Deviation of light by a prismPDF
A prism of angle at the apex A and index n – the air, of unit index, surrounds the prism – deflects a light beam, whose angle of incidence on one of the lateral surfaces of the prism is i, according to the laws of Snell-Descartes of geometric optics: sin i = n sin r and n sin r’ = sin i’ (Figure 1 for the notations). The angle of deflection D = i + i’ – A, with A = r + r’.
The light beam can only emerge from the prism if A < 2 a sin(1/n) ; for ice n = 1.31, hence A < 99.5⁰. If we trace the deviation D as a function of i, we see that it decreases rapidly, reaches a minimum minimorum corresponding to a symmetrical crossing of the prism (i = i’), then increases slowly. The minimum is very flattened, so that a change in the angle of incidence around the incidence that corresponds to this minimum does not significantly change its value; it results in an accumulation of light and therefore a high luminosity around this minimum. For A = 60⁰, the minimum is 22⁰; if A = 90⁰, it is 46⁰ (Figure 2). Figure 3 shows the value of this minimum for the different values of A allowed: it increases with A.
In addition, since the index n depends on the colour of the incident radiation, the minimum also depends on it; a prism breaks down white light into its various monochromatic components. This explains the iridescence of halos obtained by refraction. For A = 60⁰, we have a minimum close to 22⁰ that grows from red to blue (Figure 4).
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