If your ears have ever popped on a plane flight or ached during a deep dive in a swimming pool, you have experienced the effect of depth on pressure in a fluid. At the Earth’s surface, the air pressure exerted on you is a result of the weight of air above you. This pressure is reduced as you climb up in altitude and the weight of air above you decreases. Under water, the pressure exerted on you increases with increasing depth. In this case, the pressure being exerted upon you is a result of both the weight of water above you *and* that of the atmosphere above you. You may notice an air pressure change on an elevator ride that transports you many stories, but you need only dive a meter or so below the surface of a pool to feel a pressure increase. The difference is that water is much denser than air, about 775 times as dense.

Consider the container in Figure 11.9. Its bottom supports the weight of the fluid in it. Let us calculate the pressure exerted on the bottom by the weight of the fluid. That pressure is the weight of the fluid $\text{mg}$ divided by the area $A$ supporting it (the area of the bottom of the container):

We can find the mass of the fluid from its volume and density:

The volume of the fluid $V$ is related to the dimensions of the container. It is

where $A$ is the cross-sectional area and $h$ is the depth. Combining the last two equations gives

If we enter this into the expression for pressure, we obtain

The area cancels, and rearranging the variables yields

This value is the *pressure due to the weight of a fluid*. The equation has general validity beyond the special conditions under which it is derived here. Even if the container were not there, the surrounding fluid would still exert this pressure, keeping the fluid static. Thus the equation $P=\mathrm{h\rho g}$ represents the pressure due to the weight of any fluid of *average density* $\rho $ at any depth $h$ below its surface. For liquids, which are nearly incompressible, this equation holds to great depths. For gases, which are quite compressible, one can apply this equation as long as the density changes are small over the depth considered. Example 11.4 illustrates this situation.

### Example 11.3

#### Calculating the Average Pressure and Force Exerted: What Force Must a Dam Withstand?

In Example 11.1, we calculated the mass of water in a large reservoir. We will now consider the pressure and force acting on the dam retaining water. (See Figure 11.10.) The dam is 500 m wide, and the water is 80.0 m deep at the dam. (a) What is the average pressure on the dam due to the water? (b) Calculate the force exerted against the dam and compare it with the weight of water in the dam (previously found to be $1.96\times {10}^{13}\phantom{\rule{0.25em}{0ex}}\text{N}$).

#### Strategy for (a)

The average pressure $\overline{P}$ due to the weight of the water is the pressure at the average depth $\overline{h}$ of 40.0 m, since pressure increases linearly with depth.

#### Solution for (a)

The average pressure due to the weight of a fluid is

Entering the density of water from Table 11.1 and taking $\overline{h}$ to be the average depth of 40.0 m, we obtain

#### Strategy for (b)

The force exerted on the dam by the water is the average pressure times the area of contact:

#### Solution for (b)

We have already found the value for $\overline{P}$. The area of the dam is $A=\text{80.0 m}\times \text{500 m}=4.00\times {\text{10}}^{4}\phantom{\rule{0.25em}{0ex}}{\text{m}}^{2}$, so that

#### Discussion

Although this force seems large, it is small compared with the $1.96\times {\text{10}}^{\text{13}}\phantom{\rule{0.25em}{0ex}}\text{N}$ weight of the water in the reservoir—in fact, it is only
$\mathrm{0.0800\%}$ of the weight. Note that the pressure found in part (a) is completely independent of the width and length of the lake—it depends only on its average depth at the dam. Thus the force depends only on the water’s average depth and the dimensions of the dam, *not* on the horizontal extent of the reservoir. In the diagram, the thickness of the dam increases with depth to balance the increasing force due to the increasing pressure.epth to balance the increasing force due to the increasing pressure.

*Atmospheric pressure* is another example of pressure due to the weight of a fluid, in this case due to the weight of *air* above a given height. The atmospheric pressure at the Earth’s surface varies a little due to the large-scale flow of the atmosphere induced by the Earth’s rotation (this creates weather “highs” and “lows”). However, the average pressure at sea level is given by the *standard atmospheric pressure* ${P}_{\text{atm}}$, measured to be

This relationship means that, on average, at sea level, a column of air above $1.00\phantom{\rule{0.25em}{0ex}}{\text{m}}^{2}$ of the Earth’s surface has a weight of $1.01\times {\text{10}}^{5}\phantom{\rule{0.25em}{0ex}}\text{N}$, equivalent to $\text{1 atm}$. (See Figure 11.11.)

### Example 11.4

#### Calculating Average Density: How Dense Is the Air?

Calculate the average density of the atmosphere, given that it extends to an altitude of 120 km. Compare this density with that of air listed in Table 11.1.

#### Strategy

If we solve $P=\mathrm{h\rho g}$ for density, we see that

We then take $P$ to be atmospheric pressure, $h$ is given, and $g$ is known, and so we can use this to calculate $\overline{\rho}$.

#### Solution

Entering known values into the expression for $\overline{\rho}$ yields

#### Discussion

This result is the average density of air between the Earth’s surface and the top of the Earth’s atmosphere, which essentially ends at 120 km. The density of air at sea level is given in Table 11.1 as $1\text{.}\text{29}\phantom{\rule{0.25em}{0ex}}{\text{kg/m}}^{3}$ —about 15 times its average value. Because air is so compressible, its density has its highest value near the Earth’s surface and declines rapidly with altitude.

### Example 11.5

#### Calculating Depth Below the Surface of Water: What Depth of Water Creates the Same Pressure as the Entire Atmosphere?

Calculate the depth below the surface of water at which the pressure due to the weight of the water equals 1.00 atm.

#### Strategy

We begin by solving the equation $P=\mathrm{h\rho g}$ for depth $h$:

Then we take $P$ to be 1.00 atm and $\rho $ to be the density of the water that creates the pressure.

#### Solution

Entering the known values into the expression for $h$ gives

#### Discussion

Just 10.3 m of water creates the same pressure as 120 km of air. Since water is nearly incompressible, we can neglect any change in its density over this depth.

What do you suppose is the *total* pressure at a depth of 10.3 m in a swimming pool? Does the atmospheric pressure on the water’s surface affect the pressure below? The answer is yes. This seems only logical, since both the water’s weight and the atmosphere’s weight must be supported. So the *total* pressure at a depth of 10.3 m is 2 atm—half from the water above and half from the air above. We shall see in Pascal’s Principle that fluid pressures always add in this way.