To address this issue, we must analyze the relationship between the speed of a transverse wave on a string and its physical characteristics. The speed \( v \) of a transverse wave on a string is determined by the equation:
\(v = \sqrt{\frac{T}{\mu}}\)
where:
Given that both strings are composed of the same material and are subjected to identical tension, the primary determinant of the wave's speed is the linear mass density \(\mu\). Linear mass density is defined as:
\(\mu = \frac{m}{L}\),
where \(m\) is the mass of the string and \(L\) is its length. For a string with a circular cross-section, \( \mu \) can also be expressed in terms of its volume as:
\(\mu = \rho \cdot A\)
where:
For a circular cross-section, the area \( A \) is calculated as:
\(A = \pi R^2\)
Consequently, the linear mass density is:
\(\mu = \rho \pi R^2\)
With constant tension, the ratio of velocities depends on the ratio of the square roots of the inverse of their linear densities:
\(\frac{v_2}{v_1} = \sqrt{\frac{\mu_1}{\mu_2}}\)
For the first string with radius \( R \), the linear density is:
\(\mu_1 = \rho \pi R^2\)
For the second string with radius \( \frac{R}{2} \), the linear density is:
\(\mu_2 = \rho \pi \left(\frac{R}{2}\right)^2 = \rho \pi \frac{R^2}{4}\)
The ratio calculation yields:
\(\frac{v_2}{v_1} = \sqrt{\frac{\rho \pi R^2}{\rho \pi \frac{R^2}{4}}} = \sqrt{4} = 2\)
Therefore, the ratio \(\frac{v_2}{v_1}\) is \(2\). The correct answer is:
Option: 2