To solve this problem, we need to understand the relationship between excess pressure inside a soap bubble and its radius, and subsequently its volume.
The formula for excess pressure (\(\Delta P\)) inside a soap bubble is given by:
\(\Delta P = \frac{4T}{R}\)
where \(T\) is the surface tension of the liquid and \(R\) is the radius of the soap bubble.
According to the question, the excess pressure inside the first bubble is thrice that inside the second bubble, so:
\(\Delta P_1 = 3 \Delta P_2\)
By substituting the formula for excess pressure, we get:
\(\frac{4T}{R_1} = 3 \times \frac{4T}{R_2}\)
After simplifying, the above equation becomes:
\(\frac{1}{R_1} = \frac{3}{R_2}\)
This implies:
\(R_2 = 3R_1\)
The volume of a sphere (or bubble) is given by:
\(V = \frac{4}{3} \pi R^3\)
Thus, the volumes of the bubbles can be represented as:
After substituting \(R_2 = 3R_1\) into the equation for \(V_2\), we find:
\(V_2 = \frac{4}{3} \pi (27R_1^3) = 27 \times \frac{4}{3} \pi R_1^3 = 27V_1\)
Therefore, the ratio of the volumes of the first and second bubble is:
\(\frac{V_1}{V_2} = \frac{1}{27}\)
Based on this calculation, the correct answer is 1 : 27.
The excess pressure \( P_{\text{excess}} \) inside a soap bubble is given by the formula:
\[ P_{\text{excess}} = \frac{4T}{r}, \] where \( T \) is the surface tension and \( r \) is the radius of the bubble.
Let the radii of the two bubbles be \( r_1 \) and \( r_2 \), and their excess pressures be \( P_1 \) and \( P_2 \), respectively.
Given:
\[ P_1 = 3P_2. \]
Using the formula for excess pressure:
\[ \frac{4T}{r_1} = 3 \times \frac{4T}{r_2}. \]
Cancelling common terms:
\[ \frac{1}{r_1} = 3 \times \frac{1}{r_2} \Rightarrow r_1 = \frac{r_2}{3}. \]
Since the volume of a sphere is \( V = \frac{4}{3} \pi r^3 \), the ratio of the volumes is:
\[ \frac{V_1}{V_2} = \left( \frac{r_1}{r_2} \right)^3 = \left( \frac{1}{3} \right)^3 = \frac{1}{27}. \]
Thus, the ratio of the volumes 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 \( Y=2.0\times10^{11}\,\text{N/m}^2 \)). 
Let the lines $L_1 : \vec r = \hat i + 2\hat j + 3\hat k + \lambda(2\hat i + 3\hat j + 4\hat k)$, $\lambda \in \mathbb{R}$ and $L_2 : \vec r = (4\hat i + \hat j) + \mu(5\hat i + + 2\hat j + \hat k)$, $\mu \in \mathbb{R}$ intersect at the point $R$. Let $P$ and $Q$ be the points lying on lines $L_1$ and $L_2$, respectively, such that $|PR|=\sqrt{29}$ and $|PQ|=\sqrt{\frac{47}{3}}$. If the point $P$ lies in the first octant, then $27(QR)^2$ is equal to}