To determine the fractional decrease in radius of a spherical object subjected to uniform pressure, we need to use the concept of bulk modulus. The bulk modulus \( B \) is defined as the ratio of the applied pressure change \( \Delta p \) to the relative change in volume \( \frac{\Delta V}{V} \):
B = \frac{\Delta p}{\frac{\Delta V}{V}}Here, \( \Delta p = p \) since the pressure applied is \( p \), and \( \Delta V \) is the change in volume.
For a sphere, the volume \( V \) is given by:
V = \frac{4}{3} \pi r^3where \( r \) is the radius of the sphere.
If there's a small change in radius \( \Delta r \), the new volume \( V' \) becomes:
V' = \frac{4}{3} \pi (r + \Delta r)^3The change in volume \( \Delta V \) is:
\Delta V = V' - V = \frac{4}{3} \pi \left[(r + \Delta r)^3 - r^3\right]For small changes, this can be approximated using a derivative. The derivative of the volume with respect to the radius is:
\frac{dV}{dr} = 4 \pi r^2Thus, the change in volume \( \Delta V \) is approximately:
\Delta V \approx 4 \pi r^2 \Delta rSubstituting into the formula for bulk modulus, we have:
B = \frac{p}{\frac{\Delta V}{V}} = \frac{p}{\frac{4 \pi r^2 \Delta r}{\frac{4}{3} \pi r^3}}Simplifying further gives:
B = \frac{p}{3 \frac{\Delta r}{r}}Solving for the fractional change in radius, we find:
\frac{\Delta r}{r} = \frac{p}{3B}Thus, the fractional decrease in radius is \frac{p}{3B}.
Therefore, the correct answer is \frac{p}{3B}.
A 2 $\text{kg}$ mass is attached to a spring with spring constant $ k = 200, \text{N/m} $. If the mass is displaced by $ 0.1, \text{m} $, what is the potential energy stored in the spring?
