Step 1: Understanding the Concept:
The fundamental frequency of a stretched string vibrating transversely depends on three factors: its length, the tension applied, and its linear mass density (mass per unit length).
The linear mass density itself is determined by the material's density and the string's cross-sectional area, which directly relates to its diameter.
Step 2: Key Formula or Approach:
The fundamental frequency \( f \) is given by Mersenne's law:
\[ f = \frac{1}{2L} \sqrt{\frac{T}{\mu}} \]
where \( L \) is length, \( T \) is tension, and \( \mu \) is linear mass density.
Express \( \mu \) in terms of diameter \( d \) and material density \( \rho \):
\[ \mu = \text{Volume density} \times \text{Cross-sectional area} = \rho \cdot \pi \left(\frac{d}{2}\right)^2 = \frac{\pi \rho d^2}{4} \]
Step 3: Detailed Explanation:
Substitute the expression for \( \mu \) into the frequency formula:
\[ f = \frac{1}{2L} \sqrt{\frac{T}{\frac{\pi \rho d^2}{4}}} \]
\[ f = \frac{1}{2L} \sqrt{\frac{4T}{\pi \rho d^2}} \]
\[ f = \frac{1}{2L} \cdot \frac{2}{d} \sqrt{\frac{T}{\pi \rho}} \]
\[ f = \frac{1}{L \cdot d} \sqrt{\frac{T}{\pi \rho}} \]
The problem states that both strings have the same material (same density \( \rho \)), same length (\( L \)), and are under equal tension (\( T \)).
Therefore, all terms except \( f \) and \( d \) are constant.
This establishes an inverse proportionality between frequency and diameter:
\[ f \propto \frac{1}{d} \implies d \propto \frac{1}{f} \]
We can write this as a ratio for the two strings:
\[ \frac{d_1}{d_2} = \frac{f_2}{f_1} \]
Given the fundamental frequencies are \( f_1 = 1600 \text{ Hz} \) and \( f_2 = 900 \text{ Hz} \), we plug these in to find the ratio of their respective diameters:
\[ \frac{d_1}{d_2} = \frac{900}{1600} \]
\[ \frac{d_1}{d_2} = \frac{9}{16} \]
Thus, the ratio \( d_1 : d_2 \) is \( 9 : 16 \).
Step 4: Final Answer:
The correct ratio matches option (E).