NivaarExam PrepOfficial exam papers ↗

04-BS-7 · December 2018

Question 10 of 13: Sliding Stability of Two Triangular Dams

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

Notes on this paper

Reference texts: White, F.M., Fluid Mechanics (8th ed.) — fluid statics and hydrostatic force on plane/curved surfaces incl. gravity-dam stability (Ch. 2), buoyancy and Archimedes' principle (Ch. 2), orifice/nozzle discharge and jet momentum forces (Ch. 3, 6), viscous flow in ducts and the Moody chart (Ch. 6), open-channel flow and the hydraulic jump (Ch. 10), drag and stability of bluff bodies (Ch. 7), turbomachinery and jet propulsion (Ch. 11).

Question 10: Sliding Stability of Two Triangular Dams (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.

Given. Dam A: sloping upstream (water) face, vertical downstream (dry) face. Dam B: vertical upstream (water) face, sloping downstream (dry) face. Both dams have the same base friction coefficient $\mu$ and rest on a firm, flat, non-seeping foundation.

Dam A (sloping upstream face) +vertical comp. Dam B (vertical upstream face) horizontal only
Dam A's sloping upstream face gives the hydrostatic thrust a downward vertical component (added to the weight); Dam B's vertical upstream face gives a purely horizontal thrust with no such addition.

Find. Which dam is more likely to slide, and the physical reason.

Dam B (the vertical-upstream-face dam) is the one most likely to slide. Sliding resistance at the base is frictional, $F_{friction}=\mu N$, where $N$ is the total NORMAL (vertical) force pressing the dam onto its foundation. For Dam B, the upstream face is vertical, so the hydrostatic pressure acts everywhere horizontally — it contributes nothing to $N$, which is therefore just the dam's own weight, $N_B=W_B$. The full horizontal hydrostatic thrust $F_H$ must then be resisted by friction from that weight alone, $\mu W_B$, with no help from the water itself.

Dam A's upstream face is sloped, so the hydrostatic pressure — which always acts perpendicular to the wetted surface — is no longer purely horizontal. Resolving it into components, the horizontal component is (for the same water depth) essentially the same driving force as Dam B's, but there is now ALSO a downward vertical component, because the pressure pushes perpendicular to a surface that is tilted. This vertical component adds directly to the dam's own weight in the normal-force balance, $N_A=W_A+F_{V}$, which increases the available frictional resistance $\mu N_A$ beyond $\mu W_A$ alone — the water itself is, in effect, helping to hold Dam A down onto its foundation. With a larger resisting force available against essentially the same horizontal driving force, Dam A is therefore LESS likely to slide, and by the same argument, Dam B is more likely to slide.