arago spot, though with no physical root.
Image of Huygens-Fresnel wave diffraction -- Image coursey of Wikimedia Commons
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A good instance of this could be explained with a simple showing with two rooms with a common doorway. When sound is produced in one of the rooms, someone in the other room will assume the same produced sound in the next room is emanating from the doorway they share, as s/he view the doorway as the source of the source due to the vibrating of air at the doorway.
Now let’s consider a source at the point Po, with vibrating frequency f. The disturbance we describe as a complex variable Uo known as the complex amplitude, produces a wave with a wavelength λ, and wave number k = 2π/λ.
The complex amplitude of the primary wave at the point Q located at a distance ro from Po can be given as
THE PRINCIPLE OF BRAGG’S LAW
Sir William Lawrence Bragg in 1912 proposed a law that states that, diffraction occurs when electromagnetic radiation or subatomic particle waves with wavelength comparable to atomic spacing, are incident upon a crystalline sample, scattered by the atoms in the system and undergo constructive interference.
http://www.microscopy.ethz.ch/bragg.htm
Destructive interference of reflected waves (in the reflected waves, maximum and minimum of the wave amplitude are superimposed).
http://www.microscopy.ethz.ch/bragg.htm
Constructive Interference of reflected waves (reflected waves in phase, i.e., maxima are superimposed).
Mathematical form of Bragg's Law
nλ = 2.d.sinΘ
Where
• n is an integer determined by the order given,
• λ is the wavelength of x-rays, and moving electrons, protons and neutrons,
• d is the spacing between the planes in the atomic lattice, and
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The derivation of Bragg's Law
http://skuld.bmsc.washington.edu/~merritt/bc530/bragg/
Taking into account the conditions necessary to make phases coincide when the incident angle equals the reflecting angle, the initial rays (incident rays) will be parallel and in phase with the point where the top beam hits the top layer at atom z. In the next layer, the second beam continues where its being scattered by the atom B. The second beam has to travel an additional distance of AB + BC for the two beams to move adjacently and in parallel to each other. The additional distance must an integral (n) multiple of the wavelength (λ) for the phases of the two beams to be the same:
Using pythagoras theorem,
AB/d= sinθ
AB = d sinθ
Since AB = BC, then
nλ = 2AB
Recall that, AB = d sinθ
Thus
nλ = 2.d.sinθ
APPLICATION OF DIFFRACTION
There are several applications of diffraction and these are somewhat evident in our daily contact with objects exhibiting diffraction or diffraction properities, without we noticing,or on the other hand noticing the object but not knowing the principle behind it or what made the object look or act like that.
Here are some of the applications of diffraction
- SCIENTIFIC APPLICATION
- DAY TO DAY APPLICATION
The effects of diffraction are usually seen in everyday life. One of the most evident examples of diffraction are those involving light; for example,when you take a keen look at a CD or DVD the closely spaced tracks on a CD or DVD act as a diffraction grating to form the familiar rainbow pattern. This principle can be extended to engineer a grating with a structure such that it will produce any diffraction pattern desired; the hologram on a credit card.