Articles | Volume 15, issue 19
https://doi.org/10.5194/gmd-15-7471-2022
https://doi.org/10.5194/gmd-15-7471-2022
Model evaluation paper
 | 
10 Oct 2022
Model evaluation paper |  | 10 Oct 2022

Tropospheric transport and unresolved convection: numerical experiments with CLaMS 2.0/MESSy

Paul Konopka, Mengchu Tao, Marc von Hobe, Lars Hoffmann, Corinna Kloss, Fabrizio Ravegnani, C. Michael Volk, Valentin Lauther, Andreas Zahn, Peter Hoor, and Felix Ploeger

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Interactive discussion

Status: closed

Comment types: AC – author | RC – referee | CC – community | EC – editor | CEC – chief editor | : Report abuse
  • RC1: 'Comment on gmd-2022-97', Anonymous Referee #1, 16 Jun 2022
    • AC1: 'Reply on RC1', Paul Konopka, 26 Aug 2022
  • RC2: 'Comment on gmd-2022-97', Anonymous Referee #2, 19 Jun 2022
    • AC2: 'Reply on RC2', Paul Konopka, 26 Aug 2022

Peer review completion

AR: Author's response | RR: Referee report | ED: Editor decision | EF: Editorial file upload
AR by Paul Konopka on behalf of the Authors (26 Aug 2022)  Author's response   Author's tracked changes   Manuscript 
ED: Referee Nomination & Report Request started (29 Aug 2022) by Olaf Morgenstern
RR by Anonymous Referee #2 (04 Sep 2022)
ED: Publish as is (20 Sep 2022) by Olaf Morgenstern
AR by Paul Konopka on behalf of the Authors (20 Sep 2022)  Manuscript 
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Short summary
Pure trajectory-based transport models driven by meteorology derived from reanalysis products (ERA5) take into account only the resolved, advective part of transport. That means neither mixing processes nor unresolved subgrid-scale advective processes like convection are included. The Chemical Lagrangian Model of the Stratosphere (CLaMS) includes these processes. We show that isentropic mixing dominates unresolved transport. The second most important transport process is unresolved convection.