If the surface tension of water-air interface is 0.073 N/m, the gauge pressure inside a rain drop of 1 mm diameter will be
292 N/m2
This question involves calculating the gauge pressure inside a small spherical liquid drop due to surface tension. Surface tension is a property of liquids that allows them to resist an external force, acting like a stretched elastic membrane on the surface. For a spherical liquid drop, this surface tension creates an inward pull, resulting in a higher pressure inside the drop compared to the outside. This excess pressure is known as gauge pressure.
The excess pressure ($ \Delta P $) inside a spherical drop due to surface tension ($ \gamma $) is given by the Laplace pressure formula for a single interface:
$$ \Delta P = \frac{2 \gamma}{r} $$
Where:
From the question, we have the following information:
To find the gauge pressure, we first need to determine the radius of the rain drop and ensure all units are consistent.
$$ r = \frac{d}{2} $$
$$ r = \frac{1 \, \text{mm}}{2} = 0.5 \, \text{mm} $$
$$ 1 \, \text{mm} = 1 \times 10^{-3} \, \text{m} $$
Therefore,
$$ r = 0.5 \, \text{mm} = 0.5 \times 10^{-3} \, \text{m} $$
$$ \Delta P = \frac{2 \gamma}{r} $$
$$ \Delta P = \frac{2 \times 0.073 \, \text{N/m}}{0.5 \times 10^{-3} \, \text{m}} $$
$$ \Delta P = \frac{0.146 \, \text{N/m}}{0.5 \times 10^{-3} \, \text{m}} $$
$$ \Delta P = \frac{0.146}{0.5} \times 10^3 \, \text{N/m}^2 $$
$$ \Delta P = 0.292 \times 10^3 \, \text{N/m}^2 $$
$$ \Delta P = 292 \, \text{N/m}^2 $$
The calculated gauge pressure inside the rain drop is 292 N/m2. This value corresponds to one of the given options.
Which of the following statements is NOT correct about surface tension?
If a liquid droplet and a soap bubble are formed from the same liquid and have the same radius $R$, how does the excess pressure inside the soap bubble ($\Delta P_{bubble}$) compare to the excess pressure inside the liquid droplet ($\Delta P_{droplet}$)?
Mercury does NOT wet the glass. This is due to the property of the liquid known as
________ is a surface phenomenon.
A liquid drop is spherical in shape due to