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 \( 1 : 27 \).
A steel wire of length 2 m and Young's modulus \( 2.0 \times 10^{11} \, \text{N/m}^2 \) is stretched by a force. If Poisson's ratio and transverse strain for the wire are \( 0.2 \) and \( 10^{-3} \) respectively, then the elastic potential energy density of the wire is \( \times 10^6\), in SI units .
Two slabs with square cross section of different materials $(1,2)$ with equal sides $(l)$ and thickness $\mathrm{d}_{1}$ and $\mathrm{d}_{2}$ such that $\mathrm{d}_{2}=2 \mathrm{~d}_{1}$ and $l>\mathrm{d}_{2}$. Considering lower edges of these slabs are fixed to the floor, we apply equal shearing force on the narrow faces. The angle of deformation is $\theta_{2}=2 \theta_{1}$. If the shear moduli of material 1 is $4 \times 10^{9} \mathrm{~N} / \mathrm{m}^{2}$, then shear moduli of material 2 is $\mathrm{x} \times 10^{9} \mathrm{~N} / \mathrm{m}^{2}$, where value of x is _______ .
Let \( y^2 = 12x \) be the parabola and \( S \) its focus. Let \( PQ \) be a focal chord of the parabola such that \( (SP)(SQ) = \frac{147}{4} \). Let \( C \) be the circle described by taking \( PQ \) as a diameter. If the equation of the circle \( C \) is: \[ 64x^2 + 64y^2 - \alpha x - 64\sqrt{3}y = \beta, \] then \( \beta - \alpha \) is equal to: