\(\frac{I}{2}\)
\(\frac{I}{16}\)
\(\frac{I}{4}\)
The problem asks for the intensity of light from a point source at a distance of 4 cm, given that its intensity is I at a distance of 2 cm.
The intensity of light from a point source follows the inverse square law. This law states that the intensity (E) of the light is inversely proportional to the square of the distance (d) from the source. This is because a point source radiates energy uniformly in all directions, and as the distance increases, this energy spreads over the surface of an increasingly larger sphere.
The surface area of a sphere with radius \(d\) is \(A = 4\pi d^2\). If the source has a constant power P, the intensity (Power per unit area) is:
\[ E = \frac{P}{A} = \frac{P}{4\pi d^2} \]From this equation, we can see the relationship:
\[ E \propto \frac{1}{d^2} \]Step 1: Formulate the relationship between intensities at two different distances.
Let \(E_1\) be the intensity at a distance \(d_1\) and \(E_2\) be the intensity at a distance \(d_2\). From the inverse square law, we can write the ratio:
\[ \frac{E_2}{E_1} = \frac{1/d_2^2}{1/d_1^2} = \frac{d_1^2}{d_2^2} = \left(\frac{d_1}{d_2}\right)^2 \]Step 2: Identify the given values from the problem statement.
The initial intensity is \(E_1 = I\).
The initial distance is \(d_1 = 2 \, \text{cm}\).
The final distance is \(d_2 = 4 \, \text{cm}\).
We need to find the final intensity, \(E_2\).
Step 3: Substitute the known values into the ratio equation.
\[ \frac{E_2}{I} = \left(\frac{2 \, \text{cm}}{4 \, \text{cm}}\right)^2 \]Step 4: Calculate the final intensity \(E_2\).
First, simplify the fraction inside the parentheses:
\[ \frac{E_2}{I} = \left(\frac{1}{2}\right)^2 \]Now, square the fraction:
\[ \frac{E_2}{I} = \frac{1}{4} \]Finally, solve for \(E_2\):
\[ E_2 = \frac{I}{4} \]The intensity at a distance of 4 cm from the source shall be I/4.

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