Water hammer 

Water hammer (or, more generally, fluid hammer) is a pressure surge or wave resulting when a fluid in motion is forced to stop or change direction suddenly (momentum change). Water hammer commonly occurs when a valve is closed suddenly at an end of a pipeline system, and a pressure wave propagates in the pipe.

Contents

The magnitude of the pulse

The size of the water hammer pulse can be estimated from the Joukowsky equation 1

ΔP = ρaΔC

Where ΔP is the magnitude of the pressure wave (Pa), ρ is the density of the fluid (kgm−3), a is the speed of sound in the fluid (ms−1), and ΔC is the change in the fluid's velocity (ms−1). The pulse comes about due to Newton's laws of motion and the continuity equation applied to the deceleration of a fluid element 2.


As the speed of sound in a fluid is the \sqrt{\frac{\text{effective bulk modulus}} {\text{density}}} , the peak pressure will depend on the fluid compressibility.

One approximation to the maximum pressure (using Imperial units), P, produced in a water filled line is:

P = 0.07VL / t + P1

Where P1 is the inlet pressure, V is the flow velocity in ft/sec, t is the valve closing time in seconds and L is the upstream pipe length in feet 3

For this reason, pipe-sizing charts for some applications recommend flow velocity at or below 5 ft/s (1.5 m/s). If the pipe is suddenly closed at the outlet (downstream), the mass of water before the closure is still moving forward with some velocity, building up a high pressure and shock waves. In domestic plumbing this is experienced as a loud bang resembling a hammering noise. Water hammer can cause pipelines to break if the pressure is high enough. Air traps or stand pipes (open at the top) are sometimes added as dampers to water systems to provide a cushion to absorb the force of moving water in order to prevent damage to the system. (At some hydroelectric generating stations what appears to be a water tower is actually one of these devices.)

On the other hand, when a valve in a pipe is closed, the water downstream of the valve will attempt to continue flowing, creating a vacuum that may cause the pipe to collapse or implode. This problem can be particularly acute if the pipe is on a downhill slope. To prevent this, air and vacuum relief valves, or air vents, are installed just downstream of the valve to allow air to enter the line and prevent this vacuum from occurringcitation needed.

In the home water hammer often occurs when a dishwasher, washing machine, or toilet shuts off water flow, resulting in a loud bang or banging sound. A hydropneumatic device similar in principle to a shock absorber called a 'Water Hammer Arrestor' can be installed between the water pipe and the machine which will absorb the shock and stop the banging.

Expansion joints on a steam line that have been destroyed by steam hammer

Steam distribution systems may also be vulnerable to a situation similar to water hammer, known as steam hammer. In a steam system, water hammer most often occurs when some of the steam condenses into water in a horizontal section of the steam piping. Subsequently, steam picks up the water, forms a "slug" and hurls it at high velocity into a pipe fitting, creating a loud hammering noise and greatly stressing the pipe. This condition is usually caused by a poor condensate drainage strategy.

Where air filled traps are used, these eventually become depleted of their trapped air over a long period of time through absorption into the water. This can be cured by shutting off the supply and draining the system by opening taps at the highest and lowest locations, which restores the air to the traps and then closing the taps and opening the supply.

Hydroelectric power plants must be carefully designed and maintained because the water hammer can cause water pipes to fail catastrophically. One of the first to successfully investigate the water hammer problem was the Italian engineer Lorenzo Allievi.

Dynamic Equations

The water hammer effect can be simulated by solving the following partial Differential equations.

 \frac{\partial V}{\partial x}+ \frac{1}{B_m}.\frac{\partial P}{\partial t}=0\,
 \frac{\partial V}{\partial t}+ \frac{1}{\rho}.\frac{\partial P}{\partial x}+\frac{f}{2d}v|v|=0\,

Where, V is the fluid velocity inside pipe, ρ is the fluid density and Bm is the equivalent bulk modulus, f is the friction factor.

Possible causes

Software

Most water hammer software packages use the method of characteristics 2 to solve the differential equations involved. This method works well if the wave speed does not vary in time due to either air or gas entrainment in a pipeline. Many commercial and non commercial packages exist today.

Software packages vary in complexity, dependent on the processes modeled. The more sophisticated packages may have any of the following features:

Mitigating measures

Water hammer has caused accidents and fatalities, but is usually less threatening. In many cases damage is limited to breakage of pipes or appendages. An engineer should always assess (at least qualitatively) risk of a pipeline burst. Pipelines with hazardous goods should always receive special attention and should be thoroughly investigated.

The following characteristics may reduce or eliminate water hammer:

Applications

See also

References

  1. ^ Thorley, ADR, Fluid Transients in Pipelines, 2nd ed. Professional Engineering Publishing, 2004
  2. ^ a b Streeter, VL and Wylie, EB, Fluid mechanics, McGraw-Hill Higher Education; International 9th Revised Ed edition, 1998
  3. ^ "Water Hammer & Pulsation"

External links