dc.contributor.advisor | Chakraborty, Arindam | |
dc.contributor.advisor | Nanjundiah, Ravi S | |
dc.contributor.author | Jain, Deepeshkumar | |
dc.date.accessioned | 2021-02-03T06:35:03Z | |
dc.date.available | 2021-02-03T06:35:03Z | |
dc.date.submitted | 2018 | |
dc.identifier.uri | https://etd.iisc.ac.in/handle/2005/4848 | |
dc.description.abstract | Clouds exist on all scales from turbulent processes to global scale and are organized
on all the scales in between. They truly are multi-scale in nature. This makes them a
very challenging simulation problem for atmospheric models. No model can resolve all
of the scales relevant for cloud formation. Any attempt to develop a theory to resolve
or represent all these processes require a deeper understanding of cloud scale processes
at all the scales. It also requires the understanding of the state of the art in modeling
these processes. The present research focuses on the moist convective representation
in a hierarchy of models from General Circulation Model (GCM) to Large Eddy
Simulations (LES). In finding out the missing gap between the different convective
representations, we improve the simulation skill of GCM over India during monsoon,
we propose a mechanism for the southward propagating meso-scale convective systems
over Bay of Bengal (BoB) using Cloud Resolving Model (CRM), and explore the role
of sea surface temperature (SST) in modifying the boundary layer stability using
LES. The three types of studies are described below.
In the rst part of the study we carry out a 28 year long simulation using a GCM.
We focus on the intra-seasonal and inter-annual variability of Indian monsoon and
its teleconnection with El Nino Southern Oscillation and Indian ocean dipole in the
model. To perform a sensitivity study, we change the cloud adjustment time scale
(CATS) in the Relaxed Arakawa-Schubert (RAS) cumulus parameterization. RAS
is designed to perform well in a typical GCM resolution. CATS ( adj) implicitly
determines the rate of change of convective available potential energy (CAPE) in the
model by the clouds. We nd that changing the adj not only improves the mean monsoon predictability, it also in
uences the teleconnections of Indian monsoon with
El-nino Southern Oscillations and Indian Ocean dipole. It is realized in this part of the
study that a better understanding of relationship between CAPE and precipitation
is crucial to improving simulation skill of the model.
To analyze the relationship between CAPE and deep convection, we carry out a
season long CRM simulation over India. We nd that mesoscale convective systems
(MCS) constitute a major portion of the overall precipitation over India. As MCS
consume CAPE in a characteristically di erent way from what is proposed in a typical
cumulus parameterization used in a GCM, a GCM is unable to correctly simulate
most of the Indian monsoon precipitation. Present day cumulus parameterization
lack representation of MCS.
In our CRM simulation, one of the most signi cant MCS we found was the southward
propagating MCS over the BoB. These MCSs move south within northward moving
synoptic scale cloud clusters over the BoB. These systems have gravity currentlike
structure and propagate orthogonal to lower tropospheric winds. High-resolution
and cloud microphysics schemes are necessary to simulate these events using numerical
models. A model with cumulus parameterization is unable to simulate the
updraft-downdraft pair and the gravity current structure of this southward propagating
mesoscale system. We nd that high model resolution is needed to resolve
the updraft-downdraft pair and cumulus parameterization assumptions break down
at such high resolutions.
The southward propagating MCSs over the BoB sometimes originate over land
(due to diurnal land heating) and sometimes over ocean. To understand the process
of convective initiation over the ocean, it is necessary to understand the relationship
of lower atmospheric stability as a function of SST. In the last part of the thesis, we
use LES to simulate the boundary layer structure in response to changing sea surface
temperature. A threshold value of SST (28 C) is found in the tropics above which
there is a high probability of getting convection. LES simulations show that above
this SST, the mixed layer depth is higher than the lifting condensation level. | en_US |
dc.language.iso | en_US | en_US |
dc.relation.ispartofseries | ;G29712 | |
dc.rights | I grant Indian Institute of Science the right to archive and to make available my thesis or dissertation in whole or in part in all forms of media, now hereafter known. I retain all proprietary rights, such as patent rights. I also retain the right to use in future works (such as articles or books) all or part
of this thesis or dissertation | en_US |
dc.subject | atmospheric models | en_US |
dc.subject | General Circulation Model | en_US |
dc.subject | Large Eddy Simulations | en_US |
dc.subject | Cloud Resolving Model | en_US |
dc.subject.classification | Research Subject Categories::NATURAL SCIENCES::Earth sciences::Atmosphere and hydrosphere sciences | en_US |
dc.title | Multi-Scale Modeling of Moist Convection Over India | en_US |
dc.type | Thesis | en_US |
dc.degree.name | PhD | en_US |
dc.degree.level | Doctoral | en_US |
dc.degree.grantor | Indian Institute of Science | en_US |
dc.degree.discipline | Engineering | en_US |