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Physics · Ch 6 — Optics

Dispersive Power

6.7.5

Dispersive Power

If δV,δR\delta_V,\delta_R are the deviations a prism produces for violet and red light, of refractive indices nV,nRn_V,n_R, then δV−δR=(nV−nR)A\delta_V-\delta_R=(n_V-n_R)A is called the angular dispersion -- the angular gap between the two extreme colours of the spectrum, depending on the prism's apex angle AA and on the material (through nV−nRn_V-n_R). Taking δ\delta as the deviation for a mean (middle) colour such as yellow or green, and nn as its corresponding refractive index, dispersive power is defined as ω=δV−δRδ=nV−nRn−1\boxed{\omega=\dfrac{\delta_V-\delta_R}{\delta}=\dfrac{n_V-n_R}{n-1}}, a dimensionless, always-positive quantity that depends only on the nature of the prism material, not on the size of its ape …

Table 6.4Refractive indices for different wavelengths
ColourWavelength (nm)Crown glassFlint glass
Violet396.91.5331.663
Blue486.11.5231.639
Figure 6.45Angle of deviation for different colours

What this figure shows. A prism is shown splitting an incident beam into just its two extreme visible colours, violet and red, each deviated by its own angle, delta(V) for violet (the larger deviation) and delta(R) for red (the smaller deviation); the angular gap between these two deviated rays, delta(V) minus delta(R), is the angular dispersion produced by the prism, the quantity dispersive power is built from by dividing it by the deviation of a middle (mean) …

Misc Example 6.22Dispersive power of flint glass

Worked out. Flint glass has refractive indices 1.632 for violet, 1.613 for red, and 1.620 for (mean) green light. Substituting into the dispersive-power formula omega = (nV - nR)/(nG - 1) gives omega = (1.632 - 1.613)/(1.620 - 1) = 0.019/0.620 = 0.0306. Because dispersive power is a dimensionless ratio, this value of about 0.031 characterises flint glass's colour-splitting ability on its own, independent of whatever particular apex angle a prism happens …