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Archive / FAA Aviation Weather Handbook / FAA Aviation Weather Handbook: Chapter 15 — Weather Radar

Chapter 15 — Weather Radar, Part 2

Chapter 15 — Weather Radar — Part 2

FAA-H-8083-28B (2026)

Chapter 15, Weather Radar 15-8

15.2.7.1 Normal (Standard) Refraction

Under normal (i.e., standard) conditions, the atmosphere ’s density gradually decreases with increasing

height. As a result, the upper portion of a radar beam travels faster than the lower portion of the beam. This

causes the beam to bend downward (see Figure 15-8).

The radar beam curvature is less than the curvature of the Earth. Therefore, the height of the radar beam

above the Earth’s surface increases with an increasing range.

Figure 15-8. Normal Refraction

15.2.7.2 Subrefraction

Atmospheric conditions are never normal or standard. Sometimes, the density of the atmosphere decreases

with height at a more -than-normal rate (actual density is less than normal) . When this occurs, the radar

beam bends less than normal and climbs skyward. This phenomenon is known as subrefraction (see Figure

15-9).

Subrefraction may cause the radar beam to overshoot objects that would normally be detected. For example,

distant thunderstorms may not be detected with subrefraction. Subrefraction may also cause radar to

underestimate the true strength of a thunderstorm. Thunderstorms may appear weaker on radar because

subrefraction causes the radar beam to strike the thunderstorm near the top of the cumulonimbus cloud,

where the precipitation particles tend to be smaller.

Chapter 15, Weather Radar 15-9

Figure 15-9. Subrefraction

15.2.7.3 Superrefraction

Conversely, sometimes the density of the atmosphere decreases with height at a less -than-normal rate

(actual density is greater than normal) or even increases with height. When this occurs, the radar beam will

bend more than normal toward the Earth’s surface. This phenomenon is called superrefraction (see Figure

15-10).

Superrefraction causes the radar beam to travel closer to the Earth ’s surface than what would occur in a

normal atmosphere. This can lead to overestimating the strength of a thunderstorm, as the beam would

detect the stronger core of the storm, where precipitation-sized particles are larger.

Figure 15-10. Superrefraction

15.2.7.4 Ducting

If the atmospheric condition that causes superrefraction bends the beam equal to, or greater than, the Earth’s

curvature, then a condition called ducting (or trapping) occurs (see Figure 15-11).

When ducting occurs, the radar beam will hit the surface of the Earth, causing some of the beam ’s energy

to backscatter. This often leads to false echoes, also known as anomalous propagation (AP), to appear in

the radar display.

Chapter 15, Weather Radar 15-10

Figure 15-11. Ducting

15.2.8 Radar Beam Overshooting and Undershooting

Radar beam overshooting may occur because the lowest radar beam can be higher than the top of

precipitation. This will most likely occur with stratiform precipitation and low -topped convection. For

example, at a distance of 124 NM from the radar, the lowest radar beam is at an altitude of approximately

18,000 ft; at 248 NM the beam height is approximately 54,000 ft. Any precipitation with tops below these

altitudes and distances will not be displayed on a single-site radar image. Therefore, it is quite possible that

precipitation may be occurring where none appears on the single-site radar image.

Radar overshooting occurs more often in the mountainous western U nited States where some radars are

located on a mountaintop (e.g., the WSR-88D near Cedar City, UT).

Radar undershooting occurs when precipitation occurs above the lowest radar beam, usually with

high-cloud-based precipitation near the radar site. This often occurs in the western United States during the

summer months.

Undershooting may occur at and near the radar site even in mosaic products when the precipitation is above

the highest elevation angle. This region above the radar is known as the “cone of silence ” (see Figure

15-12).

Figure 15-12. Cone of Silence

Chapter 15, Weather Radar 15-11

15.2.9 Beam Blockage

Beam blockage (see Figure 15-13) occurs when the radar beam is blocked by terrain and is particularly

predominant in mountainous terrain. See Section 24.6.1 for more information on the WSR-88D.

Beam blockage is most easily seen on the lowest radar beam (also known as “Base Reflectivity,” “Lowest

Tilt,” and “Reflectivity at Lowest Altitude ”) images where it appears as a pie -shaped area (or areas)

perpetually void of echoes. When animating the imagery, the beam blockage area will remain clear of

echoes even as precipitation and other targets pass through. In many cases, the beam blockage effect seen

on a single-site radar can be minimized by viewing mosaic images.

Figure 15-13. WSR-88D Weather Radar Beam Blockage on Base Reflectivity Product Example

15.2.10 Ground Clutter

Ground clutter (see Figure 15-14) is radar echoes ’ returns from trees, buildings, or other objects on the

ground. It appears as a roughly circular region of high reflectivity at ranges close to the radar. Ground

clutter appears stationary when animating images and can mask precipitation located near the r adar. Most

ground clutter is automatically removed from WSR-88D imagery, so typically it is does not interfere with

image interpretation.

Chapter 15, Weather Radar 15-12

Figure 15-14. WSR-88D Weather Radar Ground Clutter Example

15.2.11 Ghost

A ghost (see Figure 15-15) is a diffused echo in apparently clear air caused by a “cloud” of point targets,

such as insects, or by refraction returns of the radar beam in truly clear air.

The latter case commonly develops at sunset due to superrefraction during the warm season. The ghost

develops as an area of low reflectivity echoes (typically less than 15 decibels of Z ( dBZ)) near the radar

site and quickly expands. When animating the imagery, the ghost echo shows little movement.

Chapter 15, Weather Radar 15-13

Figure 15-15. WSR-88D Weather Radar Ghost Example

15.2.12 Angels

Angels are echoes caused by a physical phenomenon not discernible by the eye at the radar site. They are

usually caused by bats, birds, or insects. Angels typically appear as a donut -shaped echo with low

reflectivity values (see Figure 15-16). When animated, the echo expands and becomes more diffuse

with time.

Angels typically only appear when the WSR-88D radar is in Clear Air Mode because of their weak

reflectivity (see Section 24.6.1.3 for additional information on modes). Echoes caused by birds are typically

detected in the morning when they take flight for the day. Echoes caused by bats are typically detected in

the evening when they are departing from caves.

Original source PDFPublished from pages 178–183 of the recorded source chapter.
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