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The Diffraction Grating A diffraction grating has thousands of narrow apertures. Consider a typical grating having 500linesmm-1. The situation can be analysed in the same way as Young’s two slit experiment.
If distance b–c is l then waves from a and b will interfere constructively at a point in a direction q to the normal. However, if b–c is l then d–e will be 2l, f–g will be 3l and so on. Therefore, waves from hundreds of slits will interfere constructively, producing a well defined maximum of the diffraction pattern, called a diffraction image. Other maxima will occur when b–c = 2l, 3l etc. The width of the apertures is only 1/500mm so the fringe spacing is much wider than in Young’s experiment which means that the angles q are not small angles. Therefore, to find the angular positions of the maxima, we use the equation
where n (= 1, 2, 3 etc) is now called the order of the image of the diffraction pattern.
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© David Hoult 2008 |
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