For thin spherical shell of water (radius R, thickness t), volume of water:
- π R²
- V = 0
- (4/3)π R³
- ≈ 4π R² t (for t << R, approximate via differential)
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Correct answer: D. ≈ 4π R² t (for t << R, approximate via differential)
dV/dR = 4πR² (surface area).
Thin shell V ≈ 4πR² × t for t << R. Useful in fluid dynamics, atomic structure (shell-by-shell electron density).