To resolve this, we must first establish the connection between the excess pressure within a soap bubble and its radius, which subsequently determines its volume.
The formula defining the excess pressure (\(\Delta P\)) inside a soap bubble is:
\(\Delta P = \frac{4T}{R}\)
Here, \(T\) denotes the surface tension of the liquid, and \(R\) represents the bubble's radius.
The problem states that the excess pressure in the first bubble is three times that in the second bubble, thus:
\(\Delta P_1 = 3 \Delta P_2\)
Substituting the excess pressure formula yields:
\(\frac{4T}{R_1} = 3 \times \frac{4T}{R_2}\)
Simplifying this equation leads to:
\(\frac{1}{R_1} = \frac{3}{R_2}\)
This implies the relationship:
\(R_2 = 3R_1\)
The volume of a sphere, or bubble, is calculated using the formula:
\(V = \frac{4}{3} \pi R^3\)
Consequently, the volumes of the bubbles are expressed as:
Upon substituting \(R_2 = 3R_1\) into the equation for \(V_2\), we obtain:
\(V_2 = \frac{4}{3} \pi (27R_1^3) = 27 \times \frac{4}{3} \pi R_1^3 = 27V_1\)
Therefore, the ratio of the volumes of the first to the second bubble is:
\(\frac{V_1}{V_2} = \frac{1}{27}\)
Based on these calculations, the correct answer is 1 : 27.
One end of a steel wire is fixed to the ceiling of an elevator moving up with an acceleration \( 2\,\text{m/s}^2 \) and a load of \( 10\,\text{kg} \) hangs from the other end. If the cross-section of the wire is \( 2\,\text{cm}^2 \), then the longitudinal strain in the wire is given. (Take \( g=10\,\text{m/s}^2 \) and \( Y=2.0\times10^{11}\,\text{N/m}^2 \)). 