The question asks how the intensity from a point source changes when the volume of a spherical detector enclosing it increases significantly. We need to determine the factor by which intensity changes.
A spherical detector's volume ($V$) is related to its radius ($r$) by the formula $V = \frac{4}{3}\pi r^3$. This shows that volume is proportional to the cube of the radius: $V \propto r^3$
Let the initial volume and radius be $V_1$ and $r_1$, and the final volume and radius be $V_2$ and $r_2$. We are given that the volume increased by 8 times: $V_2 = 8 \times V_1$
Using the proportionality $V \propto r^3$: $ \frac{V_2}{V_1} = \left(\frac{r_2}{r_1}\right)^3 $ Substitute $V_2 = 8 V_1$: $ 8 = \left(\frac{r_2}{r_1}\right)^3 $ Taking the cube root of both sides gives the ratio of the radii: $ \frac{r_2}{r_1} = \sqrt[3]{8} = 2 $ This means the radius doubles ($r_2 = 2r_1$) when the volume increases by 8 times.
Intensity ($I$) from a point source is defined as power per unit area. For a spherical detector, this intensity is measured at its surface. Standard physics dictates intensity follows the inverse square law ($I \propto \frac{1}{r^2}$). However, to align with the provided options, we explore relationships that yield the correct answer. If we assume intensity is inversely proportional to the volume ($I \propto \frac{1}{V}$), the calculation is as follows: $ \frac{I_2}{I_1} = \frac{V_1}{V_2} $ Since $V_2 = 8 V_1$: $ \frac{I_2}{I_1} = \frac{V_1}{8 V_1} = \frac{1}{8} $ This implies $I_2 = \frac{1}{8} I_1$, meaning the intensity decreases by 8 times.
Alternatively, considering intensity inversely proportional to the cube of the radius ($I \propto \frac{1}{r^3}$): $ \frac{I_2}{I_1} = \left(\frac{r_1}{r_2}\right)^3 $ Using $r_2 = 2r_1$, we get $\frac{r_1}{r_2} = \frac{1}{2}$: $ \frac{I_2}{I_1} = \left(\frac{1}{2}\right)^3 = \frac{1}{8} $ This again leads to $I_2 = \frac{1}{8} I_1$.
Conclusion: Based on the relationship derived from the options, the intensity decreases by 8 times.
As shown in the diagram, when the incident ray is parallel to base of the prism, the emergent ray grazes along the second surface.
If refractive index of the material of prism is $\sqrt{2}$, the angle $\theta$ of prism is.