NivaarExam PrepOfficial exam papers ↗

04-BS-7 · Undated paper

Question 11 of 13: Shape of a Falling Raindrop

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

04-BS-7 Mechanics of Fluids — undated sitting, identified as May 2019 (National Examinations, three hours, closed book). Section A (Calculative) offers 9 questions and instructs “do seven”; Section B (Analytical) offers 4 questions and instructs “do three.” A complete paper is any 10 of the 13, each worth 5 marks. Every question is answered below (13 of 13) so the set can be used as a full study resource. Constants used throughout (from the paper's own Constants page, p.12): g = 9.81 m/s², patm = 100 kPa, ρwater = 1000 kg/m³, SGbenzene = 0.90, SGmercury = 13.56, SGcarbon tetrachloride = 1.59, ρair = 1.19 kg/m³ (20°C), μwater = 1.0×10⁻³ N·s/m², μair = 1.8×10⁻⁵ N·s/m².

Reference texts: F. M. White, Fluid Mechanics, 8th ed. (McGraw-Hill) — fluid statics and manometry (Ch. 2), hydrostatic forces on plane surfaces (Ch. 2), the Bernoulli/continuity pair and orifice flow (Ch. 3), the linear-momentum equation for moving vanes (Ch. 3), pipe friction and the Moody/Colebrook relation (Ch. 6), boundary layers and drag (Ch. 7), capillary rise (Ch. 1), high-lift devices and aircraft wing aerodynamics (J. D. Anderson, Fundamentals of Aerodynamics, Ch. 4–5).

Question 11: Shape of a Falling Raindrop (5 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

A very large raindrop falling at its terminal velocity assumes an oblate (flattened) shape, not a sphere and certainly not the pointed "tear-drop" prolate shape so often drawn in cartoons. The competing influences on a falling drop's shape are surface tension, which always acts to minimise surface area and pull the drop toward a sphere, and aerodynamic pressure, which builds up on the drop's underside as it falls through the air at increasing speed. For a large drop the aerodynamic (dynamic) pressure acting over its relatively large cross-sectional area becomes comparable to, and eventually exceeds, the stabilising surface-tension pressure (which scales as 2σ/r and therefore weakens as the drop grows). The high pressure on the flat underside pushes the base of the drop inward and outward radially, flattening it into a shape resembling a hamburger bun; at the largest stable sizes the underside can even develop a concave dimple before the drop becomes aerodynamically unstable and breaks apart into smaller droplets.

A very small drop, by contrast, has a much larger surface-tension pressure (2σ/r grows as r shrinks) relative to the aerodynamic pressure it experiences at its much lower terminal velocity, so surface tension dominates completely and the drop remains essentially spherical. The familiar pointed "tear-drop" silhouette is not physically observed in free fall at all — it is an artefact of drops clinging to and stretching from a surface (a tap or a leaf) under gravity before they detach, not of drops falling freely through air.

Drop sizeDominant effectShape
Very smallsurface tension dominatesspherical
Very largeaerodynamic pressure dominatesoblate (flattened)