Daniel B. answered 06/06/21
A retired computer professional to teach math, physics
Let
H = 280m - 22m = 258m be the height of the water,
s = 10³ kg/m³ be the density of water,
g = 9.8 m/s² be gravitational acceleration.
At some depth h from the water surface, consider a very thin horizontal strip of size dh.
The length of the strip can be obtained from
y = 0.8x4
x = (y/0.8)1/4
If we set y = H-h, then x = ((H-h)/0.8)1/4.
Therefore the length of the strip, denoted L(h):
L(h) = 2 ((H-h)/0.8)1/4 = 2 (5(H-h)/4)1/4
For future use, let's precompute the indefinite integrals
∫L(h)dh = -2 (4/5)² (5(H-h)/4)5/4 = -2 (4/5)² (5(H-h)/4) (5(H-h)/4)1/4 = -(4/5)(H-h)L(h) (1)
∫(∫L(h)dh)dh = 2(4/5)³(4/9)(5(H-h)/4)9/4 = (4/5)³(4/9)(5(H-h)/4)²L(h) = (4/5)(4/9)(H-h)²L(h) (2)
The area of the strip is L(h)dh.
The pressure at depth h is sgh.
The force F(h) acting on that strip is the pressure times the area:
F(h) = sghL(h)dh
The force acting on the whole dam is the sum over all such strips,
that is, the definite integral from h=0 to h=H over F(h).
Let's first do the indefinite integral
∫F(h)dh = ∫sghL(h)dh = sg ∫hL(h)dh
Let's do the integral by parts following the formula
∫uv' = uv - ∫u'v, where
u = h, u' = 1
v' = L(h), v = ∫L(h)dh = -(4/5)(H-h)L(h) (by (1))
Thus
∫F(h)dh =
sg ∫hL(h)dh = sg (-(4/5)h(H-h)L(h) - ∫(∫L(h)dh)dh) =
sg ((-(4/5)h(H-h)L(h) -(4/5)(4/9)(H-h)²L(h)) = (by (2))
sg(-4/5)(H-h) (hL(h) + (H-h)L(h)) (3)
When computing the definite ∫F(h)dh from h = 0 to h=H,
then for h=H the formula (3) is 0.
Therefore the whole definite integral is
sg(4/5)H²L(0) = (8/5)sgH²(H/0.8)1/4
Substituting actual numbers, the force on the dam is
(8/5)×10³×9.8×258²×(258/0.8)1/4 = 4423×106N