The excess pressure inside a soap bubble is given by the formula: \[ \Delta P = \frac{4 \sigma}{r} \]
where:
- \( \Delta P \) is the excess pressure,
- \( \sigma \) is the surface tension of the soap film,
- \( r \) is the radius of the bubble. Let \( r_1 = 2 \, {cm} \) and \( r_2 = 3 \, {cm} \) be the radii of the two bubbles.
The ratio of the excess pressures is: \[ \frac{\Delta P_1}{\Delta P_2} = \frac{\frac{4 \sigma}{r_1}}{\frac{4 \sigma}{r_2}} = \frac{r_2}{r_1} \]
Substituting the given values: \[ \frac{\Delta P_1}{\Delta P_2} = \frac{3}{2} \]
Thus, the ratio of the excess pressures is 3:2.
Therefore, the correct answer is (B).
Kepler's second law (law of areas) of planetary motion leads to law of conservation of
A glass capillary of radius 0.15 mm is dipped into a liquid of density and surface tension 1600 kg/m3 and 0.12 Nm-1,respectively. The liquid in the capillary rises by a height of 5.0 cm. The contact angle between liquid and glass will be:(Take g=10 ms-2)
Kepler's second law (law of areas) of planetary motion leads to law of conservation of