<p>Understanding elevation-dependent warming is essential for assessing risks to the cryosphere and water resources in mountainous regions. However, warming patterns above 5 km a.s.l. on the Tibetan Plateau are poorly understood due to data scarcity. Here, we integrate station observations with 12 ice core δ<sup>18</sup>O records to reconstruct annual and summer temperature records for the westerlies-dominated Tibetan Plateau since the 1950s, and systematically evaluate the three-dimensional structure and seasonal differences of elevation-dependent warming. Our results reveal a clear pattern of elevation-dependent warming in annual mean temperature between 2 and 7.5 km, primarily driven by snow albedo and cloud feedbacks. In contrast, summer temperatures show no elevation-dependent warming due to the competing effects of multiple feedback processes. Furthermore, we identified a warming peak between 2.5 and 3 km driven by radiative forcing and sensible heat, and muted warming between 6 and 6.5 km due to cloud-radiation-glacier feedbacks.</p>

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Elevation-dependent warming at high altitudes in the westerlies-dominated Tibetan Plateau

  • Xiaoqian Liu,
  • Renhui Huang,
  • Wangbin Zhang,
  • Shuangye Wu,
  • Hongxi Pang,
  • Shugui Hou

摘要

Understanding elevation-dependent warming is essential for assessing risks to the cryosphere and water resources in mountainous regions. However, warming patterns above 5 km a.s.l. on the Tibetan Plateau are poorly understood due to data scarcity. Here, we integrate station observations with 12 ice core δ18O records to reconstruct annual and summer temperature records for the westerlies-dominated Tibetan Plateau since the 1950s, and systematically evaluate the three-dimensional structure and seasonal differences of elevation-dependent warming. Our results reveal a clear pattern of elevation-dependent warming in annual mean temperature between 2 and 7.5 km, primarily driven by snow albedo and cloud feedbacks. In contrast, summer temperatures show no elevation-dependent warming due to the competing effects of multiple feedback processes. Furthermore, we identified a warming peak between 2.5 and 3 km driven by radiative forcing and sensible heat, and muted warming between 6 and 6.5 km due to cloud-radiation-glacier feedbacks.