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Inference of Solar Irradiance Variability from Terrestrial Temperature Changes, 1880-1993: An Astrophysical Application of the Sun-Climate Connection

机译:从地面温度变化推论太阳辐照度的变化,1880-1993年:太阳-气候连接的天体应用

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Information can be inferred on the timing and amplitude of solar total irradiance changes over 1880- 1993 by simulating the global terrestrial surface temperature changes produced by these irradiance changes and comparing them with observed temperatures. The profiles of solar irradiance variations used in the climate simulations are adopted from several different proxies: (1) the length of the sunspot cycle, (2) the mean sunspot number, and (3) a composite proxy that includes the two previous indicators plus the equatorial solar rotation rate, the fraction of penumbral spot coverage, and the rate of decay of the sunspot cycle. We use a seasonal energy-conservation climate/upwelling-diffusion ocean model, forced by the assumed profiles of solar total irradiance variations, combined with variations in anthropogenic greenhouse gases. Optimized cases imply total irradiance changes during 1880-1993 in the range 0.18%-0.77%.If the solar irradiance profiles found from the climate simulations are required to be consistent with recent satellite observations, then the composite solar profile reconstructed by Hoyt & Schatten, combined with the anthropogenic greenhouse forcing, explains the highest fraction of the variance of observed global mean temperatures. In this case, the solar and greenhouse combination accounts for 92% of the observed long-term temperature variance during 1880-1993. The simulation implies that the solar part of the forcing alone would account for 71% of the global mean temperature variance, compared to 51% for the greenhouse gases' part alone. It also suggests a solar total irradiance variation of 0.5% during the interval 1880-1993. Such an amplitude of solar total irradiance change is consistent with astrophysical limits of brightness changes on timescales of decades to centuries independently derived from observations of solar-type stars (including the Sun).
机译:通过模拟由这些辐照度变化产生的全球陆地表面温度变化并将其与观测温度进行比较,可以推断出1880-1993年期间太阳总辐照度变化的时间和幅度。气候模拟中使用的太阳辐照度变化曲线来自以下几种不同的代理:(1)太阳黑子周期的长度;(2)太阳黑子的平均数;(3)包括两个先前指标加上赤道太阳旋转速度,半影斑覆盖率和黑子周期的衰减率。在假定的太阳总辐照度变化以及人为温室气体变化的共同作用下,我们使用了季节性节能气候/上升扩散海洋模型。最优化的情况意味着1880-1993年期间的总辐照度变化在0.18%-0.77%范围内。如果要求从气候模拟中找到的太阳辐照度剖面与最近的卫星观测结果一致,则由Hoyt&Schatten重建的复合太阳剖面结合人为温室强迫,解释了观测到的全球平均温度方差的最大部分。在这种情况下,太阳能和温室的结合占了1880-1993年间观测到的长期温度变化的92%。该模拟表明,强迫的仅太阳部分将占全球平均温度变化的71%,而温室气体仅这一部分为51%。这也表明在1880-1993年间太阳总辐照度变化为0.5%。太阳总辐照度变化的这种幅度与几十到几百年时间尺度上亮度变化的天体极限一致,这是独立于对太阳型恒星(包括太阳)的观测得出的。

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