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Archive / FAA Aviation Weather Handbook / FAA Aviation Weather Handbook: Chapter 8 — Atmospheric Pressure and Altimetry

Chapter 8 — Atmospheric Pressure and Altimetry, Part 1

Chapter 8 — Atmospheric Pressure and Altimetry — Part 1

FAA-H-8083-28B (2026)

Chapter 8, Atmospheric Pressure and Altimetry 8-1

8 Atmospheric Pressure and Altimetry

8.1 Introduction

Atmospheric pressure is one of the most basic variables used to describe the state of the atmosphere and is

commonly reported in weather observations. Unlike temperature and relative humidity, changes in

atmospheric pressure are not as readily sensed by people. However, variations of pressure across the Earth

are associated with pressure centers (either high -pressure centers or low -pressure centers) that cause the

wind to blow and can bring important weather changes. Density, which is directly related to pressure, is a

property of the atmosphere, which can be used by pilots to help determine how their aircraft will perform

at various altitudes.

This chapter discusses atmospheric pressure, how it is measured, and how it varies across the Earth. This

chapter also covers the altimeter, which is a pressure sensor used by pilots to determine altitude. Finally,

density will be discussed, along with its relationship to density altitude.

Chapter 8, Atmospheric Pressure and Altimetry 8-2

8.2 Atmospheric Pressure

The atoms and molecules that make up the various layers in the atmosphere are always moving in random

directions. Despite their tiny size, when they strike a surface, they exert pressure.

Each molecule is too small to feel and only exerts a tiny bit of pressure. However, when add ing up all the

pressures from the large number of molecules that strike a surface each moment, the total pressure is

considerable. This is air pressure. As the density of the air increases, the number of strikes per unit of time

and area also increases.

Since molecules move in all directions, they even exert air pressure upwards as they smash into objects

from underneath. Air pressure is exerted in all directions.

Atmospheric pressure is the force per unit area exerted by the weight of the atmosphere. Since air is not

solid, it cannot be weighed with conventional scales. Yet, three centuries ago, Evangelista Torricelli proved

he could weigh the atmosphere by balancing it against a column of mercury. He actually measured pressure,

converting it directly to weight.

Air is composed of matter and thus, has weight due to

the pull of Earth’s gravity.

Figure 8-1. Air Has Weight

8.2.1 Barometer

The instrument Torricelli designed to measure pressure was called a barometer. The aneroid barometer is

the type most commonly used by meteorologists and the aviation community.

Essential features of an aneroid barometer (see Figure 8-2) are a flexible metal cell and the registering

mechanism. Air is taken out of the cell to create a partial vacuum. The cell contracts or expands as pressure

changes. One end of the cell is fixed, while the other end moves the registering mechanism. The co upling

mechanism magnifies the movement of the cell driving an indicator hand along a scale graduated in

pressure units.

Chapter 8, Atmospheric Pressure and Altimetry 8-3

Figure 8-2. Aneroid Barometer

8.2.2 Atmospheric Pressure Units

Atmospheric pressure is expressed in many ways throughout the world (see Table 8-1). Meteorologists

worldwide have long measured atmospheric pressure in millibars (mb or mbar), which denote pressure as

a force per square centimeter. However, after the introduction of the Intern ational System of Units (SI)

in 1960, the hectopascal (hPa) was adopted by most countries and is used in the METAR/SPECI code first

developed in 1968. Many meteorologists prefer to use the term they learned during their education and

work experience. Therefore, some continue to use the term “millibars,” while others use “hectopascal”

(which are equivalent). The unit inch of mercury (inHg or Hg) is still used in the United States for altimetry.

Table 8-1. Units of Pressure

Units of Pressure Standard Atmosphere

Value at Sea Level Common Use

Hectopascals (hPa) 1013.2 hPa METAR/SPECI

Millibars (mb or mbar) 1013.2 mb U.S. Weather Charts

Inches of mercury (inHg or Hg) 29.92 inHg U.S. Aviation

Pounds per square inch (psi) 14.7 psi U.S. Engineering

8.2.3 Station Pressure

The pressure measured at an airport is called station pressure, or the actual pressure at field elevation.

Pressure is lower at higher altitudes. Therefore, airports with higher field elevations usually have lower

pressure than airports w ith lower field elevations. For instance, station pressure at Denver is less than at

New Orleans (see Figure 8-3).

Chapter 8, Atmospheric Pressure and Altimetry 8-4

Figure 8-3. Station Pressure

The next few sections will examine some factors that influence pressure.

8.2.4 Pressure Variation

Atmospheric pressure varies with altitude and the temperature of the air, as well as with other minor

influences, such as water vapor.

8.2.4.1 Pressure Changes with Altitude

As a person moves upward through the atmosphere, the weight of the air above the person decreases. If a

person carries a barometer, then they can measure a decrease in pressure as the weight of the air above them

decreases. Figure 8-4 shows the pressure decrease with height in the standard atmosphere.

The standard altitudes in Figure 8-4 are based on standard temperatures. In the real atmosphere,

temperatures are seldom standard, so temperature ’s effects on pressure will be explored in the following

section.

Chapter 8, Atmospheric Pressure and Altimetry 8-5

Figure 8-4. Air Pressure in the Standard Atmosphere

Chapter 8, Atmospheric Pressure and Altimetry 8-6

8.2.4.2 Temperature’s Effects on Pressure

Like most substances, air expands as it becomes warmer and contracts as it cools. Figure 8-5 shows three

columns of air: one colder than standard, one with standard temperature, and one warmer than standard.

Pressure is equal at the bottom and top of each column. Vertical expansion of the warm column has made

it taller than the column at standard temperature. Contraction of the cold column has made it shorter than

the standard column. Since the total pressure decrease is the same in each column, the rate of decrease of

pressure with height in warm air is less than standard, while the rate of decrease in pressure with height in

cold air is greater than standard.

Figure 8-5. Temperature’s Effect on Pressure

8.2.5 Sea Level Pressure

Since pressure varies greatly with altitude, people cannot readily compare station pressures between stations

at different altitudes. To make them comparable, they are adjusted to some common level. Mean sea level

(MSL) is the most useful common reference. In Figure 8-6, pressure measured at a station at a 5,000 -ft

elevation is 25 inHg; pressure increases about 1 inHg for each 1,000 ft, or a total of 5 inHg. Sea level

pressure is approximately 25 + 5, or 30 inHg.

Figure 8-6. Reduction of Station Pressure to Sea Level

Chapter 8, Atmospheric Pressure and Altimetry 8-7

Sea level pressure is typically displayed on surface weather charts. Pressure continually changes across the

Earth, so a sequence of surface charts must be viewed to follow these changing pressures.

8.3 Density

Density is the ratio of any quantity to the volume or area it occupies. Atmospheric density is defined as

ratio of the mass (or weight) of the air to the volume occupied by it, usually expressed in kilograms per

cubic meter (see Figure 8-7).

Figure 8-7. Density is Mass (Weight) per Volume

8.3.1 Volume’s Effects on Density

The density of an air parcel varies inversely with its volume. Assuming equal mass, an air parcel with a

higher density has a smaller volume than an air parcel with a lower density (see Figure 8-8).

The shorter parcel (i.e., the parcel with the smaller volume) has a higher density than the taller parcel, which

contains the larger volume. This is due to the fact that the air molecules within the shorter parcel must be

compressed within the smaller volume.

Chapter 8, Atmospheric Pressure and Altimetry 8-8

Figure 8-8. Volume’s Effects on Density

8.3.2 Changes in Density

In general, the density of an air parcel can be changed by changing its mass, pressure, or temperature.

Boyle’s law says that the density of an ideal gas (ρ, the Greek letter rho) is given by:

𝜌 = 𝑀𝑃

𝑅𝑇

Where M is the molar mass, P is the pressure, R is the universal gas constant, and T is the absolute

temperature.

8.3.3 Density’s Effects on Pressure

Density is directly related to pressure. Assuming constant mass and temperature, an air parcel with a higher

pressure is denser than an air parcel with a lower pressure.

As previously discussed, air pressure decreases with height in the atmosphere. Therefore, the density also

decreases with height (see Figure 8-9). In the atmosphere, pressure has the greatest effect on density in the

vertical direction.

Original source PDFPublished from pages 95–102 of the recorded source chapter.
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