Question:

Energy needed in breaking a liquid drop of radius \( R \), into \( n \) smaller drops each of radius \( r \), is
[ \( T \) - Surface tension of the liquid ]

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Always equate initial and final surface energies when dealing with droplet division. Surface energy = surface area × surface tension.
Updated On: May 17, 2025
  • \( (4\pi r^2 n - 4\pi R^2)T \)
  • \( \left(\frac{4}{3}\pi r^3 n - \frac{4}{3}\pi R^3\right)T \)
  • \( (4\pi R^2 - 4\pi r^2)nT \)
  • \( \frac{(4\pi R^2 - n4\pi r^2)}{T} \)
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The Correct Option is A

Solution and Explanation

The energy required to break a large drop into smaller drops is equal to the increase in surface energy.
Surface energy \( E = \text{Surface area} \times T \)
- Surface area of the original drop = \( 4\pi R^2 \)
- Total surface area of \( n \) small drops = \( n \cdot 4\pi r^2 \)
So the increase in surface area: \[ \Delta A = 4\pi r^2 n - 4\pi R^2 \] Hence, the required energy: \[ E = T \cdot \Delta A = (4\pi r^2 n - 4\pi R^2)T \]
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