To determine the new speed of the longitudinal wave in the metallic bar, we use the formula for the speed of a wave in a solid medium given by:
\(v = \sqrt{\frac{E}{\rho}}\)
where:
Initially, the speed of the wave \(v_1\) is given as \(400\,\text{m/s}\).
When the density increases by 0.5%, the new density will be: \(\rho' = \rho + 0.005\rho = 1.005\rho\)
Similarly, when Young's modulus increases by 1%, the new modulus will be: \(E' = E + 0.01E = 1.01E\)
The new speed of the wave \(v_2\) is calculated as:
\(v_2 = \sqrt{\frac{E'}{\rho'}}\)
Substituting the changes in \(E\) and \(\rho\), we have:
\(v_2 = \sqrt{\frac{1.01E}{1.005\rho}}\)
\(= \sqrt{\frac{1.01}{1.005}} \cdot \sqrt{\frac{E}{\rho}}\)
Since \(\sqrt{\frac{E}{\rho}} = v_1 = 400 \, \text{m/s}\), substitute in:
\(v_2 = \sqrt{\frac{1.01}{1.005}} \times 400\)
Using a calculator to find \(\sqrt{\frac{1.01}{1.005}} \approx 1.0025\),
\(v_2 = 1.0025 \times 400 \approx 401 \, \text{m/s}\)
Therefore, the new speed of the wave in the metallic bar is approximately \(401\,\text{m/s}\).
This matches the provided correct answer option: \(401\).
A small block of mass \(m\) slides down from the top of a frictionless inclined surface, while the inclined plane is moving towards left with constant acceleration \(a_0\). The angle between the inclined plane and ground is \(\theta\) and its base length is \(L\). Assuming that initially the small block is at the top of the inclined plane, the time it takes to reach the lowest point of the inclined plane is _______. 