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Water hammer pressure and stress, 2300 m pipeline

Short answer

Water hammer pressure rise Δp = 2.38 MPa, hoop stress = 63.9 MPa. At 1725 m downstream from reservoir (575 m from valve): pressure steps: 0 to 0.50 s static, +2.38 MPa from 0.50 to 3.50 s, 0 from 3.50 to 4.50 s, -2.38 MPa from 4.50 to 7.51 s, 0 thereafter; cycle 8.01 s.

A 2300 m long pipeline leading from a large tank has a diameter of 15 cm and thickness of 2.8 mm. When a discharge of 2200 liters per minute of water was flowing, the valve was suddenly closed completely. What water hammer pressure and stress would develop at this condition? Also sketch the variation of the water hammer pressure with time at a distance of 1725 m downstream from reservoir end. Take K=2×109K = 2\times10^9 Pa for water and E=2.08×1011E = 2.08\times10^{11} Pa for steel.

Data. L=2300L = 2300 m, D=0.15D = 0.15 m, t=2.8t = 2.8 mm, Q=2200Q = 2200 l/min =0.03667= 0.03667 m³/s, K=2×109K = 2\times10^9 Pa, E=2.08×1011E = 2.08\times10^{11} Pa. Instantaneous closure.

Velocity and wave speed

V0=QπD2/4=0.036670.017671=2.075 m/sV_0 = \frac{Q}{\pi D^2/4} = \frac{0.03667}{0.017671} = 2.075\ \text{m/s} c=K/ρ1+KDEt=2×1061+2×109(0.15)2.08×1011(0.0028)=1414.21+0.5151=1148.9 m/sc = \sqrt{\frac{K/\rho}{1 + \dfrac{KD}{Et}}} = \frac{\sqrt{2\times10^{6}}}{\sqrt{1 + \dfrac{2\times10^9(0.15)}{2.08\times10^{11}(0.0028)}}} = \frac{1414.2}{\sqrt{1 + 0.5151}} = 1148.9\ \text{m/s}

Check closure type: 2L/c=4.002L/c = 4.00 s, and the valve closes instantaneously, so the closure is rapid (full Joukowsky rise).

Water hammer pressure

Δp=ρcV0=1000(1148.9)(2.075)=2.384×106 Pa=2.38 MPa(ΔH=243.0 m of water)\Delta p = \rho cV_0 = 1000(1148.9)(2.075) = 2.384\times10^6\ \text{Pa} = 2.38\ \text{MPa}\quad(\Delta H = 243.0\ \text{m of water})

Stress developed

Hoop (circumferential) stress due to the pressure rise, thin-walled pipe:

σ=Δp D2t=(2.384×106)(0.15)2(0.0028)=63.9 MPa\sigma = \frac{\Delta p\,D}{2t} = \frac{(2.384\times10^6)(0.15)}{2(0.0028)} = 63.9\ \text{MPa}

(The longitudinal stress is about half of this, ΔpD/4t\Delta p D/4t.)

Pressure-time variation at 1725 m from the reservoir

The point is d=2300−1725=575d = 2300 - 1725 = 575 m from the valve (x=1725x = 1725 m from the reservoir). Wave arrival times (c=1148.9c = 1148.9 m/s):

  • t1=d/c=0.500t_1 = d/c = 0.500 s: wave from the valve arrives; pressure rises by +2.38+2.38 MPa
  • t2=(2L−d)/c=3.503t_2 = (2L - d)/c = 3.503 s: wave reflected from the reservoir arrives (negative); pressure falls back to the static value
  • t3=(2L+d)/c=4.504t_3 = (2L + d)/c = 4.504 s: negative wave reflected from the valve arrives; pressure falls to −2.38-2.38 MPa
  • t4=(4L−d)/c=7.507t_4 = (4L - d)/c = 7.507 s: positive wave reflected from the reservoir arrives; pressure returns to the static value
  • The cycle repeats with period 4L/c=8.0074L/c = 8.007 s.
Time interval (s)Pressure change at the point
0 to 0.500
0.50 to 3.50+2.38+2.38 MPa
3.50 to 4.500
4.50 to 7.51−2.38-2.38 MPa
7.51 to 8.010 (then the cycle repeats)
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(top = 1.0, bottom = -1.0; '-' is zero line)

(Pressure change relative to static pressure: +1 = +Δp+\Delta p, −1-1 = −Δp-\Delta p; time from 0 to 4L/c=8.04L/c = 8.0 s.)

Answer: Δp=2.38\Delta p = 2.38 MPa (243 m of water); hoop stress σ=63.9\sigma = 63.9 MPa; the pressure at 1725 m from the reservoir is a stepped wave with the changes at tt = 0.50, 3.50, 4.50 and 7.51 s.

✓ Answer checked by Claude Opus 5.5 (high effort)

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