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EARTH EXPLAINED · LESSON GUIDE

Why Hurricanes Spin

The engine, the eye and the Coriolis effect

Video 8:51Level Grades 6–12 · Introductory university meteorologyStandards MS-ESS2-4, MS-ESS2-5, MS-ESS2-6, MS-ESS3-2, HS-ESS3-1
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What powers a hurricane, and why does every one north of the equator turn counter-clockwise while every one south of it turns clockwise?

A hurricane is a heat engine that runs on warm sea water and takes its spin from the turning Earth. This lesson follows the episode from the fuel (sea water of at least 26.5 °C) and the self-feeding cycle of evaporation and condensation, through the Coriolis effect that winds the inflowing air into a spiral, to the calm eye and the violent eyewall around it. It then turns to people: why storms have names, what the Galveston hurricane of 1900 and Hurricane Katrina in 2005 revealed about storm surge, and how three-day track forecasts improved from misses of more than 350 miles in 1990 to about 100 miles in the mid-2020s, while sudden strengthening remains hard to predict.

Captions (.vtt)Captions (.srt)

Learning objectives After this lesson, students can:

  1. Explain how a hurricane works as a heat engine: warm water evaporates, moist air rises, its vapor condenses, and the heat released drives the air upward faster, drawing in more moist air.
  2. State the ocean conditions a hurricane needs (sea surface at least 26.5 °C, about 80 °F, warm to a depth of about 50 m) and use them to explain why the Atlantic season peaks in late summer.
  3. Describe the Coriolis effect and use it to predict the direction a storm turns in each hemisphere, and explain why hurricanes almost never form within about 5° of the equator.
  4. Describe the structure of a mature hurricane, including the spiral bands, the eyewall and the eye, and explain why the wind drops and then returns from the opposite direction as the eye passes.
  5. Explain why tropical cyclones are named, how the Atlantic name lists rotate, and why some names are retired.
  6. Compare the Galveston hurricane of 1900 and Hurricane Katrina in 2005, and use them to explain why storm surge, not wind category alone, often determines how deadly a hurricane is.
  7. Interpret a forecast cone correctly, and evaluate how much track forecasts have improved compared with forecasts of strength, using rapid intensification as the example.

Before watching

Key vocabulary ★ extension terms for older students

Tropical cyclone
A large, rotating storm system with a warm center that forms over tropical or subtropical seas. When its sustained winds reach 74 mph (119 km/h), it is called a hurricane in the Atlantic and the eastern and central North Pacific, a typhoon in the western North Pacific, and a cyclone in the South Pacific and Indian Ocean.
Heat engine
A system that turns heat into motion. A hurricane takes heat from the warm sea surface and turns a small part of it into wind.
Condensation
The change of water vapor into liquid droplets, which forms cloud. It releases the heat that was absorbed when the water evaporated, and that heat is the hurricane's main source of energy.
Coriolis effect
The apparent deflection of anything that travels a long way across the surface of the rotating Earth: to the right in the Northern Hemisphere and to the left in the Southern. It is zero at the equator and strongest at the poles.
Spiral bands
The long, curved bands of cloud and rain that spiral in toward a hurricane's center; their curve shows which way the storm is turning.
Eye
The roughly circular area of light winds at the center of a strong hurricane, usually 30 to 60 km across. The air inside it sinks, so the sky can be partly clear.
Eyewall
The ring of towering thunderstorm clouds around the eye, where a hurricane's strongest winds and heaviest rain are found.
Millibar
A unit of air pressure, equal to one hectopascal (hPa). Average sea-level pressure is about 1,013 mb; the lowest sea-level pressure ever measured, 870 mb, was in the eye of Typhoon Tip in 1979.
Storm surge
The rise of the sea above the normal tide, pushed ashore mainly by a storm's winds. It is usually the deadliest part of a hurricane.
Levee
An embankment or wall built to hold back water from a river, lake or sea. In New Orleans in 2005, levees and floodwalls failed, and lake and canal water flooded most of the city.
Cone of uncertainty
The forecast graphic that shows where the center of a storm will probably go. The center stays inside it about two times out of three. It does not show the size of the storm or where its impacts will be felt.
Rapid intensification
An increase in a tropical cyclone's maximum sustained winds of at least 30 knots (35 mph, 55 km/h) within 24 hours.
Retired name
A storm name removed from the rotating lists by the World Meteorological Organization because the storm was so deadly or costly that reusing the name would be inappropriate.
Latent heat★
The heat absorbed when water evaporates and released again when the vapor condenses, about 2.5 million joules for every kilogram of water. It carries energy from the sea surface into the storm.
Pressure gradient force★
The push on air from higher toward lower pressure. It drives air in toward a hurricane's center; the Coriolis effect then bends that inflow into rotation.
Saffir-Simpson Hurricane Wind Scale★
The 1-to-5 rating of a hurricane based only on its maximum sustained wind, from Category 1 (74 to 95 mph, 119 to 153 km/h) to Category 5 (157 mph, 252 km/h, or more). It does not account for storm surge, rainfall flooding or tornadoes.

Chapter outline Select a time to play from there

0:00The Engine

A hurricane is a heat engine that runs on warm sea water, at least 26.5 °C (about 80 °F) and warm to a depth of about 50 meters. Evaporation, rising air and condensation feed one another, and in a single day an average hurricane releases more than a hundred times as much heat as all the electricity the world generates.

1:45Why It Spins

Air flows in toward the low pressure at the center, and the Coriolis effect bends it to the right in the Northern Hemisphere and to the left in the Southern, so storms turn counter-clockwise in the north and clockwise in the south. Within about 5° of the equator the effect is too weak to start a storm turning.

2:49The Eye

Hurricane Patricia (2015), whose 215 mph (345 km/h) winds are the strongest measured in a hurricane, and the eye of Isabel (2003): sinking air and light winds in the eye, the strongest winds in the eyewall. Typhoon Tip (1979) holds the records for the lowest sea-level pressure, 870 mb, and the largest size, about 2,220 km across.

4:10The Names

Atlantic storms have been named since 1950, with women's names from 1953 and men's names added in 1979. Six lists of 21 names rotate, so each name returns every six years unless a storm is so deadly or costly that its name is retired.

5:061900 and 2005

In 1900 a storm surge of more than 15 feet swept over Galveston, where nobody could see how strong the storm had grown, killing about 8,000 people; the city rebuilt behind a seawall and raised itself. In 2005 Katrina's surge broke through the levees and floodwalls of New Orleans, flooding 80 percent of the city: nearly 1,400 deaths and $125 billion in damage.

6:52The Forecast

The forecast cone shows where the center will probably go, not the storm's size. Three-day track errors fell from more than 350 miles in 1990 to about 100 miles in the mid-2020s, but rapid intensification, as in Hurricane Milton (2024), remains hard to predict.

8:00Still Spinning

Cyclone Winston (2016), in the South Pacific, turns clockwise on the same engine. The summary: a heat engine on warm water, a spin from Earth's rotation, and tracks forecast far better than strength.

Common misconceptions For the teacher

MisconceptionBecause of the Coriolis effect, toilets and sinks drain one way in the Northern Hemisphere and the other way in the Southern.

What the evidence showsThe Coriolis effect matters only for motions that are large and last a long time, such as winds that travel hundreds of kilometers over many hours. In a sink or toilet it is thousands of times too weak to compete with the shape of the bowl and the way the water was poured or flushed. Only in carefully controlled experiments, with the water left to settle for many hours, has the Earth's rotation been shown to set the direction of a draining vortex.

MisconceptionThe eye is the most violent part of a hurricane, or, when the wind suddenly drops, the storm is over.

What the evidence showsInside the eye the air is sinking and the wind is light; the strongest winds are in the eyewall that surrounds it. When the eye passes over a town, the calm is temporary: the far side of the eyewall arrives and the wind returns just as hard from the opposite direction. People who go outside during the calm can be caught in the open.

MisconceptionA storm's category tells you how dangerous it is.

What the evidence showsThe Saffir-Simpson category is based only on the strongest sustained wind. It says nothing about storm surge, which is usually the deadliest hazard, or about rainfall flooding. Katrina was a Category 3 when it came ashore, weaker than its Category 5 peak, yet its surge broke through the defenses of New Orleans and flooded 80 percent of the city.

MisconceptionThe forecast cone shows how big the storm is, and places outside the cone are safe.

What the evidence showsThe cone shows only the likely path of the storm's center, and the center leaves the cone about one time in three. Strong winds, surge and heavy rain often reach far beyond the center, and well outside the cone.

MisconceptionSince forecasters can predict a storm's path three days ahead to within about 100 miles, they can predict its strength just as well.

What the evidence showsTrack forecasts have improved more than threefold since 1990, but intensity forecasts have improved much more slowly. Rapid intensification is the hardest case: Milton went from Category 1 to Category 5 in about a day in 2024, and Patricia's winds rose by 105 knots (about 120 mph) in 24 hours in 2015, far faster than its forecasts.

Discussion questions

  1. The episode says a hurricane 'runs on' warm water. What happens to a hurricane when it moves over land or over cooler water, and why?
  2. Looking at a satellite image, you can tell which hemisphere a hurricane is in. Explain how. Why is it so rare for a hurricane to cross the equator?
  3. In 1900, nobody in Galveston could see how strong the storm had become out in the Gulf. List the technologies that would warn Galveston today. Which do you think matters most, and why?
  4. Katrina was weaker at landfall than at its peak, yet it was far deadlier and costlier than many stronger storms. What does this tell you about the ways we communicate hurricane danger? How would you design a better warning message?
  5. Galveston answered 1900 with a seawall and by raising the city; New Orleans answered 2005 with a $14 billion system of levees, gates and pumps. What are the strengths and limits of protecting a city with engineering? What else could a coastal community do?
  6. Forecasts of where a storm will go have improved far more than forecasts of how strong it will be. If you were an emergency manager and a storm could jump from Category 1 to Category 5 in a day, how would that change your decisions about evacuation?

Quiz Choose an answer; it checks itself

1.According to the episode, what does a hurricane need from the ocean?

2.In the hurricane's engine, what releases the heat that makes the air rise even faster?

3.Air flows in toward a hurricane's low-pressure center. In the Northern Hemisphere, what does the Coriolis effect do to it?

4.Why do hurricanes almost never form within about 5° (some 550 km) of the equator?

5.Where are a hurricane's strongest winds found?

6.Why does the World Meteorological Organization retire a storm's name?

7.Most of the water that flooded New Orleans after Hurricane Katrina came from where?

8.What does the cone in a hurricane forecast show?

9.Forecasters call it rapid intensification when a storm's maximum winds rise by at least how much in 24 hours?

10.Cyclone Winston (2016) in the South Pacific turned clockwise. Why?

Written response

1. Draw a labeled diagram of the hurricane heat engine. Show the warm sea surface, evaporation, rising moist air, condensation into cloud, the release of heat, and the inflow of new air at the surface. Explain in two or three sentences why the cycle feeds itself, and what would stop it.

What a strong answer includes

A strong answer shows warm water (at least 26.5 °C) evaporating; moist air rising; the vapor condensing into towering cloud and releasing heat; the warmed air rising faster, lowering the pressure at the surface; and more moist air flowing in over the sea to replace it, closing the loop. The cycle stops when the supply of warm, moist air is cut off: over land, over cooler water, or when the storm stirs up cold water from below a shallow warm layer.

2. Explain why hurricanes turn counter-clockwise in the Northern Hemisphere and clockwise in the Southern, and why they almost never form at the equator.

What a strong answer includes

Air flows in toward the low pressure at the center from every side. Because the Earth is turning, air that travels a long way across its surface is deflected, to the right in the Northern Hemisphere and to the left in the Southern (the Coriolis effect). The inflowing air therefore curves around the center instead of reaching it, winding the storm into a counter-clockwise spiral in the north and a clockwise one in the south. The deflection is zero at the equator and too weak within about 5° of it to start a storm turning, so hurricanes almost never form there or cross from one hemisphere into the other.

3. Using Galveston (1900) and Katrina (2005) as evidence, explain why a hurricane's category alone does not tell you how dangerous it will be, and describe how each city responded afterward.

What a strong answer includes

The category measures only the strongest sustained wind. In both disasters most deaths came from water: in Galveston, a surge of more than 15 feet swept over a low sand island and killed about 8,000 people; in New Orleans, Katrina came ashore as a Category 3, weaker than its Category 5 peak, but its surge broke through levees and floodwalls and flooded 80 percent of a city that lies largely below sea level, and nearly 1,400 people died. Surge depends on the storm's size, its track and the shape of the coast and seafloor, not only on wind speed. Galveston built a 17-foot seawall and raised much of the city on jacks; New Orleans built a $14 billion system of levees, gates and pumps.

Going deeper University and advanced high school

Why storms do not form at the equator

The strength of the Coriolis effect is measured by the Coriolis parameter, f = 2Ω sin φ, where Ω = 7.29 × 10-5 rad/s is Earth's rotation rate and φ is the latitude. Whether rotation matters for a flow of speed U and size L is judged by the Rossby number, Ro = U / (f L): rotation dominates when Ro is about 1 or less.

ProblemCalculate f at the equator, at 5° and at 20° latitude. For a developing storm with U = 10 m/s and L = 500 km, find Ro at 5° and at 20°. Then find Ro for water draining from a sink (U = 0.1 m/s, L = 0.3 m) at 45° latitude, and explain what your answers say about the episode's claims and about the toilet myth.

Worked answer

f = 0 at the equator; f = 2 × 7.29 × 10-5 × sin 5° ≈ 1.27 × 10-5 s⁻¹ at 5°; and f ≈ 4.99 × 10-5 s⁻¹ at 20°, almost four times larger. For the storm, Ro ≈ 10 ÷ (1.27 × 10-5 × 5 × 105) ≈ 1.6 at 5°, but Ro ≈ 0.4 at 20°, where rotation controls the flow. At the equator Ro is infinite: there is no deflection at all. For the sink, f ≈ 1.03 × 10-4 s⁻¹ and Ro ≈ 0.1 ÷ (1.03 × 10-4 × 0.3) ≈ 3,000: the Earth's rotation is irrelevant compared with the shape of the basin and the way it was filled. (Near the top of a hurricane, the air flowing out of the storm turns the opposite way, clockwise in the Northern Hemisphere, for the same reason.)

The energy budget of a day of rain

Every kilogram of water vapor that condenses releases its latent heat, about L = 2.5 × 106 J/kg. A standard estimate assumes that an average hurricane rains 1.5 cm a day over a circle of radius 665 km. World electricity demand passed 30,000 TWh in 2024 (Ember, 2025).

ProblemCalculate the mass of rain that falls in one day, the heat released by its condensation in joules per day and in watts, and the world's average electric power in watts. Check the episode's claim that an average hurricane releases more than a hundred times as much heat in a day as all the electricity the world generates.

Worked answer

Area = π × (6.65 × 105 m)² ≈ 1.39 × 1012 m²; volume of rain = 0.015 m × 1.39 × 1012 m² ≈ 2.1 × 1010 m³, a mass of about 2.1 × 1013 kg. Heat released ≈ 2.1 × 1013 kg × 2.5 × 106 J/kg ≈ 5.2 × 1019 J per day, or 5.2 × 1019 ÷ 86,400 s ≈ 6.0 × 1014 W. World electricity: 30,000 TWh = 1.08 × 1020 J a year, or about 3.4 × 1012 W on average. The ratio is about 6.0 × 1014 ÷ 3.4 × 1012 ≈ 175, consistent with 'more than a hundred times'. Only a small part of this heat ends up as wind; the next problem estimates how much.

Why each step in wind speed matters so much

The force of the wind on a wall grows with the square of the wind speed, V², and the rate at which the wind carries and dissipates energy grows with its cube, V³. The power a hurricane's winds dissipate by friction at the sea surface can be estimated as P ≈ ρ CD V³ A, with air density ρ ≈ 1.2 kg/m³, a drag coefficient CD ≈ 2 × 10-3 and A the area of strong wind.

ProblemCompare the force and the energy flux of the wind at the bottom of Category 5 (157 mph) with those at the bottom of Category 1 (74 mph). Do the same for Katrina at its peak (175 mph) and at its Louisiana landfall (125 mph). Then estimate P for a storm core of radius 50 km in which the wind averages 40 m/s, and compare it with the heat released by rain in the previous problem.

Worked answer

157 ÷ 74 ≈ 2.1, so the force is about 2.1² ≈ 4.5 times larger and the energy flux about 2.1³ ≈ 9.5 times larger. For Katrina, 175 ÷ 125 = 1.4: about 2.0 times the force and 2.7 times the energy flux at its peak, which is why the weakening before landfall mattered for wind damage, even though the surge was still catastrophic. P ≈ 1.2 × 2 × 10-3 × (40)³ × π × (5 × 104)² ≈ 154 W/m² × 7.9 × 109 m² ≈ 1.2 × 1012 W, comparable to a third of the world's average electric power, but only about 0.2 percent of the 6.0 × 1014 W of heat released by condensation. Most of that heat is carried up and out of the storm and eventually radiated to space; a hurricane is a powerful engine, but not an efficient one.

How much better are the forecasts?

The National Hurricane Center publishes the average error of its official forecasts every year, in nautical miles (1 n mi = 1.151 statute miles = 1.852 km). For all Atlantic tropical cyclones, the average 72-hour track error was 312.3 n mi in 1990 and 78.1 n mi in 2022; the average for 2020 to 2025 was 89.4 n mi.

ProblemConvert the 1990 error and the 2020–2025 average to statute miles and kilometers. By what percentage did the error fall, and by what factor? What average yearly rate of improvement does that imply? If the area of uncertainty around a forecast position scales with the square of the error, how much smaller is that area now?

Worked answer

1990: 312.3 × 1.151 ≈ 359 mi (578 km); 2020–2025: 89.4 × 1.151 ≈ 103 mi (166 km), matching the episode's 'more than 350' and 'about a hundred'. The error fell by (312.3 − 89.4) ÷ 312.3 ≈ 71 percent, a factor of 3.5: 'more than threefold'. A factor of 3.5 over about 32 years is (1/3.5)^(1/32) ≈ 0.962, close to 4 percent improvement a year. The area scales as the square: 3.5² ≈ 12 times smaller. The best single year, 2022, reached 78.1 n mi (about 90 mi), a factor of 4.0. Year-to-year values vary with the storms of each season: 2023 averaged 111 n mi.

How much of a storm surge is caused by low pressure?

Lower air pressure lets the sea surface rise beneath it, by Δh = Δp / (ρ g), with sea-water density ρ = 1,025 kg/m³ and g = 9.81 m/s². This is the 'inverse barometer' effect. The rest of a surge is water piled up by the wind, which is greatest over a wide, shallow continental shelf.

ProblemShow that the inverse barometer raises the sea by about 1 cm for every hectopascal (millibar) of pressure drop. Katrina's central pressure at its Louisiana landfall was 920 mb; take the surrounding pressure as 1,010 mb. Estimate the pressure part of the surge, and compare it with the highest surge measured, 27.8 ft (8.5 m) at Pass Christian, Mississippi. What does Typhoon Tip's 870 mb give?

Worked answer

1 hPa = 100 Pa, so Δh = 100 ÷ (1,025 × 9.81) ≈ 0.0099 m ≈ 1 cm per hPa. For Katrina, Δp ≈ 90 hPa gives about 0.9 m (3 ft), roughly a tenth of the 8.5 m surge; the rest was pushed ashore by the wind over the shallow, gently sloping Gulf shelf. Tip's 140 hPa drop gives only about 1.4 m. Wind, storm size and the shape of the coast, not the central pressure, make the great surges.

Standards alignment

Next Generation Science Standards

MS-ESS2-4

Develop a model to describe the cycling of water through Earth's systems driven by energy from the sun and the force of gravity.

In this episode: The hurricane engine: evaporation from the warm sea, condensation in the eyewall, and rain.

MS-ESS2-5

Collect data to provide evidence for how the motions and complex interactions of air masses results in changes in weather conditions.

In this episode: Air flowing from high to low pressure into the storm; the calm and the wind reversal as the eye passes; forecasts within probabilistic ranges (the cone).

MS-ESS2-6

Develop and use a model to describe how unequal heating and rotation of the Earth cause patterns of atmospheric and oceanic circulation that determine regional climates.

In this episode: The Coriolis effect, opposite spins in the two hemispheres, and why hurricanes need the warm tropical sea.

MS-ESS3-2

Analyze and interpret data on natural hazards to forecast future catastrophic events and inform the development of technologies to mitigate their effects.

In this episode: Satellites, hurricane hunters and models; track-error data since 1990; seawalls, levees and pumps.

HS-ESS3-1

Construct an explanation based on evidence for how the availability of natural resources, occurrence of natural hazards, and changes in climate have influenced human activity.

In this episode: Galveston's seawall and grade raising, New Orleans after Katrina, and the retirement of storm names.

Advanced Placement

University courses

Introductory meteorology

Pressure gradient force and the Coriolis effect; the Coriolis parameter and Rossby number; tropical cyclone structure (eye, eyewall, spiral bands); latent heat and moist convection

Tropical meteorology and climate

Conditions for tropical cyclone genesis; the hurricane as a heat engine; rapid intensification; forecast verification and track versus intensity skill

Coastal hazards and oceanography

Storm surge, wind setup and the inverse barometer effect; the limits of the Saffir-Simpson scale; coastal defenses and risk communication

Transcript The narration, word for word

0:00The Engine

This is Hurricane Isabel, in the Atlantic, in September 2003: a Category 5 storm, an engine the size of a country, turning. If you follow its spiral bands, you'll see that the winds near the surface all turn the same way, counter-clockwise. Every hurricane north of the equator turns like this, and every one south of it turns the other way. That pattern isn't chance. The planet itself creates it.

0:27In this episode, we'll find out what a hurricane runs on, why it spins the way it does, and what happens inside the eye. We'll go back to two storms that changed America, and see how forecasts that once missed by more than 350 miles now miss by about 100.

0:47We'll start with the fuel. A hurricane is a heat engine, and it runs on warm water. The sea surface has to be at least 26.5 °C, about 80 °F, and the water has to stay that warm to a depth of some 50 meters. This map shows the sea in late August 2005, with the warmest water in red. It also explains why the season peaks at the end of summer, when the ocean has had months to absorb the Sun's heat.

1:14The engine works like this. Warm water evaporates, and the moist air above it rises. As the air climbs, its water vapor condenses into cloud, and condensation releases heat. That heat makes the air rise even faster, which draws in more moist air from the sea, so the cycle keeps feeding itself. In a single day, an average hurricane releases more than 100 times as much heat as all the electricity the world generates.

1:45Why It Spins

Next comes the spin. Air rushes in toward the low pressure at the center of the storm from every side, and on a planet that stood still, it would flow straight in. But the Earth is turning, and anything that travels a long way across its surface is deflected, to the right in the Northern Hemisphere and to the left in the Southern. That deflection is called the Coriolis effect.

2:10As a result, the air never reaches the center directly. It curves around it, and the whole storm winds itself into a spiral, counter-clockwise in the north and clockwise in the south. Once you know that, any satellite picture of a hurricane tells you which hemisphere it is in.

2:28Right at the equator, however, there is no sideways deflection at all. Within about 5 degrees of it, some 550 kilometers on either side, the Coriolis effect is too weak to start a storm turning. That is why hurricanes almost never form there, and almost never cross from one hemisphere into the other.

2:49The Eye

Now let's look into the center of a storm. This is Hurricane Patricia, off the coast of Mexico, in October 2015. Its winds reached 345 kilometers an hour, or 215 miles an hour, the strongest ever measured in a hurricane. At its center, there is a hole in the clouds: the eye.

3:11Here is the eye of Isabel, up close. Inside it the air is sinking, so the wind is light and the sky can even clear. The swirls you can see are mesovortices, smaller whirlpools of air turning within the eye itself. An eye like this is usually 30 to 60 kilometers across, and around it stands the eyewall, a ring of towering cloud where the winds blow hardest. When the eye passes over a town, the wind suddenly drops, and then it returns just as hard from the opposite direction.

3:43The lowest air pressure ever measured at sea level was recorded inside an eye. Typhoon Tip, in the western Pacific in 1979, bottomed out at 870 millibars. Tip was also the largest tropical cyclone on record, about 2,200 kilometers across. Laid over North America, it would cover half the width of the United States.

4:10The Names

Why do storms have names at all? Forecasters were often tracking several storms at once, and long descriptions were easily confused over the radio. Atlantic storms were first named in 1950, using the radio alphabet of the time: Able, Baker, Charlie. Women's names were introduced in 1953, and men's names joined the lists in 1979.

4:33Names make a real difference when several storms are active at once. On September 14, 2020, five tropical cyclones were spinning in the Atlantic at the same time, something seen only once before, in 1971. The World Meteorological Organization keeps six lists of names for the Atlantic, used in rotation, so each name comes back every six years. The exception is a storm so deadly or so costly that its name is retired for good, as happened with Katrina, Maria, Ian and Helene.

5:061900 and 2005

The first of those two storms struck on September 8, 1900. Galveston, Texas, was then one of the richest cities in the state, built on a sand island whose highest point stood less than 9 feet above the sea. There were no satellites and no radar, and ships at sea had no radio, so nobody could see how strong the storm had grown out in the Gulf.

5:28The sea rose more than 15 feet and swept across the whole island. By morning, about 8,000 people were dead, and it remains the deadliest natural disaster in American history. Galveston rebuilt behind a seawall 17 feet high, and then raised much of the city, house by house, on jacks.

5:49A hundred and five years later came Katrina. On August 28, 2005, it was a Category 5 storm in the middle of the Gulf, with winds of 175 miles an hour, and the whole coast from Louisiana to Florida lay in its path.

6:06Katrina came ashore in Louisiana the next morning, weaker by then, as a Category 3. Much of New Orleans, however, sits below sea level behind levees, and the storm surge broke through them in about 50 places. Eighty percent of the city flooded. Nearly 1,400 people died, and the damage came to $125 billion.

6:30Most of that water did not fall from the sky. It poured in from the lake and the canals when the flood walls gave way. Since then, the city has built a $14 billion ring of levees, gates and pumps, one of the largest civil works projects the Army Corps of Engineers has ever built.

6:52The Forecast

Modern forecasters can see these storms coming far better than anyone could in Galveston. Every forecast now comes with a cone, like this one. The cone does not show the size of the storm. It shows where the center will probably go, and two times out of three, the center stays inside it.

7:09In 1990, the National Hurricane Center's three day forecasts missed the storm's position by more than 350 miles, on average. By the mid 2020s, the average miss was about 100 miles. That improvement came from satellites, from hurricane hunter aircraft that fly straight through the eyewall, and from computer models running on some of the fastest machines on Earth.

7:33What remains hard to predict is strength. Over very warm water, some storms strengthen astonishingly fast, a process forecasters call rapid intensification, defined as winds rising by at least 35 miles an hour within a single day. In October 2024, Hurricane Milton went from Category 1 to Category 5 in about a day, on its way to Florida.

8:00Still Spinning

Now look at the other side of the world. This is Cyclone Winston in the South Pacific, in February 2016, two days before it struck Fiji as one of the strongest storms ever recorded in the Southern Hemisphere. It runs on the same warm water and the same engine, but look at its spiral. This one turns clockwise.

8:22So, three things to remember. First, a hurricane is a heat engine that runs on warm sea water, at least 26.5 °C. Second, the Earth's rotation gives it its spin, counter-clockwise north of the equator and clockwise south of it, which is why hurricanes almost never form at the equator itself. And third, forecasts of where a storm will go have improved more than threefold since 1990, but how strong it will become is still the hard part.

8:38The next time you see a hurricane from space, look at the way it turns. If it turns counter-clockwise, it is north of the equator, and if it turns clockwise, it is south of it. And remember what it runs on: the warm sea beneath it, turned into wind by a planet that never stops turning.

Sources

  1. Gray, W. M. (1968). Global view of the origin of tropical disturbances and storms. Monthly Weather Review, 96(10), 669–700. doi.org/10.1175/1520-0493(1968)096<0669:GVOTOO>2.0.CO;2Used for: Conditions for tropical cyclone formation: warm water, and distance from the equator
  2. Ember (2025). Global Electricity Review 2025: 2024 in review. ember-energy.org/latest-insights/global-electricity-review-2025/2024-in-reviewUsed for: World electricity demand, above 30,000 TWh in 2024
  3. Shapiro, A. H. (1962). Bath-tub vortex. Nature, 196, 1080–1081. doi.org/10.1038/1961080b0Used for: The Coriolis effect and draining water (the toilet myth)
  4. National Hurricane Center. Saffir-Simpson Hurricane Wind Scale. NOAA. www.nhc.noaa.gov/aboutsshws.phpUsed for: Category wind ranges, and the hazards the scale does not include
  5. Kimberlain, T. B., Blake, E. S., & Cangialosi, J. P. (2016). Tropical Cyclone Report: Hurricane Patricia (EP202015), 20–24 October 2015. National Hurricane Center. www.nhc.noaa.gov/data/tcr/EP202015_Patricia.pdfUsed for: Patricia's peak winds and its record rapid intensification
  6. Dunnavan, G. M., & Diercks, J. W. (1980). An analysis of Super Typhoon Tip (October 1979). Monthly Weather Review, 108(11), 1915–1923. doi.org/10.1175/1520-0493(1980)108<1915:AAOSTT>2.0.CO;2Used for: Tip's 870 mb pressure and its record size
  7. National Hurricane Center. Tropical Cyclone Naming History and Retired Names. NOAA. www.nhc.noaa.gov/aboutnames_history.shtmlUsed for: Naming since 1950, women's names from 1953, men's from 1979; six rotating lists; retired names
  8. Cline, I. M. (1900). Special report on the Galveston hurricane of September 8, 1900. Reproduced by the NOAA National Weather Service Heritage project: Galveston Storm of 1900. vlab.noaa.gov/web/nws-heritage/-/galveston-storm-of-1900Used for: The 1900 storm tide at Galveston, from the local forecaster's own observations
  9. American Society of Civil Engineers. Galveston Seawall and Grade Raising. Historic Civil Engineering Landmark. www.asce.org/about-civil-engineering/history-and-heritage/historic-landmarks/galveston-seawall-and-grade-raisingUsed for: The 17-foot seawall and the raising of the city on jackscrews
  10. Knabb, R. D., Rhome, J. R., & Brown, D. P. (2005; updated 2023). Tropical Cyclone Report: Hurricane Katrina, 23–30 August 2005. National Hurricane Center. www.nhc.noaa.gov/data/tcr/AL122005_Katrina.pdfUsed for: Katrina's peak and landfall intensity, storm surge, levee breaches, flooding, deaths (1,392) and damage ($125 billion)
  11. National Hurricane Center. Storm Surge Overview. NOAA. www.nhc.noaa.gov/surgeUsed for: What storm surge is, and why it is the leading cause of hurricane deaths
  12. National Hurricane Center. Definition of the NHC Track Forecast Cone. NOAA. www.nhc.noaa.gov/aboutcone.shtmlUsed for: What the cone shows; the two-thirds rule
  13. National Hurricane Center. National Hurricane Center Forecast Verification: Official Error Trends. NOAA. www.nhc.noaa.gov/verification/verify5.shtmlUsed for: Average Atlantic track errors, 1990 to the mid-2020s
  14. Beven, J. L., II, Alaka, L., & Fritz, C. (2025). Tropical Cyclone Report: Hurricane Milton (AL142024), 5–10 October 2024. National Hurricane Center. www.nhc.noaa.gov/data/tcr/AL142024_Milton.pdfUsed for: Milton's rapid intensification from Category 1 to Category 5

Images in the episode: USGS, NOAA and NASA (public domain), with maps from NASA/USGS Landsat via NASA GIBS; animations by EarthWatch 24-7. Full credits: earthwatch247.com/credits.html.

Cite this lesson

EarthWatch 24-7. (2026). Why Hurricanes Spin: The engine, the eye and the Coriolis effect [Video lesson]. Earth Explained, episode 4. https://earthwatch247.com/learn/hurricanes/

Answer key

  1. C. A hurricane is a heat engine fueled by warm water; the sea surface must be at least 26.5 °C, and the warmth must extend to about 50 m so the storm's own mixing does not bring up cold water.
  2. A. Heat absorbed when sea water evaporates is released when the vapor condenses into cloud. That heat warms the rising air, which rises faster and draws in more moist air from the sea.
  3. D. Moving air is deflected to the right north of the equator, so it curves around the center instead of reaching it, and the storm winds up counter-clockwise.
  4. B. The Coriolis effect is zero at the equator and grows with latitude. Near the equator it is too weak to turn the inflowing air into a spinning storm, even though the water is warm.
  5. A. In the eye the air is sinking and the wind is light. The strongest winds blow in the eyewall that surrounds it.
  6. C. Six lists rotate, so each name normally returns every six years. Names such as Katrina, Maria, Ian and Helene were retired after storms that were exceptionally deadly or costly.
  7. B. Much of New Orleans lies below sea level behind levees. Katrina's storm surge broke through them, and lake and canal water flooded about 80 percent of the city.
  8. D. The cone is drawn from past forecast errors. It shows where the center will probably go, not the size of the storm or where its impacts will reach.
  9. C. The definition is an increase of at least 30 knots (35 mph) in a day. Milton in 2024 far exceeded it: its winds rose from 70 knots to 150 knots in 24 hours, from Category 1 to Category 5.
  10. A. Winston ran on the same warm-water engine; only the direction of the Coriolis deflection differs, so southern storms spin the opposite way.

Written response

  1. A strong answer shows warm water (at least 26.5 °C) evaporating; moist air rising; the vapor condensing into towering cloud and releasing heat; the warmed air rising faster, lowering the pressure at the surface; and more moist air flowing in over the sea to replace it, closing the loop. The cycle stops when the supply of warm, moist air is cut off: over land, over cooler water, or when the storm stirs up cold water from below a shallow warm layer.
  2. Air flows in toward the low pressure at the center from every side. Because the Earth is turning, air that travels a long way across its surface is deflected, to the right in the Northern Hemisphere and to the left in the Southern (the Coriolis effect). The inflowing air therefore curves around the center instead of reaching it, winding the storm into a counter-clockwise spiral in the north and a clockwise one in the south. The deflection is zero at the equator and too weak within about 5° of it to start a storm turning, so hurricanes almost never form there or cross from one hemisphere into the other.
  3. The category measures only the strongest sustained wind. In both disasters most deaths came from water: in Galveston, a surge of more than 15 feet swept over a low sand island and killed about 8,000 people; in New Orleans, Katrina came ashore as a Category 3, weaker than its Category 5 peak, but its surge broke through levees and floodwalls and flooded 80 percent of a city that lies largely below sea level, and nearly 1,400 people died. Surge depends on the storm's size, its track and the shape of the coast and seafloor, not only on wind speed. Galveston built a 17-foot seawall and raised much of the city on jacks; New Orleans built a $14 billion system of levees, gates and pumps.

Going deeper

  1. Why storms do not form at the equator: f = 0 at the equator; f = 2 × 7.29 × 10-5 × sin 5° ≈ 1.27 × 10-5 s⁻¹ at 5°; and f ≈ 4.99 × 10-5 s⁻¹ at 20°, almost four times larger. For the storm, Ro ≈ 10 ÷ (1.27 × 10-5 × 5 × 105) ≈ 1.6 at 5°, but Ro ≈ 0.4 at 20°, where rotation controls the flow. At the equator Ro is infinite: there is no deflection at all. For the sink, f ≈ 1.03 × 10-4 s⁻¹ and Ro ≈ 0.1 ÷ (1.03 × 10-4 × 0.3) ≈ 3,000: the Earth's rotation is irrelevant compared with the shape of the basin and the way it was filled. (Near the top of a hurricane, the air flowing out of the storm turns the opposite way, clockwise in the Northern Hemisphere, for the same reason.)
  2. The energy budget of a day of rain: Area = π × (6.65 × 105 m)² ≈ 1.39 × 1012 m²; volume of rain = 0.015 m × 1.39 × 1012 m² ≈ 2.1 × 1010 m³, a mass of about 2.1 × 1013 kg. Heat released ≈ 2.1 × 1013 kg × 2.5 × 106 J/kg ≈ 5.2 × 1019 J per day, or 5.2 × 1019 ÷ 86,400 s ≈ 6.0 × 1014 W. World electricity: 30,000 TWh = 1.08 × 1020 J a year, or about 3.4 × 1012 W on average. The ratio is about 6.0 × 1014 ÷ 3.4 × 1012 ≈ 175, consistent with 'more than a hundred times'. Only a small part of this heat ends up as wind; the next problem estimates how much.
  3. Why each step in wind speed matters so much: 157 ÷ 74 ≈ 2.1, so the force is about 2.1² ≈ 4.5 times larger and the energy flux about 2.1³ ≈ 9.5 times larger. For Katrina, 175 ÷ 125 = 1.4: about 2.0 times the force and 2.7 times the energy flux at its peak, which is why the weakening before landfall mattered for wind damage, even though the surge was still catastrophic. P ≈ 1.2 × 2 × 10-3 × (40)³ × π × (5 × 104)² ≈ 154 W/m² × 7.9 × 109 m² ≈ 1.2 × 1012 W, comparable to a third of the world's average electric power, but only about 0.2 percent of the 6.0 × 1014 W of heat released by condensation. Most of that heat is carried up and out of the storm and eventually radiated to space; a hurricane is a powerful engine, but not an efficient one.
  4. How much better are the forecasts?: 1990: 312.3 × 1.151 ≈ 359 mi (578 km); 2020–2025: 89.4 × 1.151 ≈ 103 mi (166 km), matching the episode's 'more than 350' and 'about a hundred'. The error fell by (312.3 − 89.4) ÷ 312.3 ≈ 71 percent, a factor of 3.5: 'more than threefold'. A factor of 3.5 over about 32 years is (1/3.5)^(1/32) ≈ 0.962, close to 4 percent improvement a year. The area scales as the square: 3.5² ≈ 12 times smaller. The best single year, 2022, reached 78.1 n mi (about 90 mi), a factor of 4.0. Year-to-year values vary with the storms of each season: 2023 averaged 111 n mi.
  5. How much of a storm surge is caused by low pressure?: 1 hPa = 100 Pa, so Δh = 100 ÷ (1,025 × 9.81) ≈ 0.0099 m ≈ 1 cm per hPa. For Katrina, Δp ≈ 90 hPa gives about 0.9 m (3 ft), roughly a tenth of the 8.5 m surge; the rest was pushed ashore by the wind over the shallow, gently sloping Gulf shelf. Tip's 140 hPa drop gives only about 1.4 m. Wind, storm size and the shape of the coast, not the central pressure, make the great surges.