49 free, high-quality past-paper-style questions on Greenhouse effect for IB Physics HL, each with a full mark scheme. Covers: Albedo and the solar constant; Resonance model of the greenhouse effect; Surface–atmosphere energy balance; and more. For when you have finished the past papers, or want to practise one topic at a time.B.2 at Standard Level →Read the B.2 notes →My revision plan →Not sure of your level? Diagnostic test →Multiple choice or structured questions, with the mark scheme as a separate PDF.221 marks · Updated 26 October 2026 · Created by Evan Kotronis with AI assistance · every answer re-solved before publishing · How questions are checked
1B-1A-15Albedo and the solar constantPaper 1AEasy1 mark
The solar constant at a planet with no atmosphere is S and the albedo of its surface is α.
What is the mean intensity of solar radiation absorbed by the planet, averaged over its whole surface?
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Step 1The planet intercepts radiation over its projected disc, area πr2, but its total surface area is 4πr2, so the mean incoming intensity is S/4.
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All 3 steps must be completed — there is no mark for a part-answer.
Step 2A fraction α is scattered, so a fraction (1 − α) is absorbed.
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Step 3Mean absorbed intensity = (1 − α)S/4.
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Answer D
Answer: D · 3 stages of work, one mark
Every option, and why
AThis uses the albedo as the fraction absorbed; albedo is the fraction scattered.
BThis divides by the area of a hemisphere (2πr2), as if only the day side counted in the average over the whole surface.
CThis is the intensity absorbed by a surface perpendicular to the rays; it ignores the projected-area (S/4) averaging.
DCorrect: projected area πr2 shared over 4πr2, with a fraction (1 − α) absorbed.
2IBP2H-012-01-01Resonance model of the greenhouse effectPaper 1AEasy1 mark
The resonance model is used to explain why carbon dioxide is a greenhouse gas. Which statement best describes the mechanism in this model?
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In the resonance model, the bonds in a CO2 molecule behave like springs with natural frequencies of vibration. These frequencies are in the infrared range. When the driving frequency of the radiation equals a natural frequency, the amplitude of oscillation grows and energy is absorbed. It is later re-emitted in random directions. Infrared photons are far too weak to ionise a molecule. A molecule is much smaller than an infrared wavelength. Electronic transitions correspond to visible and UV photons, not infrared.
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Answer B
Answer: B
Common error: Do not mix up electronic transitions (visible/UV) with molecular vibrations (infrared). The greenhouse effect involves vibrational resonance.
3IBP2H-012-01-08Surface–atmosphere energy balancePaper 1AEasy1 mark
In a simplified annual-mean model, each square metre of Earth's surface has the following energy flows: • it absorbs 160 W m−2 of solar radiation; • it absorbs 340 W m−2 of infrared radiation from the atmosphere; • it loses 100 W m−2 by convection and evaporation. The surface temperature is constant. What is the infrared intensity emitted by the surface?
Diagram not to scale
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At constant temperature, the total power in equals the total power out. The power in is 160 + 340 = 500 W m−2. The power out is 100 W m−2 by non-radiative losses plus the emitted infrared. The emitted infrared is therefore 500 − 100 = 400 W m−2. The value 500 W m−2 ignores convection and evaporation. The value 240 W m−2 omits the solar input. The value 60 W m−2 omits the back-radiation from the atmosphere.
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Answer C
Answer: C
Common error: Back-radiation from the atmosphere is an input to the surface. It often exceeds the direct solar input, so do not leave it out.
4IBP2H-012-00-01Equilibrium temperaturePaper 1AEasy1 mark
The solar constant at the Earth (1.0 AU from the Sun) is 1.36 kW m−2. An asteroid-mining probe is parked 2.0 AU from the Sun. What is the intensity of solar radiation at the probe?
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The Sun's power spreads over a sphere of area 4πd2, so intensity follows an inverse-square law. Doubling the distance divides the intensity by 22 = 4: 1.36/4 = 0.34 kW m−2. 0.68 assumes I ∝ 1/d, 0.96 assumes I ∝ 1/√d, and 5.4 multiplies by d2 instead of dividing.
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Answer B
Answer: B
Exam tip: Check direction first: moving away from the Sun must lower the intensity, which rules out any answer above 1.36 kW m⁻² straight away.
5IBP2H-012-00-02Albedo and melting sea icePaper 1AEasy1 mark
An area of Arctic sea ice melts and is replaced by open ocean water. The solar intensity reaching the area is unchanged. Which describes the change in the albedo of the area and the change in the solar power absorbed by it?
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Albedo is the ratio of reflected to incident power. Dark ocean water reflects far less sunlight than white ice, so the albedo decreases. Because the fraction absorbed is (1 − albedo), a smaller albedo means a larger absorbed power. Albedo is a surface property and does not depend on the incident intensity.
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Answer C
Answer: C
Common error: Albedo measures reflection, not absorption. A low albedo means strong absorption: absorbed fraction = 1 − α.
6B-1A-08Resonance model of the greenhouse effectPaper 1AMedium1 mark
In a resonance model of the greenhouse effect, the bonds in a molecule of carbon dioxide are treated as oscillators. One mode of vibration of the molecule has a natural angular frequency of 1.26 × 1014 rad s−1.
Which row gives the wavelength of the electromagnetic radiation that drives this vibration at resonance, and the direction in which the molecule re-emits the absorbed energy?
WavelengthDirection of re-emission
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Step 1Resonance occurs when the frequency of the radiation equals the natural frequency of the vibration: f = ω/2π = 1.26 × 1014/2π = 2.0 × 1013 Hz.
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All 3 steps must be completed — there is no mark for a part-answer.
Step 2λ = c/f = 3.00 × 108/2.0 × 1013 = 1.5 × 10−5 m = 15 μm, in the infrared, close to the peak of the radiation emitted by the Earth's surface.
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Step 3The excited molecule re-emits the energy in a random direction, so the radiation leaves the gas in all directions: part returns to the surface and warms it, part continues upwards.
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Answer A
Answer: A · 3 stages of work, one mark
Every option, and why
ACorrect: f = ω/2π gives 15 μm, and re-emission takes place in all directions.
BThe wavelength is right, but the molecules do not act as mirrors: the absorbed energy is re-emitted in all directions, and only part of it returns to the surface.
DThis combines both errors: the angular frequency is used as if it were the frequency, and the re-emission is taken to be directed back to the surface only.
7B-1A-37Equilibrium temperaturePaper 1AMedium1 mark
Two planets orbit the same star. Planet Y is at distance d from the star and has an equilibrium surface temperature T. Planet X is at distance 2d and has the same albedo and the same emissivity as Y. Neither planet has an atmosphere.
What is the equilibrium surface temperature of X?
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Step 1The intensity of the starlight follows an inverse-square law: at 2d it is ¼ of that at d.
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All 3 steps must be completed — there is no mark for a part-answer.
Step 2In equilibrium the power absorbed per unit area equals the power emitted per unit area: (1 − albedo)S/4 = eσT4, so T4 ∝ S.
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Step 3T ∝ S1/4: TX = T × (¼)1/4 = T/√2.
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Answer C
Answer: C · 3 stages of work, one mark
Every option, and why
AThis takes the temperature to be proportional to the intensity received, instead of to its fourth root.
BThis takes the temperature to be inversely proportional to the distance.
CCorrect: T4 ∝ 1/d2, so T ∝ 1/√d.
DThis uses an inverse (not inverse-square) law for the intensity: (½)1/4.
Two metal panels on the radiator of a spacecraft are at the same temperature. Panel X is coated with a paint of emissivity 0.30 and emits 150 W m−2. Panel Y is coated with a paint of emissivity 0.90. σ = 5.67 × 10−8 W m−2 K−4
Which row gives the power emitted per unit area by panel Y and the temperature of the panels?
Power emitted per unit area by Y / W m−2Temperature / K
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Step 1Emissivity = (power radiated per unit area)/σT⁴, so at the same temperature the emission is proportional to the emissivity: 150 × 0.90/0.30 = 450 W m−2.
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All 2 steps must be completed — there is no mark for a part-answer.
Step 2For X: T⁴ = 150/(0.30 × 5.67 × 10−8) = 8.82 × 109 K⁴, so T = 306 K.
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Answer D
Answer: D · 2 stages of work, one mark
Every option, and why
AThis inverts the ratio of emissivities: the higher-emissivity paint emits more, not less.
BThis assumes surfaces at the same temperature emit equally whatever their emissivity.
CThe temperature here comes from σT⁴ = 150 W m−2, treating X as a black body and ignoring its emissivity.
DCorrect: Y emits three times as much as X, and both are at 306 K.
At a high-latitude site, sunlight of intensity 950 W m−2 (measured on a surface perpendicular to the rays) falls on level ground covered in snow. The rays make an angle of 65° with the vertical. The albedo of the snow is 0.80.
What is the power absorbed per unit area of the ground?
Diagram not to scale
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Step 1The beam is spread over a larger area of level ground: the intensity on the ground is 950 cos 65° = 401 W m−2.
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All 3 steps must be completed — there is no mark for a part-answer.
Step 2The fraction absorbed is 1 − albedo = 0.20.
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Step 3Absorbed: 0.20 × 401 = 80 W m−2. Oblique rays and high-albedo snow are why high latitudes absorb so little.
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Answer A
Answer: A · 3 stages of work, one mark
Every option, and why
ACorrect: 950 × cos 65° × (1 − 0.80) = 80 W m−2.
BThis uses sin 65° instead of cos 65°: 950 × 0.906 × 0.20 = 172 ≈ 170 W m−2.
CThis ignores the angle of the rays: 950 × 0.20 = 190 W m−2.
DThis uses the albedo as the fraction absorbed: 401 × 0.80 = 321 ≈ 320 W m−2.
The graph shows the fraction of radiation absorbed by a layer of gas X in the atmosphere, for wavelengths from 0.20 μm to 12 μm.
The surface temperature of the Sun is 5800 K and the mean surface temperature of the Earth is 288 K. Treat both as black bodies. Which row is correct?
Fraction of radiation absorbed by gas X against wavelength (drawn to scale)
X absorbs strongly at the peak wavelength of the Sun's radiationX absorbs strongly at the peak wavelength of the radiation from the Earth's surface
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Step 1Wien: λmax(Sun) = 2.9 × 10−3/5800 = 5.0 × 10−7 m = 0.50 μm, in the visible, where X absorbs only 0.02.
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All 3 steps must be completed — there is no mark for a part-answer.
Step 2λmax(Earth) = 2.9 × 10−3/288 = 1.01 × 10−5 m = 10.1 μm, inside the infrared band (9.3–10.5 μm), where X absorbs 0.80.
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Step 3So X lets most sunlight through but absorbs strongly near the peak of the Earth's emission: no / yes.
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Answer D
Answer: D · 3 stages of work, one mark
Every option, and why
AThis takes the ultraviolet band to contain the solar peak; 0.50 μm lies in the visible, beyond the end of the UV band at about 0.33 μm.
BThis uses λmax ∝ T, which gives the hotter Sun the longer peak wavelength; Wien's law gives λmax ∝ 1/T.
CThis uses the Earth's Celsius temperature: 2.9 × 10−3/15 = 1.9 × 10−4 m (190 μm), far beyond the graph, so the infrared band seems irrelevant.
DCorrect: the solar peak (0.50 μm) is where X is almost transparent; the Earth's peak (10 μm) lies inside the strongly absorbing infrared band, so X acts as a greenhouse gas.
11B-1A-65Equilibrium temperaturePaper 1AMedium1 mark
A moon with no atmosphere is in thermal equilibrium. When its only energy source is the solar radiation it absorbs, its mean surface temperature is T0.
Tidal heating then generates thermal energy inside the moon at a rate equal to a fraction f of the solar power it absorbs. This energy also leaves as radiation from the surface. The albedo and the emissivity of the surface do not change.
What is the new mean surface temperature in equilibrium?
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Step 1Energy balance before: eσAT04 = Pabs, where Pabs is the solar power absorbed.
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All 3 steps must be completed — there is no mark for a part-answer.
Step 2After: emitted power = Pabs + fPabs, so eσAT4 = (1 + f)Pabs.
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Step 3Dividing: (T/T0)4 = 1 + f, so T = T0(1 + f)1/4. (For f = 0.70 the temperature rises by 14 %.)
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Answer D
Answer: D · 3 stages of work, one mark
Every option, and why
AThis takes the emitted power to be proportional to T; the Stefan–Boltzmann law makes it proportional to T4.
BThis uses a square root, as if emitted power were proportional to T2 (or by confusion with T ∝ d−1/2 for distance from the Sun).
CThis takes the fourth root of the extra term only; the fourth root of (1 + f) is not 1 + f1/4.
DCorrect: the total emitted power is (1 + f) times the original, and emitted power ∝ T4.
12IBP2H-012-01-02Albedo and latitudePaper 1AMedium1 mark
At noon on an equinox, the Sun is directly overhead at the equator. A weather station at latitude 60° N measures the solar intensity on horizontal ground. Ignore any difference in absorption by the atmosphere. What is the ratio \(\frac{\text{intensity on horizontal ground at }60^\circ}{\text{intensity on horizontal ground at the equator}}\)?
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At latitude 60° the Sun's rays make an angle of 60° with the vertical. A beam of cross-sectional area A is therefore spread over a horizontal area A/cos 60°. The intensity on the ground is reduced by a factor of cos 60° = 0.50. The value 0.87 (sin 60°) uses the wrong trigonometric function. The value 0.25 squares the cosine without reason. The value 1.0 assumes that the same Earth–Sun distance gives the same intensity, which ignores the angle of incidence.
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Answer C
Answer: C
Exam tip: At an equinox, the angle between the Sun's rays and the vertical at noon equals the latitude. Intensity on horizontal ground scales with the cosine of that angle.
13IBP2H-012-01-03Greenhouse gasesPaper 1AMedium1 mark
Nitrogen and oxygen together make up about 99% of dry air, yet neither is a significant greenhouse gas. What is the best explanation?
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A molecule can absorb infrared radiation only if its vibration changes the separation of positive and negative charge, that is, its dipole moment. The oscillating electric field of the radiation can then drive the vibration at resonance. N2 and O2 consist of two identical atoms. When they stretch, the molecule remains non-polar, so no infrared energy is absorbed. Their concentration is very high, not low. Molecular mass is not the deciding factor. Their vibrational frequencies are in the infrared, not the radio region.
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Answer D
Answer: D
Common error: Abundance is not what makes a greenhouse gas. What matters is whether a molecular vibration changes the dipole moment at an infrared frequency.
14IBP2H-012-01-04Equilibrium temperaturePaper 1AMedium1 mark
A simple model of a planet has a single atmospheric layer. The layer is completely transparent to incoming sunlight and absorbs all of the infrared radiation emitted by the surface. The layer radiates equally upwards and downwards. The surface and the layer both behave as black bodies. Without the layer, the surface temperature would be T0. What is the surface temperature with the layer present?
Diagram not to scale
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With the layer present, the layer must radiate the absorbed solar power P to space from its top surface. It radiates the same power P downwards. The surface therefore receives P from the Sun and P from the layer, giving 2P in total. The surface must emit 2P, so σT4 doubles and T = 21/4T0 ≈ 1.19T0. Option A assumes that T is proportional to power. Option B uses a square root instead of a fourth root. Option D is the temperature of the atmospheric layer relative to the surface, not the surface relative to T0.
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Answer C
Answer: C
Exam tip: Write a separate energy balance for each layer. Doubling the radiated power multiplies the absolute temperature by only 2¹/⁴.
15IBP2H-012-01-06Equilibrium temperaturePaper 1AMedium1 mark
A rocky planet with no atmosphere orbits a star in radiative equilibrium. Its equilibrium temperature does not depend on
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The absorbed power is (1 − α)Iπr2 and the emitted power is σT4·4πr2. The r2 terms cancel, giving T4 = (1 − α)I/(4σ), which is independent of the radius. The intensity I depends on the orbital distance through the inverse-square law. I also depends on the star's luminosity, which depends on its surface temperature. The albedo appears directly in the expression.
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Answer C
Answer: C
Exam tip: The planet intercepts sunlight over its cross-sectional area πr² but emits from its whole surface area 4πr². This is where the factor of 4 comes from, and why r cancels.
Two spherical fuel tanks on a spacecraft are at the same temperature. Tank X has radius r and a surface emissivity of 0.90. Tank Y has radius 2r and a polished surface of emissivity 0.30. What is \(\frac{\text{power radiated by Y}}{\text{power radiated by X}}\)?
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P = eσAT4 with A = 4πr2. At equal T the ratio is (eYAY)/(eXAX) = (0.30 × 4r2)/(0.90 × r2) = 4/3. 1/3 ignores the area; 2/3 takes area ∝ r; 3/4 inverts the ratio.
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Answer D
Answer: D
Common error: Surface area scales with r²: doubling the radius multiplies the radiating area by 4, not 2.
17IBP2H-012-00-04Heat shield of a solar probePaper 1AMedium1 mark
The front face of the heat shield on a solar probe faces the Sun. Which combination of surface properties for this face gives the lowest equilibrium temperature for the shield?
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At equilibrium (1 − α)I = eσT4, so T4 = (1 − α)I/(eσ). A high albedo reduces the solar power absorbed, and a high emissivity lets the surface radiate the absorbed energy away at a lower temperature. Both lower T. A dark (low-albedo) surface absorbs more sunlight, and a low emissivity forces the surface to get hotter before it radiates enough.
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Answer A
Answer: A
Exam tip: Write T⁴ = (1 − α)I/(eσ) and read off which way each property moves T. This avoids mixing up absorbing and emitting.
18IBP2H-012-00-05Greenhouse gasesPaper 1AMedium1 mark
Carbon dioxide and water vapour absorb a large fraction of the radiation emitted by the Earth's surface but only a small fraction of the incoming solar radiation. What is the main reason for this?
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The Sun (about 5800 K) emits mostly visible light, while the surface (about 290 K) emits mostly infrared, peaking near 10 μm. Molecules such as CO2 and H2O have vibrational modes with natural frequencies in the infrared. They absorb that radiation by resonance, but they are largely transparent to visible light. The other options do not depend on wavelength, so they cannot explain why one kind of radiation is absorbed and the other is not.
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Answer B
Answer: B
Exam tip: Link the explanation to wavelength: Wien's law gives the different peak wavelengths, and resonance explains the selective absorption.
19IBP2H-012-00-06Equilibrium temperaturePaper 1AMedium1 mark
A thermal camera calculates temperature by assuming that every surface has emissivity 1. It is pointed at a polished steel pan at 400 K whose emissivity is 0.20. Ignore any radiation reflected by the pan. What temperature does the camera display?
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The camera receives 0.20σ(400)4 per unit area and interprets it as σTc4. So Tc = 400 × 0.201/4 = 400 × 0.669 ≈ 268 K. 80 K scales T linearly with e, 179 K uses a square root, and 400 K ignores emissivity altogether.
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Answer C
Answer: C
Common error: Emissivity multiplies the power, which goes as T⁴. The temperature therefore changes by the fourth root of e, not by e itself.
20IBP2H-012-00-07Equilibrium temperaturePaper 1AMedium1 mark
A star has a luminosity 16 times that of the Sun. An exoplanet orbits it at 2 AU and has the same albedo and emissivity as the Earth. The Earth's equilibrium temperature is T. What is the equilibrium temperature of the exoplanet?
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The intensity at the planet ∝ L/d2 = 16/22 = 4 times the Earth's solar constant. With the same albedo and emissivity, T4 ∝ intensity, so T ∝ 41/4 = √2. The answer is √2 T. 4T assumes T ∝ intensity, 2T assumes T ∝ √intensity, and T comes from wrongly dividing 16 by 24.
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Answer C
Answer: C
Exam tip: Find the intensity ratio first, then take its fourth root. Keeping these two steps separate prevents power errors.
21B-1A-23Surface–atmosphere energy balancePaper 1AHard1 mark
The surface of a planet absorbs a mean intensity of 160 W m−2 of solar radiation and 240 W m−2 of infrared radiation emitted downwards by its atmosphere. The surface also loses 40 W m−2 to the atmosphere by convection and evaporation. The emissivity of the surface is 0.90. (σ = 5.67 × 10−8 W m−2 K−4)
What is the equilibrium temperature of the surface?
Diagram not to scale
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Step 1In equilibrium the power radiated per unit area by the surface equals the net intensity it receives: eσT⁴ = 160 + 240 − 40 = 360 W m−2.
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All 3 steps must be completed — there is no mark for a part-answer.
22B-1A-40Equilibrium temperaturePaper 1AHard1 mark
A thin, flat sunshade is in space at the same distance from the Sun as the Earth, with one face perpendicular to the Sun's rays. The intensity of sunlight there is 1.36 × 103 W m−2. The sunlit face has an albedo of 0.20. The sunshade conducts well, so both faces are at the same temperature, and both faces have an emissivity of 0.80. σ = 5.67 × 10−8 W m−2 K−4
What is the equilibrium temperature of the sunshade?
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Step 1Power absorbed per unit area of the sunshade: (1 − 0.20) × 1360 = 1088 W m−2 (a flat sheet facing the Sun intercepts with its full area, so there is no factor of 1/4).
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All 3 steps must be completed — there is no mark for a part-answer.
Step 2Power emitted per unit area of the sunshade: two faces, each 0.80σT⁴, total 1.60σT⁴.
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Step 3T⁴ = 1088/(1.60 × 5.67 × 10−8) = 1.20 × 1010 K⁴, so T = 331 K.
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Answer C
Answer: C · 3 stages of work, one mark
Every option, and why
AThis uses the albedo as the fraction absorbed: 0.20 × 1360 = 272 W m−2 gives 234 K.
BThis treats both faces as black bodies (emissivity 1): 2σT⁴ = 1088 W m−2 gives 313 K.
CCorrect: 1088 = 1.60σT⁴.
DThis lets only the sunlit face radiate: 0.80σT⁴ = 1088 W m−2 gives 394 K.
23IBP2H-012-01-05Albedo and melting sea icePaper 1AHard1 mark
During summer, a patch of Arctic sea ice of albedo 0.60 melts completely to leave open ocean of albedo 0.10. The incident solar intensity is unchanged. By what factor does the solar power absorbed by the patch increase?
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The absorbed power is proportional to (1 − α). For the ice this is 1 − 0.60 = 0.40. For the ocean it is 1 − 0.10 = 0.90. The factor is 0.90/0.40 = 2.25. The value 6.0 is the ratio of the albedos, which compares reflected power, not absorbed power. The value 0.44 is the inverse ratio. The value 1.2 is 2.251/4, which would be a temperature ratio rather than a power ratio.
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Answer B
Answer: B
Common error: Albedo is the fraction reflected. Absorbed power depends on (1 − albedo), so never take the ratio of the albedos themselves.
24IBP2H-012-01-07Equilibrium temperaturePaper 1AHard1 mark
A space agency models an exoplanet with the same albedo as Earth and no greenhouse effect. The exoplanet orbits a star whose luminosity is 4 times that of the Sun, at a distance 4 times the Earth–Sun distance. Take Earth's equilibrium temperature without a greenhouse effect to be 255 K. What is the best estimate of the exoplanet's equilibrium temperature?
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The intensity is proportional to L/d2. This gives 4/42 = 1/4 of the solar constant. The equilibrium temperature is proportional to I1/4, so T = 255 × (1/4)1/4 = 255/√2 ≈ 180 K. The value 64 K treats T as proportional to I. The value 128 K treats T as proportional to √I. The value 255 K assumes the luminosity and distance factors cancel, forgetting that intensity follows an inverse-square law.
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Answer C
Answer: C
Exam tip: Find the intensity ratio first, then take the fourth root. (1/4)¹/⁴ = 1/√2, which is easy to evaluate without a calculator.
25IBP2H-012-00-08Equilibrium temperaturePaper 1AHard1 mark
Planets A and B receive the same solar intensity and have the same albedo. Both emit as black bodies. Planet A rotates rapidly and emits uniformly from its whole surface. Planet B is tidally locked: model it as re-emitting all the energy it absorbs from its sunlit hemisphere only, at a uniform temperature. What is \(\frac{T_B}{T_A}\)?
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Both planets absorb (1 − α)SπR2. A emits from 4πR2 and B from 2πR2. Equating absorbed and emitted power gives TB4/TA4 = 4πR2/2πR2 = 2, so TB/TA = 21/4 ≈ 1.19. √2 and 2 use the wrong power of T. 2−1/4 wrongly concludes that the smaller emitting area makes B cooler.
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Answer D
Answer: D
Exam tip: In any energy-balance model, write the absorbing area (a cross-section) and the emitting area as separate quantities before equating powers.
To estimate the solar constant, a student places a thin aluminium disc of diameter 4.00 cm and mass 12.0 g, blackened on its upper face, so that it faces the Sun directly at midday. The disc rests on polystyrene. Its temperature θ is read every 30 s with a digital thermometer of resolution 0.1 °C. The specific heat capacity of aluminium is 900 J kg−1 K−1. The table and the graph show the results with the line of best fit.
t / s
0
30
60
90
120
150
θ / °C
18.0
21.2
23.8
27.1
30.2
32.9
Temperature θ of the disc against time t with the line of best fit (drawn to scale)
(a)
(i)
A classmate calculates the rate of rise of temperature from the first two readings only. Determine the rate of rise of temperature in a way that is more reliable, and explain your choice.
(2)
(b)
(i)
Determine the intensity of the solar radiation absorbed by the disc.
(2)
(c)
(i)
At the time of the experiment the atmosphere transmits 72 % of the solar radiation arriving at its top. Estimate the solar constant from the student's data.
(1)
(ii)
The accepted value of the solar constant is 1360 W m−2. Suggest, with a reason, why the student's estimate differs from this value.
(2)
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Part (a)(i)
Gradient of the line of best fit over the full range, e.g. (34.0 − 18.0)/160 = 0.10 K s−1
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Accept 0.097–0.103 K s−1. The first two readings give 0.107 K s−1: award [0] for this value.
The line uses all six readings over the whole range, so the random scatter (±0.2 °C, larger than the 0.1 °C resolution) has much less effect than in a 30 s interval
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OWTTE.
Part (b)(i)
Power absorbed = mc × gradient = 0.0120 × 900 × 0.10 = 1.08 W
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Assumes all the energy absorbed raises the temperature of the disc.
Area = π × 0.0200² = 1.26 × 10−3 m²; intensity = 859 W m−2
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Allow ECF from (a). Accept 830–880 W m−2.
Part (c)(i)
S = 859/0.72 = 1190 W m−2
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Allow ECF from (b).
Part (c)(ii)
The estimate is about 12 % too low
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Allow ECF from (c)(i). The direction of the difference must agree with the candidate's value.
The disc loses energy to the air (convection) and to its support while it warms, and its surface is not a perfect absorber, so less power raises its temperature than is incident on it
✓ 1
Accept also: the disc is not exactly perpendicular to the rays. "Human error" scores [0].
Answers: (a)(i) 0.10 K s−1 · (b)(i) 859 W m−2 · (c)(i) 1190 W m−2(the remaining parts are explanations — see the table above)
27B-1B-03Energy balance of a planetPaper 1BMedium7 marks
Three planets b, c and d orbit a faint star of mass 4.0 × 1029 kg and luminosity 2.0 × 1024 W in circular orbits. Their orbital periods are found from the regular dips in the star's brightness as each planet passes in front of it. Infrared observations of planet c suggest a mean surface temperature of 341 K. Astronomers want to know whether planet c could have an atmosphere. They model each planet as a black body with an albedo of 0.30 that radiates from its whole surface.
Planet
b
c
d
Orbital period / days
4.0
9.2
20.5
Orbital radius / 1010 m
0.432
1.28
(a)
(i)
Show that the orbital radius of planet c is about 7.5 × 109 m.
(2)
(b)
(i)
Determine the equilibrium surface temperature of planet c predicted by the model.
(3)
(c)
(i)
Discuss, with reference to your answer to (b), whether the infrared observation supports the suggestion that planet c has an atmosphere.
(2)
Show mark scheme
Marking point
Mark
Notes
Part (a)(i)
r³ = GMT²/4π² with T = 9.2 × 86 400 = 7.95 × 105 s
✓ 1
Kepler's third law from the data booklet; the conversion of days to seconds is required.
r = (6.67 × 10−11 × 4.0 × 1029 × (7.95 × 105)²/4π²)1/3 = 7.53 × 109 m
✓ 1
Answer to at least 3 s.f. Alternative: scale from planet b or d with r³ ∝ T².
Part (b)(i)
Intensity at c: S = L/4πr² = 2.0 × 1024/(4π × (7.53 × 109)²) = 2810 W m−2
✓ 1
Allow ECF from (a). Using 7.5 × 109 m gives 2830 W m−2.
Absorbed mean intensity = (1 − 0.30) × S/4 = 491 W m−2
✓ 1
The factor 1/4 (projected disc versus whole sphere) is required.
T = (491/5.67 × 10−8)1/4 = 305 K
✓ 1
Accept 300–310 K.
Part (c)(i)
341 K is about 36 K higher than the model value, more than the model's uncertainty would suggest
✓ 1
Allow ECF from (b). The comparison must use the candidate's value.
An atmosphere containing greenhouse gases absorbs part of the outgoing infrared and re-emits some back to the surface, raising the surface temperature, so the observation supports the suggestion
✓ 1
Accept also a lower true albedo, or internal/tidal heating, as an alternative explanation that weakens the conclusion.
Answers: (a)(i) 7.53 × 109 m · (b)(i) 305 K (the remaining parts are explanations — see the table above)
A satellite instrument measures the monthly mean albedo α of several regions of tropical ocean, together with the fraction f of each region covered by cloud. The graph shows α against f. Each albedo has an uncertainty of ±0.02, shown by the error bars. The solid line is the line of best fit; the dashed lines are the steepest and the shallowest lines that pass through all the error bars. The mean solar intensity arriving at the top of the atmosphere above these regions is 410 W m−2.
Cloud fraction f
0.10
0.25
0.40
0.55
0.70
0.85
Albedo α
0.12
0.20
0.29
0.35
0.44
0.50
Albedo against cloud fraction with error bars, line of best fit (solid) and steepest/shallowest lines (dashed) (drawn to scale)
(a)
(i)
Determine the gradient of the line of best fit.
(1)
(ii)
Determine the absolute uncertainty in the gradient.
(2)
(b)
(i)
Determine the difference between the mean intensities absorbed by a region with f = 0.20 and a region with f = 0.70, with its uncertainty.
(2)
(c)
(i)
A climate model assumes that the albedo of tropical ocean completely covered by cloud is 0.65. Deduce whether the data are consistent with this assumption.
A student measures the emissivity e of a matt paint. A metal plate painted on one face is heated electrically, and its temperature is measured with a thermometer embedded in the metal. A calibrated detector gives the net power radiated per unit area, I, from the painted face. The surroundings are at an unknown kelvin temperature Tr. The net intensity is modelled by
I = eσ(T⁴ − Tr⁴)
where T is the kelvin temperature of the plate. The graph shows I against T⁴ with the line of best fit, extended to lower values of T⁴.
θ / °C
40
60
80
100
120
140
T / K
313
333
353
373
393
413
T⁴ / 109 K⁴
9.60
12.30
15.53
19.36
23.85
29.09
I / W m−2
87
203
333
489
692
924
I against T⁴ with the line of best fit; the grey line marks I = 0 (drawn to scale)
(a)
(i)
Explain why the net intensity depends on T⁴ − Tr⁴ rather than on T⁴ alone.
(1)
(b)
(i)
Determine the emissivity of the paint.
(3)
(c)
(i)
Determine Tr in °C.
(2)
(d)
(i)
The manufacturer gives the emissivity of the paint as 0.90. Air flowing past the plate cools the painted surface slightly below the temperature of the metal. Explain how this accounts for the difference from your answer to (b).
(1)
Show mark scheme
Marking point
Mark
Notes
Part (a)(i)
The plate emits eσT⁴ per unit area but also absorbs radiation from the surroundings that depends on Tr⁴; I is the difference
✓ 1
Part (b)(i)
Gradient from two well-separated points on the line, e.g. (924 − 87)/((29.09 − 9.60) × 109) = 4.3 × 10−8 W m−2 K−4
✓ 1
Accept 4.1–4.5 × 10−8. The factor 109 is required.
Gradient = eσ, so e = gradient/σ
✓ 1
e = 4.3 × 10−8/5.67 × 10−8 = 0.76
✓ 1
Accept 0.72–0.79.
Part (c)(i)
I = 0 when T⁴ = Tr⁴: the extended line crosses I = 0 at T⁴ ≈ 7.7 × 109 K⁴
✓ 1
Allow ECF from (b). Accept 7.4–7.9 × 109 K⁴, or |intercept|/gradient = 328/4.3 × 10−8.
Tr = (7.7 × 109)1/4 = 296 K = 23 °C
✓ 1
Accept 20–26 °C.
Part (d)(i)
The surface radiates at a lower temperature than the recorded T, so each measured I is too small for the plotted T⁴: the gradient, and hence e, is underestimated (0.76 < 0.90)
✓ 1
Allow ECF from (b). The direction must be explained, not just stated.
Answers: (b)(i) 0.76 · (c)(i) 23 °C (the remaining parts are explanations — see the table above)
30B-2-35Albedo and melting sea icePaper 2Easy12 marks
In summer the mean intensity of sunlight reaching the surface of a region of the Arctic Ocean, averaged over day and night, is 300 W m−2. Part of the region is covered by sea ice of albedo 0.60; the rest is open sea water of albedo 0.06.
Density of ice = 917 kg m−3; specific latent heat of fusion of ice = 3.34 × 105 J kg−1.
(a)
(i)
Calculate the intensity of the sunlight absorbed by the ice.
(1)
(ii)
When the ice melts, open water is exposed. Determine the additional energy absorbed by each square metre of the surface in one day.
(2)
(b)
(i)
A sheet of sea ice 1.2 m thick is at 0 °C. Estimate the number of days for which the additional energy in (a)(ii) would have to be absorbed to melt 1.0 m² of this ice.
(3)
(c)
(i)
Explain, with reference to your answers to (a), why the loss of sea ice tends to cause further warming of the Arctic Ocean.
(2)
(d)
(i)
Sea ice floats. Show that when a block of floating ice melts, the level of the water does not change. Assume that the density of the sea water is the same as the density ρw of the melt water.
(2)
(e)
(i)
Thawing of frozen ground releases methane into the atmosphere. State one other natural source of atmospheric methane and one source that is due to human activity.
(2)
Show mark scheme
Marking point
Mark
Notes
Part (a)(i)
(1 − 0.60) × 300 = 120 W m−2
✓ 1
Part (a)(ii)
Open water absorbs 0.94 × 300 = 282 W m−2; the increase is 282 − 120 = 162 W m−2
✓ 1
Allow ECF from (a)(i).
Energy = 162 × 86 400 = 1.40 × 107 J
✓ 1
Accept 1.4 × 107 J. The time must be in seconds.
Part (b)(i)
Mass of ice = 917 × 1.2 × 1.0 = 1100 kg
✓ 1
Energy needed = 1100 × 3.34 × 105 = 3.7 × 108 J
✓ 1
Number of days = 3.7 × 108/1.4 × 107 ≈ 26
✓ 1
Allow ECF from (a)(ii). Accept 25–27 days. Award [2 max] for 15 days (total absorption of the water used instead of the additional absorption).
Part (c)(i)
Open water has a much lower albedo, so it absorbs a larger fraction of the sunlight (282 instead of 120 W m−2) and the water warms
✓ 1
Allow ECF from the candidate's values in (a).
The warmer water melts more ice, which exposes more water, so the absorption increases further (the effect reinforces itself)
✓ 1
The self-reinforcing link is required for this mark.
Part (d)(i)
The floating ice is in equilibrium, so the buoyancy force equals its weight: ρwVdispg = mg, giving Vdisp = m/ρw
✓ 1
Use of Fb = ρVg is required.
The melt water has the same mass m, so its volume is m/ρw = Vdisp: it exactly fills the volume the ice displaced, and the level is unchanged
✓ 1
Mass is conserved on melting; this must be stated or used.
Part (e)(i)
Natural: any one of wetlands (marshes, swamps); termites; wild animals (ruminants); natural gas seeping from the ground or sea floor; wildfires
✓ 1
Thawing frozen ground (permafrost) is given in the stem and is not accepted.
Human activity: any one of livestock farming (cattle); rice paddies; landfill sites; leaks from natural-gas wells, pipelines or coal mines
✓ 1
"Burning fossil fuels" alone is not accepted (it mainly releases CO2).
Answers: (a)(i) 120 W m−2 · (a)(ii) 1.40 × 107 J · (b)(i) 26 days (the remaining parts are explanations — see the table above)
31IBP2H-012-01-09Energy balance of a planetPaper 2Easy5 marks
A team planning a crewed Mars mission needs an estimate of the planet's equilibrium temperature. Mars orbits at 1.52 times the Earth–Sun distance and has a mean albedo of 0.25. The solar constant at Earth is 1360 W m−2. Treat Mars as a black-body emitter with no greenhouse effect.
(a)
Calculate the intensity of solar radiation at the orbit of Mars.
(1)
(b)
Explain why the mean solar power absorbed per unit area of the Martian surface is \(\frac{(1-\alpha)I}{4}\).
(2)
(c)
Calculate the equilibrium temperature of Mars.
(2)
Show mark scheme
Marking point
Mark
Notes
Part (a)
I = 1360/1.522 = 589 W m−2
✓ 1
Part (b)
Sunlight is intercepted over the cross-sectional area πr2, but the power is spread over the whole surface area 4πr2, so the mean incident intensity is I/4 . A fraction α is reflected, so only a fraction (1 − α) is absorbed .
✓ 2
Part (c)
σT4 = 0.75 × 589/4 = 110 W m−2 . T = (110/5.67×10−8)1/4 = 210 K; allow error carried forward from the intensity calculated in the first part .
✓ 2
Exam tip: Keep the albedo factor and the factor of 4 in the same line of working. Leaving out either one is the quickest way to lose a mark.
A cyclist at rest after a race has an exposed skin area of 1.8 m2 at a temperature of 306 K. The emissivity of skin in the infrared is 0.97. The surroundings are at 293 K. Take σ = 5.67×10−8 W m−2 K−4.
(a)
Calculate the total power radiated by the cyclist's skin.
(2)
(b)
Determine the net rate at which the cyclist loses energy by radiation.
(2)
(c)
Outline why the net rate of energy loss by radiation is much smaller than the total power radiated by the skin.
33B-2-13Energy balance of a planetPaper 2Medium9 marks
Mars orbits the Sun at a mean distance of 2.28 × 1011 m. Luminosity of the Sun = 3.83 × 1026 W; radius of the Earth's orbit = 1.50 × 1011 m.
(a)
(i)
Show that the intensity of sunlight at the mean distance of Mars is about 590 W m−2.
(1)
(b)
(i)
Mars has an albedo of 0.25. Determine the equilibrium temperature of Mars, assuming that the surface radiates as a black body and that the atmosphere has no effect.
(3)
(c)
(i)
Determine, in Earth years, the orbital period of Mars.
(1)
(d)
(i)
The distance of Mars from the Sun varies between 2.07 × 1011 m and 2.49 × 1011 m. Show that the equilibrium temperature is proportional to d−1/2, and determine the difference between the highest and the lowest equilibrium temperatures.
(2)
(e)
(i)
The measured mean surface temperature of Mars is about 210 K. Its atmosphere is mainly carbon dioxide at a very low pressure. Deduce what this suggests about the greenhouse effect on Mars.
(2)
Show mark scheme
Marking point
Mark
Notes
Part (a)(i)
S = L/4πd² = 3.83 × 1026/(4π × (2.28 × 1011)²) = 586 W m−2
✓ 1
An answer to at least 3 s.f. is required.
Part (b)(i)
Mean incoming intensity = S/4 = 147 W m−2 (sunlight is intercepted by the cross-section πR² but the energy is radiated from the whole surface 4πR²)
✓ 1
Allow ECF from (a).
Absorbed intensity = 0.75 × 147 = 110 W m−2
✓ 1
T = (110/5.67 × 10−8)1/4 = 210 K
✓ 1
Award [2 max] for 297 K (factor 4 omitted).
Part (c)(i)
Kepler's third law: T² ∝ r³, so TMars = (2.28/1.50)3/2 × 1 year = 1.87 years
✓ 1
Part (d)(i)
T⁴ ∝ S ∝ 1/d², so T ∝ d−1/2
✓ 1
210 × (2.28/2.07)1/2 = 220 K and 210 × (2.28/2.49)1/2 = 201 K: difference ≈ 19 K
✓ 1
Allow ECF from (b). Accept 18–20 K.
Part (e)(i)
The measured temperature is about equal to the value from (b), so the greenhouse effect on Mars is very small
✓ 1
Allow ECF from (b).
The thin atmosphere contains few CO2 molecules above each square metre, so it absorbs, and re-emits back towards the surface, only a small fraction of the infrared emitted by the surface
✓ 1
Answers: (a)(i) 586 W m−2 · (b)(i) 210 K · (c)(i) 1.87 years · (d)(i) ≈ 19 K (the remaining parts are explanations — see the table above)
Carbon dioxide molecules absorb infrared radiation of wavelength 15.0 μm, which makes the molecules vibrate (bend). In a simple resonance model, this vibration is treated as an oxygen atom of mass 2.66 × 10−26 kg oscillating on a spring of spring constant k.
(a)
(i)
Calculate the frequency of the radiation.
(1)
(b)
(i)
Calculate, in eV, the energy of a photon of this radiation.
(1)
(c)
(i)
Determine the value of k for which the natural frequency of the model is equal to the frequency of the radiation.
(1)
(d)
(i)
Explain, using the resonance model, how carbon dioxide in the atmosphere reduces the energy radiated from the Earth's surface to space at this wavelength.
(2)
(e)
(i)
In a molecule containing the heavier isotope oxygen-18, the vibrating mass is 18/16 times larger and k is unchanged. Deduce the wavelength absorbed by this molecule.
(2)
(f)
(i)
State one limitation of the resonance model of the greenhouse effect.
(1)
Show mark scheme
Marking point
Mark
Notes
Part (a)(i)
f = c/λ = 3.00 × 108/15.0 × 10−6 = 2.00 × 1013 Hz
✓ 1
Part (b)(i)
E = hf = 6.63 × 10−34 × 2.00 × 1013 = 1.33 × 10−20 J = 0.083 eV
✓ 1
Allow ECF from (a). The answer in eV is required.
Part (c)(i)
T = 2π√(m/k), so k = 4π²f²m; k = 4π² × (2.00 × 1013)² × 2.66 × 10−26 = 420 N m−1
✓ 1
Allow ECF from (a).
Part (d)(i)
Radiation at the natural frequency of the bond drives the vibration at resonance, so the amplitude becomes large and energy is absorbed from the radiation
✓ 1
The absorbed energy is re-emitted in all directions (or shared with other molecules by collisions), so part of it returns towards the surface and less escapes to space
✓ 1
Part (e)(i)
f ∝ 1/√m, so λ ∝ √m
✓ 1
λ = 15.0 × √(18/16) = 15.9 μm
✓ 1
Award [1 max] for 16.9 μm (λ ∝ m).
Part (f)(i)
It is a classical model: it does not explain why only particular (discrete) photon energies are absorbed, which requires molecular energy levels
✓ 1
Accept any valid limitation, e.g. it cannot predict which gases absorb.
Answers: (a)(i) 2.00 × 1013 Hz · (b)(i) 0.083 eV · (c)(i) 420 N m−1 · (e)(i) 15.9 μm (the remaining parts are explanations — see the table above)
35B-2-22Heat shield of a solar probePaper 2Medium13 marks
A spacecraft studying the Sun carries a flat heat shield that always faces the Sun. At its closest approach the spacecraft is 6.9 × 109 m from the centre of the Sun.
Luminosity of the Sun L☉ = 3.83 × 1026 W; solar constant at the Earth S = 1.36 × 103 W m−2; σ = 5.67 × 10−8 W m−2 K−4
Diagram not to scale
(a)
Intensity.
(i)
Show that the intensity of sunlight at closest approach is about 6.4 × 105 W m−2.
(2)
(ii)
Use your answer to (a)(i) and the solar constant to determine the distance of the Earth from the Sun.
(2)
(b)
The sunlit face of the shield has an albedo of 0.60 and an emissivity of 0.90. Assume that all the energy absorbed by the shield is re-radiated from its sunlit face.
(i)
Determine the equilibrium temperature of the sunlit face.
(3)
(ii)
State this temperature in °C.
(1)
(iii)
Calculate the wavelength at which the radiation emitted by the shield is most intense.
(1)
(c)
Behind the sunlit face is a layer of carbon foam of thickness 0.11 m and thermal conductivity 0.050 W m−1 K−1. The back of the foam is at 330 K.
(i)
Calculate the rate of conduction of energy per unit area through the foam.
(1)
(ii)
Hence comment on the assumption made in (b).
(1)
(d)
The coating.
(i)
Explain why the sunlit face is given a white, high-albedo coating, and determine the temperature it would reach if its albedo were 0.10 with the same emissivity.
(2)
Show mark scheme
Marking point
Mark
Notes
Part (a)(i)
b = L☉/4πd² = 3.83 × 1026/(4π × (6.9 × 109)²)
✓ 1
b = 6.40 × 105 W m−2
✓ 1
Answer to more figures than the target, e.g. 6.40 × 105 W m−2.
Part (a)(ii)
b ∝ 1/d², so dE = 6.9 × 109 × √(6.40 × 105/1360) = 6.9 × 109 × 21.7
This is about 0.2 % of the absorbed 2.56 × 105 W m−2, so almost all the absorbed energy is indeed re-radiated from the sunlit face: the assumption is justified
✓ 1
Part (d)(i)
A higher albedo reflects more of the incident radiation, so less is absorbed and the equilibrium temperature is lower
✓ 1
T ∝ (1 − albedo)1/4: T = 1497 × (0.90/0.40)1/4 = 1.8 × 103 K
✓ 1
Accept 1830–1840 K.
Answers: (a)(i) 6.40 × 105 W m−2 · (a)(ii) 1.5 × 1011 m · (b)(i) 1.5 × 103 K · (b)(ii) 1.2 × 103 °C · (b)(iii) 1.9 × 10−6 m · (c)(i) 5.3 × 102 W m−2 · (d)(i) 1.8 × 103 K (the remaining parts are explanations — see the table above)
36IBP2H-012-01-10Albedo and melting sea icePaper 2Medium7 marks
A climate research group studies a region of the Arctic Ocean during one summer. The table shows typical albedos. Surface | Albedo Fresh snow on ice | 0.85 Bare sea ice | 0.60 Open ocean | 0.06 Over a 30-day period, the mean solar intensity reaching the surface is 200 W m−2. During this period, an area of 2.0×105 km2 of bare sea ice becomes open ocean. The specific latent heat of fusion of ice is 3.3×105 J kg−1.
(a)
Calculate the increase in solar power absorbed by this area when it changes from bare sea ice to open ocean.
(2)
(b)
Explain how the change in surface described in the previous part can lead to a positive feedback.
(2)
(c)
Determine the mass of ice that the extra energy absorbed over the 30 days could melt. Assume that all of this extra energy is used to melt ice that is already at its melting point.
(3)
Show mark scheme
Marking point
Mark
Notes
Part (a)
Area = 2.0×1011 m2 and the change in absorbed fraction = 0.60 − 0.06 = 0.54 . ΔP = 200 × 0.54 × 2.0×1011 = 2.2×1013 W .
✓ 2
Part (b)
The extra absorbed energy warms the ocean surface water . The warmer water melts more of the surrounding ice, which exposes more low-albedo ocean, so absorption increases further .
✓ 2
Part (c)
t = 30 × 86400 = 2.59×106 s . E = ΔP × t = 2.2×1013 × 2.59×106 ≈ 5.6×1019 J. Accept 5.7×1019 J if the rounded power is used, and allow error carried forward from the first part . m = E/L = 5.6×1019/3.3×105 = 1.7×1014 kg .
✓ 3
Common error: Convert km² to m² by multiplying by 10⁶, not 10³.
37IBP2H-012-01-14Heat shield of a solar probePaper 2Medium7 marks
A building engineer is considering a reflective 'cool roof' coating for a flat roof of area 120 m2. At midday, the solar intensity on the roof is 850 W m−2. The existing roof has an albedo of 0.15. The coated roof has an albedo of 0.80. Both surfaces have an infrared emissivity of 0.90.
(a)
Calculate the reduction in solar power absorbed by the roof after coating.
(2)
(b)
Explain why the ideal coating has a high albedo for visible light but a high emissivity in the infrared.
(2)
(c)
Estimate the midday temperature of the uncoated roof, assuming radiation is its only means of losing energy. Suggest why the actual temperature is lower.
(3)
Show mark scheme
Marking point
Mark
Notes
Part (a)
Absorbed fraction = 1 − albedo, so the change in absorbed fraction = 0.85 − 0.20 = 0.65 . ΔP = 850 × 120 × 0.65 ≈ 6.6×104 W .
✓ 2
Part (b)
A high albedo for visible and near-infrared sunlight reflects most of the incoming solar energy, so less is absorbed . The roof emits at its own much longer (infrared) wavelengths, and a high infrared emissivity lets it radiate away the energy it does absorb efficiently, keeping it cool .
✓ 2
Part (c)
0.85 × 850 = 0.90σT4, so T4 = 722.5/(0.90 × 5.67×10−8) ≈ 1.42×1010 K4 . T ≈ 345 K . In reality, convection to the surrounding air and/or conduction into the building also remove energy, so less energy has to be lost by radiation and the roof is cooler .
✓ 3
Common error: Albedo describes reflection of incoming sunlight, while emissivity describes infrared emission at the surface's own temperature. A surface can be highly reflective and still a strong infrared emitter.
38IBP2H-012-01-15Greenhouse gasesPaper 2Medium7 marks
In hospitals, a capnograph measures the concentration of carbon dioxide in a patient's exhaled breath. It does this by measuring how much infrared radiation of wavelength 4.26 μm is absorbed as it passes through the breath sample. Exhaled breath also contains nitrogen, oxygen and water vapour. Wien's constant b = 2.9×10−3 m K; c = 3.00×108 m s−1; mean surface temperature of the Earth = 288 K.
(a)
Explain why nitrogen and oxygen in the breath do not affect the reading.
(2)
(b)
Calculate the frequency of the radiation used.
(1)
(c)
Determine the temperature of a black body whose emission peaks at 4.26 μm. Hence, using the data given, outline why the 4.26 μm CO2 absorption band contributes far less to the Earth's greenhouse effect than the 15 μm band.
(4)
Show mark scheme
Marking point
Mark
Notes
Part (a)
A molecule absorbs infrared radiation only if its vibration changes its electric dipole moment . N2 and O2 are symmetric diatomic molecules whose vibration produces no change in dipole moment, so they do not absorb at 4.26 μm .
✓ 2
Part (b)
f = c/λ = 3.00×108/4.26×10−6 = 7.04×1013 Hz
✓ 1
Part (c)
T = b/λmax = 2.9×10−3/4.26×10−6 . T ≈ 6.8×102 K (681 K) . At 288 K the Earth's surface emission peaks at about 2.9×10−3/288 ≈ 10 μm, which is much closer to 15 μm than to 4.26 μm . The surface emits very little power at 4.26 μm, so absorption in this band traps little outgoing energy compared with the 15 μm band .
✓ 4
Exam tip: How strongly a gas absorbs at a wavelength matters only if the surface emits significant power there. Compare the absorption band with the peak of the Earth's emission, which you can find using Wien's law.
39IBP2H-012-00-11Energy balance of a planetPaper 2Medium7 marks
A space telescope surveys three rocky planets orbiting the same star. The table gives the stellar intensity at each planet's orbit, its albedo and its measured mean surface temperature.
Planet | Intensity / W m−2 | Albedo | Surface temperature / K b | 2600 | 0.10 | 370 c | 1100 | 0.35 | 300 d | 450 | 0.20 | 205
Assume each planet rotates rapidly. σ = 5.67×10−8 W m−2 K−4.
(a)
Show that the equilibrium temperature of planet c, treated as a black-body emitter, is about 240 K.
(2)
(b)
The equilibrium temperatures of planets b and d are 319 K and 200 K. Identify, with a reason, the planet with the strongest greenhouse effect.
(2)
(c)
Determine the effective emissivity of planet c, treating the planet and its atmosphere as a single surface at its measured surface temperature.
(2)
(d)
Outline one reason why planet d might show very little greenhouse effect.
(1)
Show mark scheme
Marking point
Mark
Notes
Part (a)
Mean absorbed intensity = (1 − 0.35) × 1100/4 = 179 W m−2
✓ 1
T = (179/5.67×10−8)1/4 = 237 K
✓ 1
Part (b)
Planet c
✓ 1
Its surface temperature exceeds its equilibrium temperature by about 63 K, compared with about 51 K for b and about 5 K for d (allow comparison of the ratios of surface to equilibrium temperature)
✓ 1
Part (c)
e = absorbed intensity/(σTs4) = 179/(5.67×10−8 × 3004)
✓ 1
e ≈ 0.39
✓ 1
Allow error carried forward from the first part
—
Part (d)
Any one: thin or absent atmosphere / very low concentration of greenhouse gases / water vapour frozen out as surface ice at such low temperatures, so little remains in the atmosphere
✓ 1
Common error: Remember to divide by 4 for a rapidly rotating planet. The planet intercepts power over πR² but radiates from 4πR².
40IBP2H-012-00-13Equilibrium temperaturePaper 2Medium7 marks
A thin flat solar panel on a CubeSat in Earth orbit faces the Sun directly. The solar intensity is 1360 W m−2. The panel reflects 15% of the incident sunlight. Both faces have emissivity 0.85, and the panel radiates from both faces at a uniform temperature. σ = 5.67×10−8 W m−2 K−4.
(a)
The panel is switched off. Calculate its equilibrium temperature.
(3)
(b)
The panel is switched on and delivers electrical energy, used elsewhere in the satellite, at a rate equal to 20% of the incident solar intensity. Determine the new equilibrium temperature of the panel.
(3)
(c)
Explain why the equilibrium temperature does not depend on the area of the panel.
(1)
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Notes
Part (a)
Absorbed intensity = 0.85 × 1360 = 1156 W m−2
✓ 1
Emitted from both faces: 1156 = 2 × 0.85 × σT4
✓ 1
T ≈ 331 K
✓ 1
Part (b)
Power per unit area to be radiated = 1156 − 0.20 × 1360 = 884 W m−2
✓ 1
884 = 2 × 0.85 × 5.67×10−8 × T4
✓ 1
T ≈ 309 K (accept 309–310 K)
✓ 1
Allow error carried forward from an incorrect absorbed intensity in the first part
—
Part (c)
Both the absorbed and the emitted power are proportional to the area, so the area cancels in the energy balance
✓ 1
Common error: A panel that radiates from both faces has twice its face area as emitting area. Leaving out the factor 2 makes T too high by a factor of 2¹/⁴.
41IBP2H-012-00-14Energy balance of a planetPaper 2Medium7 marks
A red dwarf star has a surface temperature of 3100 K and a radius of 1.46×108 m. Astronomers look for a planet orbiting where the stellar intensity equals the Earth's solar constant, 1360 W m−2. Treat the star as a black body. σ = 5.67×10−8 W m−2 K−4; Wien constant = 2.9×10−3 m K.
(a)
Calculate the peak wavelength of the star's emission.
(1)
(b)
Calculate the luminosity of the star.
(2)
(c)
Determine the orbital radius at which the intensity is 1360 W m−2.
(2)
(d)
Snow and ice reflect visible light strongly but absorb much of the near-infrared. Suggest how this affects the energy balance of an icy planet at this orbit compared with an icy planet orbiting the Sun.
(2)
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Notes
Part (a)
λmax = 2.9×10−3/3100 = 9.4×10−7 m
✓ 1
Part (b)
L = 4πR2σT4 = 4π(1.46×108)2 × 5.67×10−8 × 31004
✓ 1
L ≈ 1.4×1024 W
✓ 1
Part (c)
I = L/(4πd2), so d = √(L/(4π × 1360))
✓ 1
d ≈ 9.1×109 m
✓ 1
ECF from (b)
—
Part (d)
Much of this star's radiation is near-infrared (peak about 0.94 μm), so the ice's effective albedo is lower
✓ 1
The planet absorbs a larger fraction of the incident intensity and so reaches a higher equilibrium temperature
✓ 1
Exam tip: Algebra first: d = RT²√(σ/I). Cancelling 4π before substituting numbers shortens the calculation.
42B-2-23Surface–atmosphere energy balancePaper 2Hard14 marks
A rocky planet with an atmosphere orbits a distant star. The intensity of the starlight at the distance of the planet is S = 2.00 × 103 W m−2.
The diagram shows the mean energy flows per unit area of the planet's surface, in W m−2. Of the 520 W m−2 emitted by the surface, 40 W m−2 passes directly through the atmosphere to space and the rest is absorbed by the atmosphere. σ = 5.67 × 10−8 W m−2 K−4
Mean energy flows per unit area of the planet's surface, in W m−2. Gold: starlight; red: infrared radiation; grey: convection and evaporation. P, Q and R are unknown.
(a)
(i)
Outline why the mean intensity of the incoming starlight shown in the diagram is 500 W m−2.
(1)
(ii)
Determine the albedo of the planet and the value of P.
(2)
(b)
(i)
By considering the energy balance of the surface, determine Q.
(2)
(ii)
By considering the energy balance of the atmosphere, determine R, and verify that the planet as a whole is in energy balance.
(2)
(c)
(i)
The emissivity of the surface is 0.95. Determine the mean surface temperature.
(1)
(d)
(i)
Explain, with reference to the energy flows in the diagram, why an increase in the concentration of greenhouse gases in the atmosphere would raise the surface temperature.
(3)
(e)
(i)
The star has a luminosity of 2.7 × 1026 W and a mass of 1.8 × 1030 kg. Determine, in Earth days, the orbital period of the planet.
(3)
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Part (a)(i)
The planet intercepts starlight over its cross-section πR² but the energy is shared over its whole surface 4πR², so the mean is S/4 = 2000/4 = 500 W m−2
✓ 1
The ratio of the two areas must be seen.
Part (a)(ii)
Albedo = 160/500 = 0.32
✓ 1
P = 500 − 160 − 90 = 250 W m−2
✓ 1
Part (b)(i)
Surface: energy in = energy out, so P + Q = 520 + 110
✓ 1
Q = 630 − 250 = 380 W m−2
✓ 1
Allow ECF from (a)(ii).
Part (b)(ii)
Atmosphere: 90 + (520 − 40) + 110 = 680 W m−2 = Q + R, so R = 680 − 380 = 300 W m−2
✓ 1
Allow ECF from (b)(i).
Outgoing at the top: 160 + 40 + 300 = 500 W m−2, equal to the incoming 500 W m−2
✓ 1
Part (c)(i)
0.95σT⁴ = 520, so T⁴ = 520/(0.95 × 5.67 × 10−8) = 9.65 × 109 K⁴; T = 313 K
✓ 1
Accept 312–314 K. 309 K (emissivity ignored) scores 0.
Part (d)(i)
More greenhouse gas absorbs a larger fraction of the infrared emitted by the surface, so the 40 W m−2 escaping directly to space decreases
✓ 1
The atmosphere re-emits the absorbed energy in all directions, so the downward flow Q to the surface increases
✓ 1
The surface then gains more than it loses, so its temperature rises until it emits enough (the 520 W m−2 increases) for the outgoing radiation at the top of the atmosphere to balance the absorbed starlight again
✓ 1
"The greenhouse effect traps heat" alone scores [0].
Part (e)(i)
d = √(L/4πS) = √(2.7 × 1026/(4π × 2000)) = 1.04 × 1011 m
✓ 1
The gravitational force provides the centripetal force: GMm/d² = m(2π/T)²d, so T = 2π√(d³/GM)
✓ 1
Kepler's third law in the data-booklet form is equivalent.
T = 2π√((1.04 × 1011)³/(6.67 × 10−11 × 1.8 × 1030)) = 1.9 × 107 s = 221 days
✓ 1
Accept 215–225 days. Allow ECF from the distance.
Answers: (a)(ii) 0.32; 250 W m−2 · (b)(i) 380 W m−2 · (b)(ii) 300 W m−2 · (c)(i) 313 K · (e)(i) 221 days (the remaining parts are explanations — see the table above)
43IBP2H-012-01-11Albedo and latitudePaper 2Hard9 marks
An oceanographer models noon absorption of sunlight by the sea at an equinox. Assume that 70% of the top-of-atmosphere intensity of 1360 W m−2 reaches the surface as a direct beam at every latitude. The albedo of the ocean depends on the solar elevation angle (the angle of the Sun above the horizon): Solar elevation | Ocean albedo 90° | 0.03 30° | 0.06 10° | 0.35 Sea ice has an albedo of 0.60 at all elevations. At noon on an equinox, the solar elevation is (90° − latitude).
(a)
Outline why the solar intensity on a horizontal surface decreases as the latitude increases.
(2)
(b)
Calculate the solar power absorbed per square metre of ocean at noon at latitude 60°.
(2)
(c)
Using the data, explain why replacing sea ice with open ocean gives a smaller fractional increase in absorbed power at 10° elevation than at 30° elevation.
(3)
(d)
Determine the ratio of the power absorbed per square metre of ocean at the equator to that at latitude 80°.
(2)
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Notes
Part (a)
At higher latitude the rays arrive at a smaller elevation angle . A beam of given cross-section is spread over a larger horizontal area, so the power per unit area is lower; the intensity is proportional to sin(elevation) .
✓ 2
Part (b)
Intensity on horizontal surface = 1360 × 0.70 × sin 30° = 476 W m−2 . Absorbed = 476 × (1 − 0.06) = 447 W m−2 .
✓ 2
Part (c)
At 30°: absorbed fraction rises from 0.40 to 0.94, a factor of about 2.4 . At 10°: it rises from 0.40 to 0.65, a factor of about 1.6 . At low elevation the ocean reflects strongly, so its albedo is closer to that of ice and melting has less effect .
✓ 3
Part (d)
Equator: 952 × 1 × 0.97 = 923 W m−2; 80°: 952 × sin 10° × 0.65 = 107 W m−2 . Ratio = 923/107 ≈ 8.6 .
✓ 2
Exam tip: The angle of incidence enters twice: once through the geometric spreading of the beam, and once through the albedo. Apply both effects.
44IBP2H-012-01-13Surface–atmosphere energy balancePaper 2Hard9 marks
A planetary model has a surface that absorbs a mean solar intensity of 240 W m−2. The atmosphere is transparent to sunlight. The atmosphere is a single layer at temperature Ta that absorbs a fraction ε of the infrared emitted by the surface and has emissivity ε. The layer emits εσTa4 both upwards and downwards. The surface, at temperature Ts, is a black body.
Diagram not to scale
(a)
By considering the energy balance of the atmospheric layer, show that \(T_a = 2^{-1/4}T_s\).
(2)
(b)
By considering the energy balance at the top of the atmosphere, show that \(\sigma T_s^4 = \frac{240}{1-\varepsilon/2}\).
(2)
(c)
Calculate the value of ε needed for Ts = 288 K.
(2)
(d)
Increased greenhouse gas concentration raises ε to 0.80. Determine the resulting increase in surface temperature from 288 K.
(3)
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Notes
Part (a)
Power absorbed by the layer = εσTs4, and power emitted = 2εσTa4 . Equating gives Ta4 = Ts4/2, so Ta = 2−1/4Ts .
45IBP2H-012-01-16Albedo and melting sea icePaper 2Hard10 marks
Satellite data show that 4.0×1012 m2 of Arctic sea ice of albedo 0.55 has been replaced by open ocean of albedo 0.07. The Earth's surface area is 5.1×1014 m2, its mean albedo is 0.30 and the solar constant is 1360 W m−2. Averaged over a year, the Arctic receives 0.55 times the global mean solar intensity per unit area. Ignore the effect of clouds.
(a)
Calculate the equilibrium temperature of the Earth with no greenhouse effect.
(2)
(b)
Show that a small change Δα in mean albedo causes a change in equilibrium temperature given by \(\frac{\Delta T}{T} \approx -\frac{\Delta\alpha}{4(1-\alpha)}\).
(2)
(c)
Show that the loss of sea ice reduces the Earth's mean albedo by about 0.002.
(2)
(d)
Determine the resulting increase in the Earth's equilibrium temperature.
(2)
(e)
Suggest why the actual increase in surface temperature could be larger than the value calculated in the previous part.
(2)
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Notes
Part (a)
σT4 = 0.70 × 1360/4 = 238 W m−2 . T = (238/5.67×10−8)1/4 = 255 K .
✓ 2
Part (b)
σT4 = (1 − α)S/4, so T4 ∝ (1 − α) and 4 ln T = ln(1 − α) + constant. Alternatively, use 4ΔT/T = Δ(1 − α)/(1 − α) . This gives 4ΔT/T = −Δα/(1 − α), which rearranges to the result .
ΔT = 255 × 2.1×10−3/(4 × 0.70) . ΔT ≈ 0.19 K. Allow error carried forward from the equilibrium temperature and albedo change found earlier .
✓ 2
Part (e)
Warming increases evaporation, and water vapour is a greenhouse gas, so the greenhouse effect is enhanced . Further melting of ice lowers the albedo again, giving a positive feedback. Also allow reduced snow cover on land, or release of CH4 from thawing permafrost .
✓ 2
Exam tip: When you combine regional and global albedo changes, weight the local change by both the area fraction and the share of sunlight the region receives.
46IBP2H-012-00-10Heat shield of a solar probePaper 2Hard9 marks
A solar probe carries a flat heat shield whose front face points directly at the Sun. At closest approach the probe is 0.060 AU from the Sun. The solar constant at 1.0 AU is 1360 W m−2. The front face has albedo 0.60 and emissivity 0.80. Assume the shield is thermally insulated at the back, so it radiates only from its front face. σ = 5.67×10−8 W m−2 K−4.
(a)
Show that the intensity of solar radiation at 0.060 AU is about 3.8×105 W m−2.
(2)
(b)
Determine the equilibrium temperature of the front face.
(3)
(c)
Explain why the front face is given a high albedo and a high emissivity.
(2)
(d)
The shield material can safely reach 1700 K. Determine the closest distance, in AU, to which the probe could approach the Sun.
(2)
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Notes
Part (a)
Inverse-square law: I = 1360 × (1.0/0.060)2
✓ 1
I = 3.78×105 W m−2
✓ 1
Part (b)
Absorbed power per unit area = (1 − 0.60) × 3.78×105 = 1.51×105 W m−2
✓ 1
Equate to emitted power per unit area: 1.51×105 = 0.80 × 5.67×10−8 × T4
✓ 1
T ≈ 1350 K
✓ 1
Part (c)
A high albedo reflects most of the incident sunlight, so less power is absorbed
✓ 1
A high emissivity means the absorbed power is radiated away at a lower temperature, since T4 = (1 − α)I/(eσ)
✓ 1
Part (d)
T4 ∝ I ∝ 1/d2, so T ∝ d−1/2, giving d = 0.060 × (1350/1700)2
✓ 1
d ≈ 0.038 AU
✓ 1
ECF from (b)
—
Exam tip: Using the proportionality T ∝ d⁻¹/² in the last part saves recalculating the intensity and reduces arithmetic slips.
47IBP2H-012-00-12Surface–atmosphere energy balancePaper 2Hard9 marks
A simple climate model treats the atmosphere as a single layer. The layer is transparent to sunlight and absorbs a fraction f of the infrared radiation emitted by the ground. The layer radiates equal power per unit area upwards and downwards. The ground behaves as a black body and absorbs a mean solar intensity of 240 W m−2. σ = 5.67×10−8 W m−2 K−4.
Diagram not to scale
(a)
Show that, at equilibrium, \(\sigma T_s^4 = \frac{240}{1 - f/2}\), where Ts is the ground temperature.
(3)
(b)
Calculate Ts for f = 0.78. Give your answer to four significant figures.
(2)
(c)
Rising greenhouse gas concentrations increase f to 0.80. Determine the change in Ts.
(2)
(d)
Outline, with reference to the model, the enhanced greenhouse effect.
(2)
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Notes
Part (a)
Ground: 240 + A = σTs4, where A is the intensity radiated down by the atmosphere
✓ 1
Atmosphere: absorbed fσTs4 = emitted 2A (A up and A down)
✓ 1
Substitute A = fσTs4/2: σTs4(1 − f/2) = 240, which rearranges to the result
✓ 1
Part (b)
σTs4 = 240/0.61 = 393.4 W m−2
✓ 1
Ts = (393.4/5.67×10−8)1/4 = 288.6 K
✓ 1
Part (c)
σTs4 = 240/0.60 = 400 W m−2, giving Ts = 289.8 K
✓ 1
ΔTs = 289.8 − 288.6 ≈ +1.2 K
✓ 1
Alternative: ΔTs = 288.6 × [(0.61/0.60)1/4 − 1] ≈ 1.2 K, which earns both marks. Allow ECF from (b) if (b) is given to four significant figures.
—
Part (d)
More greenhouse gas absorbs a larger fraction of the infrared from the ground, and the atmosphere re-radiates part of it back down
✓ 1
The ground receives more power, so its temperature rises until the power it emits balances the larger input
✓ 1
Exam tip: When a difference of about 1 K is found from two temperatures near 290 K, keep at least four significant figures in the intermediate values, or use the ratio (0.61/0.60)¹/⁴ directly.
The Earth's equilibrium temperature of 255 K is given by \(T = \left(\frac{(1-\alpha)S}{4\sigma}\right)^{1/4}\), where S is the intensity of solar radiation arriving at the Earth (the solar constant, whose value varies slightly with solar activity) and α = 0.30 is the albedo.
(a)
Show that, for a small change ΔS, \(\frac{\Delta T}{T} \approx \frac{1}{4}\frac{\Delta S}{S}\).
(2)
(b)
Over a solar cycle, S varies by 0.10%. Estimate the resulting change in the equilibrium temperature.
(1)
(c)
A large volcanic eruption raises the albedo from 0.30 to 0.31. Determine the change in the equilibrium temperature.
(2)
(d)
Explain how a fall in temperature could lead to a further change in albedo, and state the effect of this on the temperature change.
(2)
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Notes
Part (a)
With α constant, T ∝ S1/4. Any one of these starting steps earns the mark: ln T = ¼ ln S + constant, OR T + ΔT ∝ (S + ΔS)1/4 = S1/4(1 + ΔS/S)1/4, OR dT/dS = ¼ T/S
✓ 1
Differentiating, or using (1 + x)1/4 ≈ 1 + x/4 for small x, gives ΔT/T ≈ ¼ ΔS/S
✓ 1
Part (b)
ΔT = ¼ × 0.0010 × 255 ≈ 0.064 K (accept 0.06 K)
✓ 1
Part (c)
(1 − α) falls from 0.70 to 0.69, a fractional change of −0.01/0.70 = −1.43%
✓ 1
ΔT = ¼ × (−0.0143) × 255 ≈ −0.91 K. Accept −0.9 K, or −0.92 K from exact calculation 255 × [(0.69/0.70)1/4 − 1]
✓ 1
Part (d)
Cooling allows snow and ice cover to grow, which raises the albedo further
✓ 1
Less solar power is absorbed, so the cooling is amplified (positive feedback)
✓ 1
Exam tip: Compare effects by fractional change. A 0.01 rise in albedo is a 1.4% change in (1 − α), about fourteen times the solar-cycle variation in S.
49IBP2H-012-00-16Equilibrium temperaturePaper 2Hard7 marks
A lunar rover must get rid of 300 W of heat produced by its electronics. It uses a flat radiator panel that emits from one face only. The panel's coating has emissivity 0.88 for infrared radiation. It reflects 80% of incident sunlight, so its albedo for sunlight is 0.80. In the design case the panel is in shadow at 290 K and absorbs no radiation. The solar intensity at the Moon is 1360 W m−2. σ = 5.67×10−8 W m−2 K−4.
(a)
Calculate the area of radiator needed.
(2)
(b)
The rover turns so that sunlight falls perpendicularly on the radiating face. The electronics still produce 300 W. Determine the new equilibrium temperature of the radiator.
(3)
(c)
With the rover back in shadow, the radiating face is tilted so that part of its view includes hot, sunlit lunar ground. Explain the effect of this on the equilibrium temperature of the radiator.
(2)
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Notes
Part (a)
300 = 0.88 × 5.67×10−8 × A × 2904
✓ 1
A ≈ 0.850 m2
✓ 1
Part (b)
Solar power absorbed = (1 − 0.80) × 1360 × 0.850 ≈ 231 W
✓ 1
Power emitted 300 + 231 = 531 W = 0.88 × 5.67×10−8 × 0.850 × T4
✓ 1
T ≈ 335 K (accept 334–335 K)
✓ 1
Allow ECF from (a).
—
Part (c)
The hot ground emits infrared radiation, and the radiator absorbs much of it because its high emissivity means it is also a good infrared absorber
✓ 1
This adds to the power input, so the equilibrium temperature rises above 290 K, or a larger area is needed to stay at 290 K
✓ 1
Common error: The internal 300 W does not stop when the Sun comes out. The radiator must emit the electronics' heat plus the absorbed sunlight.
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