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Question: Formula for dispersive power is (where symbols have their usual meanings) or If the refractive ind...

Formula for dispersive power is (where symbols have their usual meanings) or
If the refractive indices of crown glass for red, yellow, and violet colours are respectively μr{\mu _r} , μy{\mu _y} and μv{\mu _v} , then the dispersive power of this glass would be
A. μvμyμr1\dfrac{{{\mu _v} - {\mu _y}}}{{{\mu _r} - 1}}
B. μvμrμy1\dfrac{{{\mu _v} - {\mu _r}}}{{{\mu _y} - 1}}
C. μvμyμyμr\dfrac{{{\mu _v} - {\mu _y}}}{{{\mu _y} - {\mu _r}}}
D. μvμrμy1\dfrac{{{\mu _v} - {\mu _r}}}{{{\mu _y}}} - 1

Explanation

Solution

Before we get into the question, let's review some basics of dispersive power. The breaking of white light into its constituent colours is referred to as dispersion. A spectrum is a collection of colours. The separation of different colours of light by refraction is the dispersive power of a transparent medium.

Complete step by step answer:
Consider a glass prism; the refractive index of a prism is determined by the connection relationship,
μ=sinA+D2sinA2\mu = \dfrac{{\sin \dfrac{{A + D}}{2}}}{{\sin \dfrac{A}{2}}}
where AA is the prism's central angle and δ\delta is the deviation angle.

If AA is a small angled prism's refracting angle and is the angle of deviation δ\delta . The prism formula is as follows:
μ=sinA+δ2sinA2\mu = \dfrac{{\sin \dfrac{{A + \delta }}{2}}}{{\sin \dfrac{A}{2}}}
Because we're talking about small angled prisms,
sinA+δ2=A+δ2\sin \dfrac{{A + \delta }}{2} = \dfrac{{A + \delta }}{2} and sinA2=A2\sin \dfrac{A}{2} = \dfrac{A}{2}

\Rightarrow \mu A = A + \delta \\\ $$ Therefore, $$\delta = \left( {\mu - 1} \right)A$$. The corresponding wavelengths are $${\mu _v}$$and $${\mu _r}$$ if ${\delta _v}$ and $${\delta _r}$$ are the deviations of violet and red rays, respectively. As a result, the angular dispersion is expressed as, $$\delta v - \delta r = (\mu v - \mu r)A$$ The difference in deviation between extreme colours is known as angular dispersion. If ${\mu _y}$ and $${\delta _y}$$ are the refractive index and deviation of an intermediate wavelength yellow, then $${\delta _y} = \left( {{\mu _y} - 1} \right)A$$ When both equations are divided, we get $$\dfrac{{{\delta _v} - {\delta _r}}}{{{\delta _y}}} = \dfrac{{{\mu _v} - {\mu _r}}}{{{\mu _y}}}$$ The term $$\dfrac{{{\delta _v} - {\delta _r}}}{{{\delta _y}}}$$ stands for dispersive power of the prism's substance and is represented by the symbol $\omega $ , $$\omega = \dfrac{{{\mu _v} - {\mu _r}}}{{{\mu _y}}}$$ Thus, $$\omega = \dfrac{{(\mu y - 1)A}}{{(\mu v - \mu r)A}} \\\ \therefore \omega = \dfrac{{(\mu y - 1)}}{{(\mu v - \mu r)}}$$ Therefore, the dispersive power of this glass would be $$\dfrac{{{\mu _v} - {\mu _r}}}{{{\mu _y} - 1}}$$. **Hence, the correct option is B.** **Note:** Violet rays have a larger deviation and refractive index than red rays, so keep that in mind. As a result, violet light passes through glass at a slower rate than red rays. The refractive index and deviation of yellow rays are utilised as mean values.