Pressure head

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Pressure head is a term used in fluid mechanics to represent the internal energy of a fluid due to the pressure exerted on its container. It may also be called static pressure head or simply static head (but not static head pressure). It is mathematically expressed as:

$\psi = \frac{p}{\gamma} = \frac{p}{\rho \, g}$

where

ψ

is pressure head (Length, typically in units of m);

p

is fluid pressure (Force per unit Area, often as Pa units); and

γ

is the specific weight (Weight per unit volume, typically N·m⁻³ units)

ρ

is the density of the fluid (Mass per unit volume, typically kg·m⁻³)

g

is acceleration due to gravity (rate of change of velocity, given in m·s⁻²)

1 Practical uses for pressure head
2 Implications for gravitational anomalies on
3 See also
4 References

[edit] Practical uses for pressure head

A Venturi meter with two pressure instruments. (

p > 0

and

g > 0

) If the meter is turned upside down, we say by convention that

g < 0

and the fluid inside the vertical columns will pour out the two holes. See discussion below.

Fluid flow is measured with a wide variety of instruments. The venturi meter in the diagram on the right shows two columns of a measurement fluid at different heights. The height of each column of fluid is proportional to the pressure of the fluid. To demonstrate a classical measurement of pressure head, we could hypothetically replace the working fluid with another fluid having different physical properties.

For example, if the original fluid was water and we replaced it with mercury at the same pressure, we would expect to see a rather different value for pressure head. In fact, the specific weight of water is 9.8 kN/m³ and the specific weight of mercury is 133 kN/m³. So, for any particular measurement of pressure head, the height of the column of water will be about 13.6 times taller than the column of mercury would be (133/9.8 = 13.6). So if a water column meter reads "13.6 cm H₂O," then a coinciding measurement is "1.00 cm Hg."

This example demonstrates why there is a bit of confusion surrounding pressure head and its relationship to pressure. Scientists frequently use columns of water (or mercury) to measure pressure, since for a given fluid, pressure head is proportional to pressure. Measuring pressure in units of "mm of mercury" or "inches of water" makes sense for instrumentation, but these raw measurements of head must frequently be converted to more convenient pressure units using the equations above to solve for pressure.

In summary, pressure head is a measurement of length, which can be converted to the units of pressure, as long as strict attention is paid to the density of the measurement fluid and the local value of g.

[edit] Implications for gravitational anomalies on $\psi\,$

We would normally use pressure head calculations in areas in which $g$ is constant. However, if the gravitational field fluctuates, we can prove that pressure head fluctuates with it.

If we consider what would happens as gravity decreases, we would expect the fluid in the venturi meter shown above to withdraw from the pipe up into the vertical columns. Pressure head is increased.
In the case of zero gravity, the pressure head approaches infinity. Fluid in the pipe may "leak out" of the top of the vertical columns (assuming $p > 0$ ).
To simulate negative gravity, we could turn the venturi meter shown above upside down. In this case gravity is negative, and we would expect the fluid in the pipe to "pour out" the vertical columns. Pressure head is negative (assuming $p > 0$ ).
If $p < 0$ and $g > 0$ , we observe that the pressure head is also negative, and the ambient air is sucked into the columns shown in the venturi meter above. This is called a siphon, and is caused by a partial vacuum inside the vertical columns. In many venturis, the column on the left has fluid in it ( $ψ > 0$ ), while only the column on the right is a siphon ( $ψ < 0$ ).
If $p < 0$ and $g < 0$ , we observe that the pressure head is again positive, predicting that the venturi meter shown above would look the same, only upside down. In this situation, gravity causes the working fluid to plug the siphon holes, but the fluid doesn't leak out because the ambient pressure is greater than the pressure in the pipe.
The above situations imply that the Bernoulli equation, from which we obtain static pressure head, is extremely versatile.