Table 4
Hemisphere-averaged TOA radiative effect in the shortwave (dayside only) and longwave (dayside and nightside) for both water vapour (top rows) and cloud (bottom rows), including the net value (sum of three separate terms divided by two) for simulations T1:T1e, ProC:T1e, and Sun:T1e.
| Simulation | TOA radiative effect (W m−2) | |||
|---|---|---|---|---|
| Shortwave | Longwave | Net | ||
| Dayside | Dayside | Nightside | ||
| Water vapour | ||||
| T1:T1e | +28.7 | +9.47 (5.06%) | −21.4 (16.5%) | +8.37 |
| ProC:T1e | +29.1 | +8.65 (4.71%) | −21.5 (17.2%) | +8.14 |
| Sun:T1e | +5.39 | +0.412 (0.312%) | −15.2 (20.9%) | −4.71 |
| Cloud | ||||
| T1:T1e | −110 | +27.0 (14.4%) | −4.58 (3.53%) | −43.8 |
| ProC:T1e | −117 | +28.2 (15.3%) | −4.07 (3.25%) | −46.4 |
| Sun:T1e | −189 | +40.7 (30.8%) | −0.822 (1.13%) | −74.5 |
Notes. A positive radiative effect indicates a decrease in outgoing radiation. Parentheses on the longwave TOA radiative effect include the absolutepercentages of the averaged TOA outgoing longwave flux for that hemisphere. The effects of the two components are isolated using diagnostic calculations of the radiative transfer omitting their opacities (see text for explanation).
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