Ages 11–14 · Years 6–9 · Science · 6 minutes

The Greenhouse Effect Explained

Why can a little invisible gas warm a whole planet? Follow Eunice Foote’s 1856 experiments, John Tyndall’s infrared tests, and the Keeling Curve to see how the greenhouse effect works. Includes a step-by-step energy-budget example and a four-point recap.

Key terms

Infrared radiation
Invisible radiation emitted by warm surfaces, including Earth.
Greenhouse gas
A gas that absorbs and emits infrared radiation.
Energy balance
A balance between the energy a planet absorbs and the energy it sends back to space.
Keeling Curve
The long-running record of atmospheric carbon dioxide measurements begun at Mauna Loa in 1958.
Parts per million
The number of carbon dioxide molecules per million molecules of dry air.
Enhanced greenhouse effect
The strengthening of the greenhouse effect as additional greenhouse gases accumulate.

Transcript

0:00

Can a jar of invisible gas give us a clue about why a whole planet can warm? In eighteen fifty six, American scientist Eunice Foote put thermometers inside glass cylinders, filled them with different gases, and placed them in sunlight. The cylinder with carbon dioxide became the hottest. It also took longer to cool. Foote wondered what would happen if the atmosphere contained more of that gas. Keep that question in mind. We are going from her tabletop to a volcano, where the air itself keeps a record.

0:33

Foote had spotted a remarkable connection, but her jars were not a miniature Earth. Her setup combined glass, sunlight, and the gas inside. Her experiment did not isolate the mechanism we now call the greenhouse effect. Three years later, John Tyndall began separate experiments at the Royal Institution in London. He sent radiant heat through a tube of gas and measured how much got through. Some gases absorbed it strongly. Now scientists could measure how gases absorb radiant heat.

1:05

First, follow the energy. Sunlight arrives at Earth. Some is reflected back to space by clouds, the atmosphere, and bright surfaces. Some is absorbed by land and oceans, warming them. Imagine standing on a sunlit path. You can feel the warmed ground, even after a cloud passes. Warm surfaces give off energy as infrared radiation. Your eyes cannot see it, but it is part of the same family as visible light. Earth is constantly sending this invisible radiation outward. That is how our planet cools.

1:37

Here is the crucial difference: much incoming sunlight passes through the atmosphere, but some outgoing infrared is absorbed by greenhouse gases. Carbon dioxide, water vapor, and methane are examples. After energy is absorbed and shared among molecules, the atmosphere emits infrared in all directions, including back toward the surface. That slows the surface losing energy. It does not lock heat away forever: radiation still escapes to space. The natural greenhouse effect keeps Earth warmer than it would be without these gases. Invisible air is doing a very visible job.

2:14

Now for the trap in the name. Earth has no glass roof. An actual garden greenhouse mainly slows the movement of warm air out. The atmosphere works differently: greenhouse gases absorb and emit infrared radiation. And carbon dioxide does not have to make up most of the air to matter. Nitrogen and oxygen are far more abundant, but they do not absorb infrared strongly in the same way. What matters is how a gas interacts with radiation, not simply how much room it takes up.

2:45

Try a simple energy budget. These are imaginary units, not measurements of Earth. Suppose the planet absorbs one hundred units of energy and sends one hundred back to space. Balanced. Now add greenhouse gases. At the same temperature, imagine only ninety eight units leave. Pause and work it out: how much energy stays? Two units. Keep that imbalance going, and the planet warms. A warmer planet emits more infrared. If gas levels stop rising, energy leaving can eventually match energy arriving, at a higher temperature. Greenhouse gases change the temperature needed for balance.

3:23

So was Foote asking about a real change in the atmosphere? To find out, we need measurements. In nineteen fifty eight, Charles David Keeling began measuring carbon dioxide at Mauna Loa in Hawaii. The record is known as the Keeling Curve. Look at its two patterns. The little zigzags mostly track the seasonal activity of plants, especially across the Northern Hemisphere. Plants take in carbon dioxide as they grow; decay and respiration return it. But underneath those seasonal changes is something much bigger: the whole line climbs.

3:57

Near the start, the monthly average was about three hundred fifteen parts per million. By twenty twenty four, it was above four hundred twenty. Parts per million counts carbon dioxide molecules in a million molecules of dry air. The graph measures a gas, not temperature. Its upward trend shows carbon dioxide accumulating. Burning coal, oil, and gas releases carbon that had been stored underground. This human addition strengthens the greenhouse effect. Natural seasonal cycling makes the line wiggle; it does not explain the persistent climb.

4:31

Return to Foote and her glass cylinders. Her big question was whether more carbon dioxide could mean a warmer atmosphere. Today, experiments explain the infrared mechanism, and atmospheric measurements show that we are adding more of the gas. Together they tell a powerful story. Global warming means a long term increase in the planet’s average surface temperature. It does not mean every place gets warmer every single day. A cold afternoon cannot cancel a changing global energy budget. Weather is the daily detail; climate is the longer pattern.

5:07

Here are four ideas to keep. Sunlight supplies energy. Warm Earth emits infrared. Greenhouse gases absorb and emit some of that infrared, slowing energy loss from the surface. Adding greenhouse gases changes the energy balance and raises the temperature needed to restore it. Useful science phrases: absorb and emit infrared radiation; incoming and outgoing energy; enhanced greenhouse effect. From Foote’s tabletop to the Keeling Curve, the question is the same: what can invisible air do? It can slow Earth’s energy loss. Add more greenhouse gases, and you can warm a planet.

Sources

Every fact in the video, and where it comes from.

  1. 1
    aps.org/apsnews/2023/07/carbon-dioxide-atmosphere-euni…
    • In 1856 Eunice Newton Foote compared gases in glass cylinders exposed to sunlight, with thermometers; carbon dioxide became hottest and cooled slowly. She inferred that a CO2-rich atmosphere would be warmer.
  2. 2
    rigb.org/explore-science/explore/blog/who-discovered-gr…
    • Foote studied solar heating in glass vessels; Tyndall separately measured absorption of infrared heat by gases, beginning in 1859. Her experiment did not isolate the atmospheric infrared mechanism.
  3. 3
    rigb.org/explore-science/explore/collection/john-tyndal…
    • John Tyndall at the Royal Institution used a tube and heat-detecting apparatus to investigate gases; water vapor and carbon dioxide absorb radiant heat.
  4. 4
    science.nasa.gov/ems/13_radiationbudget
    • Solar energy arrives as shortwave radiation including visible light. Some reflects; absorbed energy warms Earth. Earth emits thermal infrared radiation.
  5. 5
    noaa.gov/jetstream/atmosphere/energy
    • Greenhouse gases absorb and emit infrared radiation. Atmospheric radiation goes both upward and downward, reducing surface cooling; energy still escapes to space.
  6. 6
    science.nasa.gov/earth/earth-observatory/clouds-and-radiation
    • Natural greenhouse warming keeps the surface warmer; water vapor, carbon dioxide and methane are greenhouse gases.
  7. 7
    climate.mit.edu/sites/default/files/2023-10/TILclimate Greenho…
    • A physical greenhouse primarily limits convection; the atmospheric greenhouse effect works through absorption and emission of infrared radiation.
  8. 8
    science.nasa.gov/earth/earth-observatory/climate-and-earths-ene…
    • Increasing CO2 initially reduces energy leaving at a given temperature; an energy imbalance causes warming until outgoing and incoming energy again balance. The 100/98/2 example is invented accounting, not measured Earth data.
  9. 9
    weather.gov.hk/en/climate_change/faq/faq017.htm
    • Carbon dioxide concentration is a small fraction of air; nitrogen and oxygen do not absorb infrared strongly like greenhouse gases. Abundance alone does not determine effect.
  10. 10
    noaa.gov/heritage/stories/five-significant-moments-in-c…
    • Charles David Keeling began Mauna Loa CO2 measurements in 1958. The record shows seasonal oscillations and a long-term rise.
  11. 11
    gml.noaa.gov/ccgg/trends/data.html
    • Mauna Loa monthly mean CO2 was about 315 ppm in 1958 and above 420 ppm by 2024. ppm counts molecules per million molecules of dry air. The plotted monthly observations are from NOAA/Scripps.
  12. 12
    acs.org/education/whatischemistry/landmarks/keeling-cu…
    • Seasonal CO2 cycling is strongly affected by Northern Hemisphere land vegetation; human fossil-fuel burning drives the long-term increase.
  13. 13
    science.nasa.gov/climate-change/causes
    • Burning coal, oil and gas transfers carbon to the atmosphere as CO2. Human greenhouse-gas emissions strengthen the natural greenhouse effect.
  14. 14
    science.nasa.gov/climate-change/what-is-climate-change
    • Global warming is the long-term rise in global average surface temperature, distinct from day-to-day local weather.
  15. 15
    gml.noaa.gov/ccgg/about/co2_measurements_ndir.html
    • Parts per million is the CO2 mole fraction relative to dry air.

Image and sound credits

  • CO₂ data: NOAA Global Monitoring Laboratory and Scripps Institution of Oceanography (C. D. Keeling), Mauna Loa monthly means, March 1958 – December 2024 (gml.noaa.gov/ccgg/trends)
  • Charles David Keeling and John Chin at Mauna Loa Observatory, 1997: John Miller, NOAA, public domain, via Wikimedia Commons
  • Mauna Loa Observatory: NOAA Research, public domain, via Wikimedia Commons
  • Mauna Loa Observatory, north flank of Mauna Loa: Brian Vasel, NOAA, public domain, via Wikimedia Commons
  • CO₂ infrared analyser and air-sample flask at Mauna Loa Observatory, 1982: Cdr John Bortniak, NOAA Photo Library, public domain
  • “Forest, Siberian taiga, Krasnoyarsk Sea, Russia” by Vyacheslav Argenberg, CC BY 4.0 (https://creativecommons.org/licenses/by/4.0), via Wikimedia Commons Source: (https://commons.wikimedia.org/wiki/File:Forest,_Siberian_taiga,_Krasnoyarsk_Sea,_Russia.jpg). Cropped and animated.
  • “Yallourn brown coal fired power station” by Joel200716, CC BY 4.0 (https://creativecommons.org/licenses/by/4.0), via Wikimedia Commons Source: (https://commons.wikimedia.org/wiki/File:YALLOURN_BROWN_COAL_FIRED_POWER_STATION.jpg). Cropped and animated.
  • Charts and diagrams drawn in code; NOAA/Scripps monthly observations, example energy budget and schematic molecular models
  • Paper textures: ambientCG (CC0) · Torn paper edges generated with AI
  • Sound effects: Freesound contributors (CC0)
  • Music: generated with ACE-Step · Voice: Gemini TTS
  • Earth: NASA/Apollo 17 crew, public domain. Sun: NASA/SDO AIA, public domain. Both via Wikimedia Commons.
  • Eunice Foote, Circumstances Affecting the Heat of the Sun’s Rays (1856), original paper scan, public domain; via Wikimedia Commons.
  • John Tyndall by John McLure Hamilton, public domain; https://commons.wikimedia.org/wiki/File:John_Tyndall_by_John_McLure_Hamilton.jpg

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