Head pressure

, 5 min, 900 words

Tags: fire-stuff physics

Head pressure is the pressure created by a difference in height between where water is coming from and a discharge. It's important for things like how much pressure you'll get from a hydrant or how much pressure you lose if you're pumping up a steep driveway. If you read a textbook, it'll say something like

To convert head in feet to head pressure in psi, divide the number of feet by 2.304.

IFSTA Pumping Apparatus – Driver/Operator Handbook, 1999 (!!)

This is me proving to myself that that works. (Spoiler alert: it does.)

So, we're going to start with the same simplification I made last time by converting a reservoir and some complex series of pipes into a single vertical stack of water. I've convinced myself that this will result in the same discharge pressure, though articulating why is still hard. Here's what the simplification looks like, though:

A schematic of a water tank on top of a hill providing pressure to a discharge a distance h below, alongside a simplified version with just a vertical stack of water of height h.

Okay, so given $h$, we want to calculate the pressure at the bottom of this tube. Awesome. Let's start with the easy stuff.

Let's say the cross-sectional area of the tube is $A$. Then the volume of water contained in the tube is:

$$ V = h\cdot A $$

If the density of water is $\rho$, then the mass of this water is:

$$ m = V\cdot\rho = h\cdot A\cdot\rho $$

(Note: I will use italicised $m$ for mass, and a non-italicized $\text{m}$ for meters. This is more generally true – units here will be non-italicized, while variables will look like variables.)

Okay, and the force resulting from all this water pushed down by gravity will be $F=mg$, or

$$ F = h\cdot A\cdot\rho\cdot g $$

Finally, pressure is force per area. So the pressure at the bottom of the tube is

$$ P = \frac{F}{A} = h\cdot\rho\cdot g $$

(Thank goodness, the cross-section of the tube doesn't matter.)

A quick note on the units of pressure. In SI units, pressure is measured in Pascals, which are Newtons per square meter:

$$ 1\ \text{Pa}=1\frac{\text{N}}{\text{m}^2}=1\frac{\frac{\text{kg}\cdot\text{m}}{\text{s}^2}}{\text{m}^2} =1\frac{\text{kg}}{\text{m}\ \text{s}^2} $$

In imperial units, pressure is measured in pounds per square inch (psi). Or, more properly, in pounds-force per square inch. (Pet peeve: anything to do with a system where "pounds" can mean two wildly different things with different units and that don't actually convert between each other with any simple/memorable conversion factor.)

Substituting in values for water's density and the acceleration due to the Earth's gravity:

\begin{align} P &= h\rho g\\ &= h\cdot\frac{1\ \text{kg}} {1000\ \text{cm}^3}\cdot\left(9.81\ \frac{\text{m}}{\text{s}^2}\right) \end{align}

We're now going to multiply our pressure by one in many different forms to convert from imperial units (feet) to SI and then back to imperial.

\begin{align} P &= h\rho g\\ &= h\cdot\frac{1\ \text{kg}} {1000\ \text{cm}^3}\cdot\left(9.81\ \frac{\text{m}}{\text{s}^2}\right)\\ &= h\cdot\frac{1\ \text{kg}} {1000\ \text{cm}^3}\cdot\left(9.81\ \frac{\text{m}}{\text{s}^2}\right) \cdot\left(\frac{100\ \text{cm}}{1\ \text{m}}\right)^3\\ &= h\cdot9,800\cdot\frac{\text{kg}\cdot\text{m}}{\text{m}^3\ \text{s}^2}\\ &= \frac{h}{\text{m}}\cdot 9,800\cdot\frac{\text{kg}}{\text{m}\ \text{s}^2}\\ &= \frac{h}{\text{m}}\cdot 9,800\cdot\text{Pa} \end{align}

Note that the units still work – as long as $h$ has a length-like dimension (say, feet or meters), we end with a unit of pressure, phew! Now back to psi:

\begin{align} P &= \frac{h}{\text{m}}\cdot 9,800\cdot\text{Pa}\\ &= \frac{h}{\text{m}}\cdot 9,800\ \frac{\text{N}}{\text{m}^2} \cdot\left(\frac{1\ \text{ft}}{12\ \text{in}}\cdot \frac{1\ \text{m}}{3.3\ \text{ft}}\right)^2\\ &= \frac{h}{\text{m}}\cdot 6.3\ \frac{\text{N}}{\text{in}^2}\\ &= \frac{h}{\text{m}}\cdot 6.3\ \frac{\text{N}}{\text{in}^2} \cdot\frac{1\ \text{lbf}}{4.45\ \text{N}}\\ &= \frac{h}{\text{m}}\cdot 1.4\ \frac{\text{lbf}}{\text{in}^2}\\ &= \frac{h}{\text{m}}\cdot 1.4\ \text{psi}\\ &= \frac{h}{\text{m}}\cdot\frac{1\ \text{m}}{3.3\ \text{ft}}\cdot 1.4\ \text{psi}\\ &= \frac{h}{\text{ft}}\cdot 0.4\ \text{psi}\\ &= \frac{h}{\text{ft}}\cdot\frac{1}{2.3}\ \text{psi} \end{align}

And would you look at that! If you have a height difference of, say 100 feet, then $h/\text{ft}$ is 100, and your resulting head pressure is $100/2.3\ \text{psi} = 43\ \text{psi}$.

As a side note, because everything is better in SI units, when it comes to a head measured in meters, you can convert to kPa by just multiplying the height (in meters) by ten. #SIforlife

(Is this likely to be useful to anyone but me? No. Too bad. My blog, my rules.)