---
title: "Surge and water hammer: 25 m³/s, 15 m surge tank"
subject: "Hydropower Engineering"
chapter: 6
key: "semester_7/hydropower_engineering:surge-numerical-25cumec-2-penstocks-15m-tank"
source: https://www.bctengineer.com/q/semester_7/hydropower_engineering/surge-numerical-25cumec-2-penstocks-15m-tank
site: BCT Engineering
---

# Surge and water hammer: 25 m³/s, 15 m surge tank

Hydropower Engineering · Chapter 6: Water Conveyance Structures

- Asked in: 2079 Baishakh, 8 marks
- Answer checked by Claude Opus 5.5 (high effort) on 2026-10-14
- Page: https://www.bctengineer.com/q/semester_7/hydropower_engineering/surge-numerical-25cumec-2-penstocks-15m-tank
- Whole chapter: https://www.bctengineer.com/md/semester_7/hydropower_engineering/chapter-6

## Question

The design discharge through the tunnel of a hydropower project is 25 m³/sec and is conveyed by two penstocks to the turbine. The length and diameter of the tunnel are 4 km and 8 m respectively, friction factor of the tunnel is 0.016 and length of each penstock is 500 m, diameter and friction factor of the penstock are 2 m and 0.04 respectively and velocity of wave in penstock = 1600 m/sec. If a surge tank of 15 m diameter has been provided at the end of the tunnel, find the following for full load rejection: (i) maximum up-surge, (ii) maximum down-surge, (iii) water hammer pressure, (iv) time of oscillation of wave.

## Short answer

Maximum upsurge is 5.29 m, downsurge 5.16 m. The water hammer pressure head is 649.0 m for rapid closure, and the oscillation time period is 237.9 s.

## Answer

#### Method used
Let the tunnel have area $A_t$, length $L$, diameter $D$ and friction factor $f$; the tank has area $A_s$.

- Tunnel velocity $V = Q/A_t$; steady friction loss $h_f = \dfrac{fLV^2}{2gD}$.
- Frictionless amplitude: $Z_0 = V\sqrt{\dfrac{L A_t}{g A_s}}$.
- Upsurge with friction (full load rejection), $Z$ measured above reservoir level, from the equation of motion and continuity:

$$
\frac{Z_{max}}{h_f}=\frac{Z_0^2}{2h_f^2}\left[1-e^{-2h_f (Z_{max}+h_f)/Z_0^2}\right]
$$

- The following down-surge is found by integrating the reversed-flow equations step by step (below reservoir level).
- Period of mass oscillation: $T = 2\pi\sqrt{\dfrac{L A_s}{g A_t}}$.

#### Surge in the tunnel
$A_t = 50.27\ \text{m}^2$, $A_s = \frac{\pi}{4}(15)^2 = 176.71\ \text{m}^2$, $L = 4000$ m.

- $V = 25/50.27 = 0.497$ m/s
- $h_f = \dfrac{0.016 \times 4000 \times 0.497^2}{2(9.81)(8)} = 0.101$ m
- $Z_0 = 0.497\sqrt{\dfrac{4000 \times 50.27}{9.81 \times 176.71}} = 5.36$ m

#### (i) Maximum up-surge
$Z_{max} = 5.29$ m above reservoir level.

#### (ii) Maximum down-surge
First downswing $= 5.16$ m below reservoir level.

#### (iii) Water hammer pressure
Flow per penstock $= 25/2 = 12.5$ m³/s; $v = 12.5/3.142 = 3.979$ m/s. Closure time for full load rejection is taken as less than $2L/a = 2(500)/1600 = 0.625$ s (rapid closure):

$$
h = \frac{a v}{g} = \frac{1600 \times 3.979}{9.81} = 649.0\ \text{m}
$$

$p = \rho g h = 6.37\ \text{MPa}$ ($\approx 64.9\ \text{kg/cm}^2$).

#### (iv) Time of oscillation

$$
T = 2\pi\sqrt{\frac{4000 \times 176.71}{9.81 \times 50.27}} = 237.9\ \text{s} \approx 4.0\ \text{min}
$$

**Answer: up-surge 5.29 m; down-surge 5.16 m; water hammer head 649.0 m (6.37 MPa); $T = 237.9$ s.**

## Check yourself

The answer's key points as multiple-choice questions, with the correct option and why.

1. Which expression gives the frictionless surge amplitude Z0 in the tunnel-surge tank system?
   A. Z0 = V sqrt(L At / (g As))
   B. Z0 = V sqrt(L As / (g At))
   C. Z0 = V sqrt(g At / (L As))
   D. Z0 = V^2 / (2g)
   Answer: A. Z0 comes from equating the kinetic energy of the tunnel water to the potential energy gained in the tank, giving V sqrt(L At/(g As)). (Key point: Frictionless amplitude)

2. Which formula gives the period of mass oscillation of the surge tank?
   A. T = 2 pi sqrt(L At / (g As))
   B. T = 2 pi sqrt(L As / (g At))
   C. T = 4 L / a
   D. T = 2 L / a
   Answer: B. The mass oscillation period is 2 pi sqrt(L As/(g At)); 4L/a and 2L/a belong to the pressure wave in the penstock. (Key point: Period of oscillation)

3. Which expression gives the steady friction head loss hf used in the upsurge equation?
   A. hf = f L v^2 / (2 g d) for the penstock
   B. hf = a V / g
   C. hf = f L V^2 / (2 g D) for the tunnel
   D. hf = Z0^2 / L
   Answer: C. Only the tunnel friction acts on the tank oscillation, so hf = f L V^2/(2gD) with tunnel values (0.101 m here). (Key point: Steady friction loss in tunnel)

4. With a = 1600 m/s and v = 3.979 m/s per penstock, what is the water hammer head?
   A. About 5.3 m, from v^2 / 2g
   B. About 162 m, from a v / (4g)
   C. About 1298 m, from 2 a v / g
   D. About 649 m, from a v / g
   Answer: D. h = a v / g = 1600 x 3.979 / 9.81 = 649 m for rapid closure. (Key point: Water hammer pressure)

## Close variants set in other exams

- [Surge and water hammer: 60 m³/s, 30 m surge tank](https://www.bctengineer.com/question.md?key=semester_7%2Fhydropower_engineering%3Asurge-numerical-60cumec-3-penstocks-30m-tank) — Hydropower Engineering, chapter 6, asked 2×
- [Surge and water hammer: 45 m³/s, 20 m surge tank](https://www.bctengineer.com/question.md?key=semester_7%2Fhydropower_engineering%3Asurge-numerical-45cumec-3-penstocks) — Hydropower Engineering, chapter 6, asked 2×

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- [Surge numerical: 13 m tank, 1.8 km tunnel](https://www.bctengineer.com/question.md?key=semester_7%2Fhydropower_engineering%3Asurge-numerical-13m-tank-1-8km-tunnel) — Hydropower Engineering, chapter 6
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