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SCIENCE · INVESTIGATE AND EXPLAIN

Audit surface, atmosphere and space fluxes

Use three boundaries to distinguish internal exchanges from external energy and net heat transfer.

Learning outcome: Check all radiative balances without double-counting absorbed surface radiation.

Starting recap

An arrow can be internal to the combined system while crossing a surface-only boundary. Net exchange subtracts opposing contributions.

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Try

At default settings, 79.3917 W/m² direct surface escape plus 158.7833 W/m² upward layer emission equals Q = 238.175 W/m².

Open the experiment

Predict

Can surface emission exceed absorbed sunlight while the combined system still conserves energy?

Experiment

Audit the default surface, layer and planetary ledgers, then repeat at emissivity 100% with unchanged albedo.

Trace a one-layer greenhouse energy balance

Worked teaching model · synthetic values · Global-mean radiative equilibrium, fixed sunlight 1361 W/m² and σ = 5.670374419 × 10⁻⁸ W m⁻² K⁻⁴. All unreflected sunlight reaches a blackbody surface. One uniform atmospheric layer is transparent to sunlight and has equal grey thermal absorptivity/emissivity ε. It emits upward and downward. No convection, spectral/vertical structure, heat capacity, time evolution, coupled feedback or CO₂-concentration mapping is included. Temperatures are solved model values, not measurements.

Reset keeps your prediction, captures and practice history.

One atmospheric layer · schematic paths, not a height or flux-width scaleReflected sunlight is already excluded from solar-to-ground input.Space · total thermal outgoing 238.175 W/m²Atmosphere: ε = 80%243.235 KBlackbody surface: 289.257 KSolar to ground238.175 W/m²Direct to space79.392 W/m²Absorbed by air317.567 W/m²Air to ground158.783 W/m²Air to space158.783 W/m²Surface emission = direct-to-space + absorbed-by-air = 396.958 W/m²Zero-flux arrows are omitted; their zero-valued labels remain.

The atmospheric layer emits in both directions. Gross surface emission can exceed absorbed sunlight because downward radiation also enters the surface budget. The net radiative transfer from surface to layer is 158.783 W/m² toward the layer; downward emission alone is not the net direction of heat exchange.

Separate equilibrium solutions at the same planetary albedoSolid: modeled surface · dashed: no-layer reference / effective emission150200250300350020406080100Atmospheric thermal emissivity (%) · temperature in K
Three radiative balances at the solved equilibrium (fluxes in W/m²)
BoundaryInputOutputInput − output (W/m²)
SurfaceSun 238.175 + air 158.783Gross emission 396.9580.000000
Atmospheric layerAbsorbed surface IR 317.567Up 158.783 + down 158.7830.000000
Whole systemUnreflected sunlight 238.175Direct surface 79.392 + air 158.7830.000000
Surface, layer and effective temperatures have different meanings
QuantityValue
Uniform modeled surface temperature289.257 K
Uniform atmospheric-layer temperature243.235 K
Effective emitting temperature of combined outgoing flux254.578 K
No-layer surface reference at the same albedo254.578 K
Surface difference from no-layer reference34.678 K

Let Q = (1 − α)S/4 be absorbed solar power per area, F = σTₛ⁴ be gross surface emission, and D be the layer's emission in each direction. Layer balance gives 2D = εF; surface balance gives F = Q + D. Therefore F = Q/(1 − ε/2). Direct surface escape is (1 − ε)F, so radiation reaching space is (1 − ε)F + D = Q.

For ε greater than zero, atmospheric balance gives Tₐ = Tₛ/2^(1/4). At ε = 0, dividing by ε is invalid: the layer neither absorbs nor emits, and its temperature is unconstrained by these radiative equations. It is not zero kelvin. The surface then equals the no-layer reference.

The graph compares equilibrium solutions; it is not a warming timeline. Neither parameter responds to temperature. Atmospheric emissivity is a grey teaching parameter, not CO₂ concentration, and the plotted sensitivity is not real-world equilibrium climate sensitivity. Convection, atmospheric solar absorption, wavelength-dependent absorption and emission, clouds, vertical structure and recorded observations require additional models and evidence.

Modeled surface 289.257 K; effective emission 254.578 K. Modeled atmospheric layer 243.235 K.

Absorbed sunlight 238.175 W/m²; total radiation to space 238.175 W/m². Surface gross emission 396.958 W/m² includes energy returned from the layer. All three budgets balance; the comparison does not simulate adjustment through time or predict real climate sensitivity.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

A large internal flux does not create energy

At the default settings, the surface emits about 396.9583 W/m² even though absorbed sunlight is only 238.175 W/m². Before deciding that energy has been created, inspect the boundary around the surface. It receives sunlight and downward thermal emission from the atmospheric layer. A budget that omits one input cannot explain that surface’s output.

Draw three separate boundaries on paper: surface only, atmospheric layer only, and the combined system. Arrows crossing one boundary may be internal to another. The UBC single-layer model illustrates the importance of distinguishing direct surface radiation from atmospheric radiation reaching space. Use its conceptual separation without treating this lab as a measured flux record.

The lab assumes all absorbed solar flux reaches the surface, a transparent atmosphere for sunlight, a blackbody surface, and a single grey thermal layer. These assumptions make three ledgers solvable. They do not describe every route by which energy moves through real air and water.

Audit the surface boundary

Write Q for absorbed sunlight, F for surface emission and D for downward layer emission. At the default, Q = 238.175, D = 158.7833 and F = 396.9583 W/m². The surface residual is Q + D − F, which is zero apart from rounding.

A residual is incoming minus outgoing flux for the chosen boundary. A positive residual would mean energy accumulation there; a negative residual would mean energy loss. Here equilibrium is solved directly, so a near-zero numerical residual confirms the accounting rather than demonstrating an observed adjustment process.

Change atmospheric emissivity while keeping albedo at 30%. Record both F and D. Their difference remains Q. A growing gross exchange can therefore coexist with an unchanged external supply. Explain that relationship using your ledger, not the phrase “extra energy” without a named source.

Audit the layer and space boundaries

The layer absorbs εF and emits D upward plus D downward. At ε = 0.80, absorption is 317.5667 W/m² and total layer emission is twice 158.7833 W/m². The layer residual εF − 2D is zero.

Only the transmitted surface contribution, (1 − ε)F, reaches space directly. At the default this is 79.3917 W/m². Add upward layer emission of 158.7833 W/m² to get total outgoing 238.175 W/m². The planetary residual is Q − [(1 − ε)F + D], again zero.

When you combine the surface and layer boundaries, their internal exchanges cancel. This cancellation is why you must not add downward radiation to the planetary external input. It crosses an internal boundary, not the boundary between the planet and space.

Distinguish opposing radiation from net exchange

The layer is cooler than the surface in this equilibrium model, yet it emits downward radiation that the surface absorbs. Both bodies emit radiation; the direction of one arrow does not determine the direction of net energy exchange.

The surface-to-layer exchange is εF upward absorbed by the layer, minus D downward absorbed by the surface. Because D = εF/2, the net is εF/2, nonnegative. At the default it is 158.7833 W/m² from the warmer surface toward the cooler layer. The downward arrow does not imply net heat transfer from cold to hot.

For an independent paper check, choose ε = 1 at the same albedo. There is no direct surface transmission. F = 476.35 W/m², and the layer emits 238.175 W/m² each way. Confirm all three balances and describe why the surface flux can be twice Q while total outgoing remains Q.

Transfer by repairing a ledger

A learner calculates planetary outgoing as F + D using the default values. Identify the double-counting and write the correct expression. Then calculate net surface-to-layer exchange.

Check the radiative-flows transfer

F includes radiation absorbed by the layer, so it cannot all be counted as direct escape. Planetary outgoing is (1 − ε)F + D = 238.175 W/m². Net surface-to-layer exchange is εF − D = 158.7833 W/m², upward from the warmer surface.

Apply

Which expression correctly gives outgoing thermal radiation to space?

Public practice checks a specific claim. It does not establish independent mastery.

Distinguish gross downward radiation from net surface-to-layer exchange and explain why internal fluxes cancel in the combined budget.

Continue

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