Consider a wire with density $\rho$ and stress $\sigma$. For the same density, if the stress increases 2 times, the speed of the transverse waves along the wire changes by
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Wave speed in a wire is independent of the wire's cross-sectional area as long as the material (density) and the applied stress remain the same.
Concept:
The speed ($v$) of a transverse wave in a stretched string/wire is:
\[ v = \sqrt{\frac{T}{\mu}} \]
Where $T$ is the tension and $\mu$ is the mass per unit length.
Step 1: Relate the formula to stress ($\sigma$) and density ($\rho$).
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• Tension ($T$): $\text{Stress} \times \text{Area} = \sigma A$.
• Linear Density ($\mu$): $\text{Density} \times \text{Area} = \rho A$.
Substituting these into the velocity formula:
\[ v = \sqrt{\frac{\sigma A}{\rho A}} = \sqrt{\frac{\sigma}{\rho}} \]
Step 2: Calculate the change in speed.
Since $\rho$ is constant, $v \propto \sqrt{\sigma}$.
If stress increases 2 times ($\sigma' = 2\sigma$):
\[ v' = \sqrt{\frac{2\sigma}{\rho}} = \sqrt{2} \times v \]
The speed changes by a factor of $\sqrt{2}$.