The role of Rossby waves, which are invariant sets with respect to time evolution, in the formation of large-scale structures.
JAXA Supercomputer System Annual Report February 2024-January 2025
Report Number: R24EACA46
Subject Category: JSS Inter-University Research
- Responsible Representative: Kiori Obuse, Associate Professor, Okayama University
- Contact Information: Kiori Obuse(obuse@okayama-u.ac.jp)
- Members: Kiori Obuse
Abstract
One of the simplest mathematical models describing the dynamics of planetary atmospheres, the 2D barotropic flow on a rotating sphere, shows the spontaneous formation of large-scale zonal flows such as those seen in giant gas planets. However, this mechanism has not been fully clarified. This study aims to clarify what kind of Rossby wave interaction strongly contributes to the formation of large-scale structures.
Reference URL
N/A
Reasons and benefits of using JAXA Supercomputer System
Since the research group with which we might collaborate had an account on the JAXA supercomputing system, we considered it desirable to use this system for sharing data in case of collaboration. Also, as the research was a continuation of the previous year's research and most of the data required was located on the JAXA supercomputing system, we wished to continue using the system.
Achievements of the Year
For large-scale zonal flow formation in unforced 2D turbulence on a rotating sphere, it has been suggested that the Rossby wave three-wave interaction Y_(n1)^(m) x Y_(n2)^(-m) -> Y_(n3)^0 (where Y_n^m is the spherical harmonic function), where
(1) m_1 = -m_2 is small
(2) |n_1- n_2| is very small
(3) n_1, n_2 are very large
have been suggested to be important (Hagimori et al , 2024). However, it is not yet known how and to what degree these conditions operate in the structure formation. In this study, therefore, calculations were carried out to confirm whether or not the large-scale zonal flow formation depends on the initial conditions and to clarify which of the above conditions (1)-(3) works most strongly.
The results showed that, firstly, if the zonal flow formation is continuously inhibited up to a certain stage, the zonal flow does not become predominant when the normal time development condition is subsequently restored. Furthermore, even if a large perturbation was applied to the state where the zonal flows ceased to dominate, the zonal flows did not resume their developments and dominate the flow filed. This result indicates that the faomation of large-scale zonal flows depend on initional conditions. In order to consider the importanc of conditions (1)-(3) above, the time evolution for various initial flow filed with various energy distributions (with particular attention to the distribution of m) was subsequently investigated. The results suggest that (1) is of relatively low importance. The importance of (3) is also considered to be low because of the reverse cascade that occurs when zonal flows dominate. Therefore, it was found that condition (2) "|n_1 - n_2| being very small" may be of relatively high importance among the three conditions.
Publications
- Oral Presentations
1) Kiori Obuse, Hagimori Yusuke, and Michio Yamada, "Rossby wave nonlinear interactions and large-scale zonal flow formation in two-dimensional turbulence on a rotating sphere", EGU General Assembly 2024, Austria Center Vienna, 14th-19th Apr. 2024
2) Kiori Obuse and Michio Yamada, "Large-scale zonal structure formation by Rossby wave nonlinear interaction on a rotating sphere.", Annual Meeting of JSFM, Forest Sendai, 25-27 Sep. 2024
Usage of JSS
Computational Information
- Process Parallelization Methods: N/A
- Thread Parallelization Methods: N/A
- Number of Processes: 1
- Elapsed Time per Case: 24 Hour(s)
JSS3 Resources Used
Fraction of Usage in Total Resources*1(%): 0.00
Details
Please refer to System Configuration of JSS3 for the system configuration and major specifications of JSS3.
System Name | CPU Resources Used(Core x Hours) | Fraction of Usage*2(%) |
---|---|---|
TOKI-SORA | 8.76 | 0.00 |
TOKI-ST | 0.07 | 0.00 |
TOKI-GP | 0.00 | 0.00 |
TOKI-XM | 0.00 | 0.00 |
TOKI-LM | 0.00 | 0.00 |
TOKI-TST | 0.00 | 0.00 |
TOKI-TGP | 0.00 | 0.00 |
TOKI-TLM | 0.00 | 0.00 |
File System Name | Storage Assigned(GiB) | Fraction of Usage*2(%) |
---|---|---|
/home | 140.00 | 0.09 |
/data and /data2 | 10240.00 | 0.05 |
/ssd | 0.00 | 0.00 |
Archiver Name | Storage Used(TiB) | Fraction of Usage*2(%) |
---|---|---|
J-SPACE | 0.00 | 0.00 |
*1: Fraction of Usage in Total Resources: Weighted average of three resource types (Computing, File System, and Archiver).
*2: Fraction of Usage:Percentage of usage relative to each resource used in one year.
ISV Software Licenses Used
ISV Software Licenses Used(Hours) | Fraction of Usage*2(%) | |
---|---|---|
ISV Software Licenses(Total) | 0.00 | 0.00 |
*2: Fraction of Usage:Percentage of usage relative to each resource used in one year.
JAXA Supercomputer System Annual Report February 2024-January 2025