# 2.2: The Atmosphere’s Pressure Structure - Hydrostatic Equilibrium

- Page ID
- 3356

The atmosphere’s vertical pressure structure plays a critical role in weather and climate. We all know that pressure decreases with height, but do you know why?

**Air parcel at rest with three forces in balance**

The atmosphere’s basic pressure structure is determined by the __hydrostatic balance of forces__. To a good approximation, every air parcel is acted on by three forces that are in balance, leading to no net force. Since they are in balance for any air parcel, the air can be assumed to be static or moving at a constant velocity.

There are **3 forces****that determine hydrostatic balance:**

- One force is downwards (negative) onto the top of the cuboid from the pressure,
, of the fluid above it. It is, from the definition of*p*__pressure,__

\(F_{t o p}=-p_{t o p} A\)

2. Similarly, the force on the volume element from the pressure of the fluid below pushing upwards (positive) is:

\(F_{\text {bottom}}=p_{\text {bottom}} A\)

3. Finally, the __weight__ of the volume element causes a force downwards. If the __density__ is ρ, the volume is * V*, which is simply the horizontal area

*times the vertical height,*

*A**, and*

*Δz**the*

*g*__standard gravity__, then:

\(F_{\text {weight}}=-\rho V g=-\rho g A \Delta z\)

By balancing these forces, the ** total force on the fluid** is:

\(\sum F=F_{b o t t o m}+F_{t o p}+F_{w e i g h t}=p_{b o t t o m} A-p_{t o p} A-\rho \mathrm{gA} \Delta z\)

This sum equals zero if the air's velocity is constant or zero. Dividing by * A*,

\(0=p_{b o t t o m}-p_{t o p}-\rho g \Delta z\)

or:

\(p_{t o p}-p_{b o t t o m}=-\rho g \Delta z\)

* P_{top} − P_{bottom}* is a change in pressure, and Δz is the height of the volume element – a change in the distance above the ground. By saying these changes are

__infinitesimally__small, the equation can be written in

__differential__form, where

*is top pressure minus bottom pressure just as dz is top altitude minus bottom altitude.*

*dp*\(d p=-\rho g d z\)

The result is the equation:

\(\frac{d p}{d z}=-\rho g\)

This equation is called the ** Hydrostatic Equation**. See the video below (1:18) for further explanation:

**Hydrostatic Equation**

**Click here for transcript of the Hydrostatic Equation video.**-
Consider an air parcel at rest. There are three forces in balance, the downward pressure force, which is pressure times area in the parcel's top, and an upward pressure force on the parcel's bottom, and the downward force of gravity actually on the parcel's mass, which is just the acceleration due to gravity times the parcel's density times it's volume. The volume equals the parcel's cross sectional area times its height. We can sum these three forces together and set them equal to 0 since the parcel's at rest. Notice how the cross sectional area can be divided out. The next step is to put the pressure difference on the left hand side. And then shrink the air parcel height to be infinitesimally small, which makes the pressure difference infinitesimally small. By dividing both sides by the infinitesimally small height, we end up with an equation that's the derivative of the pressure with respect to height, which is equal to minus the parcel's density times gravity. This equation is the hydrostatic equation, which describes a change of atmospheric pressure with height.

Using the Ideal Gas Law, we can replace * ρ* and get the equation for dry air:

\(\frac{d p}{d z}=-g \frac{p}{R_{d} T} \quad\) or \(\quad \frac{d p}{p}=-\frac{g}{R_{d} T} d z=-\frac{M g}{R^{*} T} d z\)

We could integrate both sides to get the altitude dependence of * p*, but we can only do that if

*is constant with height. It is not, but it does not vary by more than about ±20%. So, doing the integral,*

*T*\(p=p_{o} e^{-z / H} \quad\) where \(p_{o}=\) surf ace pressure and \(H=\frac{R^{*} \overline{T}}{M_{\text {air}} g}\)

* H* is called a scale height because when

*, we have*

*z = H**=*

*p**e*

*p*_{o}^{–1}. If we use an average

*of 250 K, with*

*T**= 0.029 kg mol*

*M*_{air}^{–1}, then

*= 7.2 km. The pressure at this height is about 360 hPa, close to the 300 mb surface that you have seen on the weather maps. Of course the forces are not always in hydrostatic balance and the pressure depends on temperature, thus the pressure changes from one location to another on a constant height surface.*

*H*From the hydrostatic equation, the atmospheric pressure falls off exponentially with height, which means that about every 7 km, the atmospheric pressure is about 1/3 less. At 40 km, the pressure is only a few tenths of a percent of the surface pressure. Similarly, the concentration of molecules is only a few tenths of a percent, and since molecules scatter sunlight, you can see in the picture below that the scattering is much greater near Earth's surface than it is high in the atmosphere.

Scattered light near Earth's surface.

Credit: NASA

### Quiz 2-2: Harnessing the power of the hydrostatic equation

This quiz will give you practice using the hydrostatic equation to learn interesting and useful properties and quantities of the atmosphere.

*I strongly suggest that you do all your calculations on this quiz using the Excel workbook.*- There is no
. However, you have extra time to take this quiz.**Practice Quiz 2-2** - When you feel you are ready, take
in Canvas. You will be allowed to take this quiz only**Quiz 2-2**. This quiz is timed, so after you start, you will have a limited amount of time to complete it and submit it. Good luck!**once**